
<bib>
<comment>
This file was created by the TYPO3 extension publications
--- Timezone: CEST
Creation date: 2026-04-15
Creation time: 07:35:48
--- Number of references
436
</comment>
<reference>
<bibtype>article</bibtype>
<title>Decoupling of external and internal dynamics in driven two-level systems</title>
<year>2024</year>
<month>11</month>
<DOI>10.1103/PhysRevResearch.6.043153</DOI>
<journal>Phys. Rev. Res.</journal>
<volume>6</volume>
<authors>
<person>
<fn>S.</fn>
<sn>Böhringer</sn>
</person>
<person>
<fn>A.</fn>
<sn>Friedrich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Janson2024</citeid>
<title>Finite pulse-time effects in long-baseline quantum clock interferometry</title>
<abstract>Quantum-clock interferometry has been suggested as a quantum probe to test the universality of free fall and the universality of gravitational redshift. In typical experimental schemes, it seems advantageous to employ Doppler-free E1–M1 transitions which have so far been investigated in quantum gases at rest. Here, we consider the fully quantized atomic degrees of freedom and study the interplay of the quantum center-of-mass (COM)—that can become delocalized—together with the internal clock transitions. In particular, we derive a model for finite-time E1–M1 transitions with atomic intern–extern coupling and arbitrary position-dependent laser intensities. We further provide generalizations to the ideal expressions for perturbed recoilless clock pulses. Finally, we show, at the example of a Gaussian laser beam, that the proposed quantum-clock interferometers are stable against perturbations from varying optical fields for a sufficiently small quantum delocalization of the atomic COM.</abstract>
<year>2024</year>
<month>5</month>
<DOI>10.1116/5.0178230</DOI>
<journal>AVS Quantum Science</journal>
<volume>6</volume>
<authors>
<person>
<fn>G.</fn>
<sn>Janson</sn>
</person>
<person>
<fn>A.</fn>
<sn>Friedrich</sn>
</person>
<person>
<fn>R.</fn>
<sn>Lopp</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>10.1116/5.0185291</citeid>
<title>Terrestrial very-long-baseline atom interferometry: Workshop summary</title>
<abstract>This document presents a summary of the 2023 Terrestrial Very-Long-Baseline Atom Interferometry Workshop hosted by CERN. The workshop brought together experts from around the world to discuss the exciting developments in large-scale atom interferometer (AI) prototypes and their potential for detecting ultralight dark matter and gravitational waves. The primary objective of the workshop was to lay the groundwork for an international TVLBAI proto-collaboration. This collaboration aims to unite researchers from different institutions to strategize and secure funding for terrestrial large-scale AI projects. The ultimate goal is to create a roadmap detailing the design and technology choices for one or more kilometer—scale detectors, which will be operational in the mid-2030s. The key sections of this report present the physics case and technical challenges, together with a comprehensive overview of the discussions at the workshop together with the main conclusions.</abstract>
<year>2024</year>
<month>5</month>
<DOI>10.1116/5.0185291</DOI>
<journal>AVS Quantum Science</journal>
<volume>6</volume>
<authors>
<person>
<fn>S.</fn>
<sn>Abend</sn>
</person>
<person>
<fn>et al.</fn>
<sn></sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Asano2024</citeid>
<title>Quantum Field Theory for Multipolar Composite Bosons with Mass Defect and Relativistic Corrections</title>
<year>2024</year>
<month>4</month>
<DOI>10.1103/PRXQuantum.5.020322</DOI>
<journal>PRX Quantum</journal>
<volume>5</volume>
<authors>
<person>
<fn>T.</fn>
<sn>Asano</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
<person>
<fn>F.</fn>
<sn>Di Pumpo</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevResearch.6.013285</citeid>
<title>Dimensional reduction in quantum optics</title>
<year>2024</year>
<month>3</month>
<DOI>10.1103/PhysRevResearch.6.013285</DOI>
<journal>Phys. Rev. Res.</journal>
<volume>6</volume>
<authors>
<person>
<fn>J.</fn>
<sn>Ströhle</sn>
</person>
<person>
<fn>R.</fn>
<sn>Lopp</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevResearch.6.013186</citeid>
<title>Average correlation as an indicator for inseparability</title>
<year>2024</year>
<month>2</month>
<DOI>10.1103/PhysRevResearch.6.013186</DOI>
<journal>Phys. Rev. Res.</journal>
<volume>6</volume>
<authors>
<person>
<fn>M. E. N.</fn>
<sn>Tschaffon</sn>
</person>
<person>
<fn>J.</fn>
<sn>Seiler</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>di_pumpo_optimal_2024</citeid>
<title>Optimal baseline exploitation in vertical dark-matter detectors based on atom interferometry</title>
<abstract>Several terrestrial detectors for gravitational waves and dark matter based on long-baseline atom interferometry are currently in the final planning stages or already under construction. These upcoming vertical sensors are inherently subject to gravity and thus feature gradiometer or multi-gradiometer configurations using single-photon transitions for large momentum transfer. While there has been significant progress on optimizing these experiments against detrimental noise sources and for deployment at their projected sites, finding optimal configurations that make the best use of the available resources is still an open issue. Even more, the fundamental limit of the device's sensitivity is still missing. Here, we fill this gap and show that (a) resonant-mode detectors based on multi-diamond fountain gradiometers achieve the optimal, shot-noise limited, sensitivity if their height constitutes 20% of the available baseline; (b) this limit is independent of the dark matter oscillation frequency; and (c) doubling the baseline decreases the ultimate measurement uncertainty by approximately 65%. Moreover, we propose a multi-diamond scheme with less mirror pulses where the leading-order gravitational phase contribution is suppressed and compare it to established geometries and demonstrate that both configurations saturate the same fundamental limit.</abstract>
<year>2024</year>
<month>1</month>
<reviewed>1</reviewed>
<DOI>10.1116/5.0175683</DOI>
<journal>AVS Quantum Science</journal>
<volume>6</volume>
<authors>
<person>
<fn>F.</fn>
<sn>Di Pumpo</sn>
</person>
<person>
<fn>A.</fn>
<sn>Friedrich</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>bott_atomic_2023</citeid>
<title>Atomic diffraction from single-photon transitions in gravity and Standard-Model extensions</title>
<abstract>Single-photon transitions are one of the key technologies for designing and operating very-long-baseline atom interferometers tailored for terrestrial gravitational-wave and dark-matter detection. Since such setups aim at the detection of relativistic and beyond-Standard-Model physics, the analysis of interferometric phases as well as of atomic diffraction must be performed to this precision and including these effects. In contrast, most treatments focused on idealized diffraction so far. Here, we study single-photon transitions, both magnetically induced and direct ones, in gravity and Standard-Model extensions modeling dark matter as well as Einstein-equivalence-principle violations. We take into account relativistic effects like the coupling of internal to center-of-mass degrees of freedom, induced by the mass defect, as well as the gravitational redshift of the diffracting light pulse. To this end, we also include chirping of the light pulse required by terrestrial setups, as well as its associated modified momentum transfer for single-photon transitions.</abstract>
<year>2023</year>
<month>11</month>
<DOI>10.1116/5.0174258</DOI>
<journal>AVS Quantum Science</journal>
<volume>5</volume>
<authors>
<person>
<fn>A.</fn>
<sn>Bott</sn>
</person>
<person>
<fn>F.</fn>
<sn>Di Pumpo</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<citeid>Tschaffon2023</citeid>
<title>A Primer on the Riemann Hypothesis</title>
<abstract>We provide an introduction for physicists into the Riemann Hypothesis. For this purpose, we first introduce, and then compare and contrast the Riemann function and the Dirichlet L-functions, with the Titchmarsh counterexample. Whereas the first two classes of functions are expected to satisfy the Riemann Hypothesis, the Titchmarsh counterexample is known to violate it. Throughout our article we employ elementary mathematical techniques known to every physicist. Needless to say, we do not verify the Riemann Hypothesis but suggest heuristic arguments in favor of it. We also build a bridge to quantum mechanics by interpreting the Dirichlet series central to this field as a superposition of probability amplitudes leading us to an unusual potential with a logarithmic energy spectrum opening the possibility of factoring numbers.</abstract>
<year>2023</year>
<month>9</month>
<DOI>10.1007/978-3-031-32469-7_7</DOI>
<journal>Sketches of Physics: The Celebration Collection</journal>
<authors>
<person>
<fn>M. E. N.</fn>
<sn>Tschaffon</sn>
</person>
<person>
<fn>I.</fn>
<sn>Tkáčová</sn>
</person>
<person>
<fn>H.</fn>
<sn>Maier</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Factorization with a logarithmic energy spectrum of a central potential</title>
<year>2023</year>
<month>6</month>
<DOI>10.12693/APhysPolA.143.S112</DOI>
<journal>Acta Physica Polonica A</journal>
<volume>143</volume>
<authors>
<person>
<fn>F.</fn>
<sn>Gleisberg</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Friedrich_2023</citeid>
<title>The Wave Functional of the Vacuum in a Resonator</title>
<year>2023</year>
<month>6</month>
<DOI>10.12693/APhysPolA.143.S52</DOI>
<journal>Acta Physica Polonica A</journal>
<volume>143</volume>
<authors>
<person>
<fn>A.</fn>
<sn>Friedrich</sn>
</person>
<person>
<fn>D.</fn>
<sn>Moll</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>L.</fn>
<sn>Plimak</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>tschaffon_average_2023</citeid>
<title>Average correlation as an indicator for nonclassicality</title>
<year>2023</year>
<month>4</month>
<day>27</day>
<DOI>10.1103/PhysRevResearch.5.023063</DOI>
<journal>Phys. Rev. Res.</journal>
<volume>5</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>M. E. N.</fn>
<sn>Tschaffon</sn>
</person>
<person>
<fn>J.</fn>
<sn>Seiler</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Boegel_2023</citeid>
<title>Controlled expansion of shell-shaped Bose–Einstein condensates</title>
<abstract>Motivated by the recent experimental realization of ultracold quantum gases in shell topology, we propose a straightforward implementation of matter-wave lensing techniques for shell-shaped Bose–Einstein condensates. This approach allows to significantly extend the free evolution time of the condensate shell after release from the trap and enables the study of novel quantum many-body effects on curved geometries. With both analytical and numerical methods we derive optimal parameters for realistic schemes to conserve the shell shape of the condensate for times up to hundreds of milliseconds.</abstract>
<year>2023</year>
<month>4</month>
<day>27</day>
<DOI>10.1088/2058-9565/acc969</DOI>
<journal>Quantum Science and Technology</journal>
<volume>8</volume>
<authors>
<person>
<fn>P.</fn>
<sn>Boegel</sn>
</person>
<person>
<fn>A.</fn>
<sn>Wolf</sn>
</person>
<person>
<fn>M.</fn>
<sn>Meister</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Glasbrenner_2023</citeid>
<title>The Landau–Zener formula made simple</title>
<abstract>We employ the Markov approximation and the well-known Fresnel-integral to derive in ‘one-line’ the familiar expression for the Landau–Zener transition probability. Moreover, we provide numerical as well as analytical justifications for our approach, and identify three characteristic motions of the probability amplitude in the complex plane.</abstract>
<year>2023</year>
<month>4</month>
<day>13</day>
<DOI>10.1088/1361-6455/acc774</DOI>
<journal>Journal of Physics B: Atomic, Molecular and Optical Physics</journal>
<volume>56</volume>
<authors>
<person>
<fn>E. P.</fn>
<sn>Glasbrenner</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>di_pumpo_universality—clock-rates_2023</citeid>
<title>Universality-of-clock-rates test using atom interferometry with T³ scaling</title>
<year>2023</year>
<month>3</month>
<DOI>10.1103/PhysRevD.107.064007</DOI>
<journal>Phys. Rev. D</journal>
<volume>107</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>F.</fn>
<sn>Di Pumpo</sn>
</person>
<person>
<fn>A.</fn>
<sn>Friedrich</sn>
</person>
<person>
<fn>C.</fn>
<sn>Ufrecht</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.106.032211</citeid>
<title>Geometric link between the Hardy nonlocality condition and the Clauser-Horne-Shimony-Holt inequality</title>
<year>2022</year>
<month>9</month>
<DOI>10.1103/PhysRevA.106.032211</DOI>
<journal>Phys. Rev. A</journal>
<volume>106</volume>
<authors>
<person>
<fn>J.</fn>
<sn>Seiler</sn>
</person>
<person>
<fn>T.</fn>
<sn>Strohm</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>schach_tunneling_2022</citeid>
<title>Tunneling gravimetry</title>
<abstract>We examine the prospects of utilizing matter-wave Fabry–Pérot interferometers for enhanced inertial sensing applications. Our study explores such tunneling-based sensors for the measurement of accelerations in two configurations: (a) a transmission setup, where the initial wave packet is transmitted through the cavity and (b) an out-tunneling scheme with intra-cavity generated initial states lacking a classical counterpart. We perform numerical simulations of the complete dynamics of the quantum wave packet, investigate the tunneling through a matter-wave cavity formed by realistic optical potentials and determine the impact of interactions between atoms. As a consequence we estimate the prospective sensitivities to inertial forces for both proposed configurations and show their feasibility for serving as inertial sensors.</abstract>
<year>2022</year>
<month>8</month>
<DOI>10.1140/epjqt/s40507-022-00140-3</DOI>
<journal>EPJ Quantum Technology</journal>
<volume>9</volume>
<authors>
<person>
<fn>P.</fn>
<sn>Schach</sn>
</person>
<person>
<fn>A.</fn>
<sn>Friedrich</sn>
</person>
<person>
<fn>J. R.</fn>
<sn>Williams</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>schleich_2021</citeid>
<title>Der Pfeil der Zeit: Festvortrag</title>
<year>2022</year>
<month>7</month>
<DOI>https://doi.org/10.11588/diglit.61622.11</DOI>
<journal>Heidelberger Akademie der Wissenschaften: Jahrbuch 2021</journal>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.106.013309</citeid>
<title>Shell-shaped Bose-Einstein condensates based on dual-species mixtures</title>
<year>2022</year>
<month>7</month>
<DOI>10.1103/PhysRevA.106.013309</DOI>
<journal>Phys. Rev. A</journal>
<volume>106</volume>
<authors>
<person>
<fn>A.</fn>
<sn>Wolf</sn>
</person>
<person>
<fn>P.</fn>
<sn>Boegel</sn>
</person>
<person>
<fn>M.</fn>
<sn>Meister</sn>
</person>
<person>
<fn>A.</fn>
<sn>Balaz</sn>
</person>
<person>
<fn>N.</fn>
<sn>Gaaloul</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>jenewein_bragg-diffraction-induced_2022</citeid>
<title>Bragg-diffraction-induced imperfections of the signal in retroreflective atom interferometers</title>
<year>2022</year>
<month>6</month>
<DOI>10.1103/PhysRevA.105.063316</DOI>
<journal>Phys. Rev. A</journal>
<volume>105</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>J.</fn>
<sn>Jenewein</sn>
</person>
<person>
<fn>S.</fn>
<sn>Hartmann</sn>
</person>
<person>
<fn>A.</fn>
<sn>Roura</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>rozenman_periodic_2022</citeid>
<title>Periodic Wave Trains in Nonlinear Media: Talbot Revivals, Akhmediev Breathers, and Asymmetry Breaking</title>
<year>2022</year>
<month>5</month>
<DOI>10.1103/PhysRevLett.128.214101</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>128</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>G. G.</fn>
<sn>Rozenman</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>L.</fn>
<sn>Shemer</sn>
</person>
<person>
<fn>A.</fn>
<sn>Arie</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>di_pumpo_light_2022</citeid>
<title>Light propagation and atom interferometry in gravity and dilaton fields</title>
<year>2022</year>
<month>4</month>
<DOI>10.1103/PhysRevD.105.084065</DOI>
<journal>Phys. Rev. D</journal>
<volume>105</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>F.</fn>
<sn>Di Pumpo</sn>
</person>
<person>
<fn>A.</fn>
<sn>Friedrich</sn>
</person>
<person>
<fn>A.</fn>
<sn>Geyer</sn>
</person>
<person>
<fn>C.</fn>
<sn>Ufrecht</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1116/5.0074429</citeid>
<title>The logarithmic phase singularity in the inverted harmonic oscillator</title>
<year>2022</year>
<month>3</month>
<DOI>10.1116/5.0074429</DOI>
<journal>AVS Quantum Science</journal>
<volume>4</volume>
<authors>
<person>
<fn>F.</fn>
<sn>Ullinger</sn>
</person>
<person>
<fn>M.</fn>
<sn>Zimmermann</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>rodrigues_goncalves_bright_2022</citeid>
<title>Bright and dark diffractive focusing</title>
<abstract>We investigate bright and dark diffractive focusing emerging in the free propagation of specific wave profiles. These general wave phenomena manifest themselves in matter, water, and classical waves. In this article, we lay the foundations for these effects and illustrate their origin in Wigner phase space. Our theoretical studies are supported by experimental demonstrations of dark focusing in water waves. Moreover, by using different phase slits we analyze several aspects of bright and dark focusing for classical and matter waves.</abstract>
<year>2022</year>
<month>2</month>
<DOI>10.1007/s00340-022-07755-5</DOI>
<journal>Applied Physics B</journal>
<volume>128</volume>
<authors>
<person>
<fn>M.</fn>
<sn>Rodrigues Gonçalves</sn>
</person>
<person>
<fn>G. G.</fn>
<sn>Rozenman</sn>
</person>
<person>
<fn>M.</fn>
<sn>Zimmermann</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
</person>
<person>
<fn>W. B.</fn>
<sn>Case</sn>
</person>
<person>
<fn>A.</fn>
<sn>Arie</sn>
</person>
<person>
<fn>L.</fn>
<sn>Shemer</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>asmann_light-pulse_2022</citeid>
<title>Light-pulse atom interferometry with entangled atom-optical elements</title>
<year>2022</year>
<month>2</month>
<DOI>10.1103/PhysRevResearch.4.013115</DOI>
<journal>Phys. Rev. Research</journal>
<volume>4</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>T.</fn>
<sn>Aßmann</sn>
</person>
<person>
<fn>F.</fn>
<sn>Di Pumpo</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>https://doi.org/10.18725/oparu-43717</citeid>
<title>Doppler-free Two-photon Transitions in Atom Interferometry</title>
<year>2022</year>
<month>1</month>
<DOI>10.18725/OPARU-43717</DOI>
<journal>Master Thesis</journal>
<keywords>DDC 530 / Physics,  Quantum theory,  Interferometry,  Atom interferometry,  Atominterferometrie,  Quantenmechanik</keywords>
<authors>
<person>
<fn>G.</fn>
<sn>Janson</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Happ_2022</citeid>
<title>Universality of excited three-body bound states in one dimension</title>
<abstract>We study a heavy–heavy–light three-body system confined to one space dimension in the regime where an excited state in the heavy–light subsystems becomes weakly bound. The associated two-body system is characterized by (i) the structure of the weakly-bound excited heavy–light state and (ii) the presence of deeply-bound heavy–light states. The consequences of these aspects for the behavior of the three-body system are analyzed. We find a strong indication for universal behavior of both three-body binding energies and wave functions for different weakly-bound excited states in the heavy–light subsystems.</abstract>
<year>2022</year>
<month>1</month>
<DOI>10.1088/1361-6455/ac3cc8</DOI>
<journal>Journal of Physics B: Atomic, Molecular and Optical Physics</journal>
<volume>55</volume>
<authors>
<person>
<fn>L.</fn>
<sn>Happ</sn>
</person>
<person>
<fn>M.</fn>
<sn>Zimmermann</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>schleich_2021</citeid>
<title>Geleitwort, in: Kurt Gödels Notizen zur Quantenmechanik</title>
<year>2021</year>
<month>12</month>
<DOI>10.1007/978-3-662-63808-8_1</DOI>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>di_pumpo_gravitational_2021</citeid>
<title>Gravitational Redshift Tests with Atomic Clocks and Atom Interferometers</title>
<year>2021</year>
<month>11</month>
<day>11</day>
<DOI>10.1103/PRXQuantum.2.040333</DOI>
<journal>PRX Quantum</journal>
<volume>2</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>F.</fn>
<sn>Di Pumpo</sn>
</person>
<person>
<fn>C.</fn>
<sn>Ufrecht</sn>
</person>
<person>
<fn>A.</fn>
<sn>Friedrich</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>W. G.</fn>
<sn>Unruh</sn>
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</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Happ_2021</citeid>
<title>Proof of universality in one-dimensional few-body systems including anisotropic interactions</title>
<abstract>We provide an analytical proof of universality for bound states in one-dimensional systems of two and three particles, valid for short-range interactions with negative or vanishing integral over space. The proof is performed in the limit of weak pair-interactions and covers both binding energies and wave functions. Moreover, in this limit the results are formally shown to converge to the respective ones found in the case of the zero-range contact interaction.</abstract>
<year>2021</year>
<month>11</month>
<DOI>10.1088/1361-6455/ac3b3f</DOI>
<journal>Journal of Physics B: Atomic, Molecular and Optical Physics</journal>
<volume>54</volume>
<authors>
<person>
<fn>L.</fn>
<sn>Happ</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
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<reference>
<bibtype>article</bibtype>
<citeid>2021</citeid>
<title>Diffractive focusing of a uniform Bose Einstein condensate</title>
<abstract>We propose a straightforward implementation of the phenomenon of diffractive focusing with uniform atomic Bose–Einstein condensates. Both, analytical as well as numerical methods not only illustrate the influence of the atom–atom interaction on the focusing factor and the focus time, but also allow us to derive the optimal conditions for observing focusing of this type in the case of interacting matter waves.</abstract>
<year>2021</year>
<month>10</month>
<day>19</day>
<DOI>10.1088/1361-6455/ac2ab6</DOI>
<journal>J. Phys. B: At. Mol. Opt. Phys.</journal>
<volume>54</volume>
<authors>
<person>
<fn>P.</fn>
<sn>Boegel</sn>
</person>
<person>
<fn>M.</fn>
<sn>Meister</sn>
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<person>
<fn>J.-N.</fn>
<sn>Siemß</sn>
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<person>
<fn>N.</fn>
<sn>Gaaloul</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
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<reference>
<bibtype>article</bibtype>
<title>Qubit-based momentum measurement of a particle</title>
<abstract>An early approach to include pointers representing measurement devices into quantum mechanics was given by von Neumann. Based on this idea, we model such pointers by qubits and couple them to a free particle, in analogy to a classical time-of-flight arrangement. The corresponding Heisenberg dynamics leads to pointer observables whose expectation values allow us to reconstruct the particle’s momentum distribution via the characteristic function. We investigate different initial qubit states and find that such a reconstruction can be considerably simplified by initially entangled pointers.</abstract>
<year>2021</year>
<month>10</month>
<day>16</day>
<DOI>10.1140/epjd/s10053-021-00282-6</DOI>
<journal>The European Physical Journal D</journal>
<volume>75</volume>
<authors>
<person>
<fn>B.</fn>
<sn>Konrad</sn>
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<person>
<fn>F.</fn>
<sn>Di Pumpo</sn>
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<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>battelier_exploring_2021</citeid>
<title>Exploring the foundations of the physical universe with space tests of the equivalence principle</title>
<abstract>We present the scientific motivation for future space tests of the equivalence principle, and in particular the universality of free fall, at the 10− 17 level or better. Two possible mission scenarios, one based on quantum technologies, the other on electrostatic accelerometers, that could reach that goal are briefly discussed. This publication is a White Paper written in the context of the Voyage 2050 ESA Call for White Papers.</abstract>
<year>2021</year>
<month>9</month>
<DOI>10.1007/s10686-021-09718-8</DOI>
<journal>Experimental Astronomy</journal>
<volume>51</volume>
<authors>
<person>
<fn>B.</fn>
<sn>Battelier</sn>
</person>
<person>
<fn>J.</fn>
<sn>Bergé</sn>
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<person>
<fn>A.</fn>
<sn>Bertoldi</sn>
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<person>
<fn>L.</fn>
<sn>Blanchet</sn>
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<person>
<fn>K.</fn>
<sn>Bongs</sn>
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<person>
<fn>P.</fn>
<sn>Bouyer</sn>
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<person>
<fn>C.</fn>
<sn>Braxmaier</sn>
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<person>
<fn>D.</fn>
<sn>Calonico</sn>
</person>
<person>
<fn>P.</fn>
<sn>Fayet</sn>
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<person>
<fn>N.</fn>
<sn>Gaaloul</sn>
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<person>
<fn>C.</fn>
<sn>Guerlin</sn>
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<person>
<fn>A.</fn>
<sn>Hees</sn>
</person>
<person>
<fn>P.</fn>
<sn>Jetzer</sn>
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<person>
<fn>C.</fn>
<sn>Lämmerzahl</sn>
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<person>
<fn>S.</fn>
<sn>Lecomte</sn>
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<person>
<fn>C.</fn>
<sn>Le Poncin-Lafitte</sn>
</person>
<person>
<fn>S.</fn>
<sn>Loriani</sn>
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<person>
<fn>G.</fn>
<sn>Métris</sn>
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<sn>Nofrarias</sn>
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<person>
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<sn>Reynaud</sn>
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<fn>C.</fn>
<sn>Salomon</sn>
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<fn>S.</fn>
<sn>Schiller</sn>
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<fn>W. P.</fn>
<sn>Schleich</sn>
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<fn>C.</fn>
<sn>Schubert</sn>
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<fn>C. F.</fn>
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<fn>T. J.</fn>
<sn>Sumner</sn>
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<fn>G. M.</fn>
<sn>Tino</sn>
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<fn>P.</fn>
<sn>Tuckey</sn>
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<person>
<fn>W. von</fn>
<sn>Klitzing</sn>
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<person>
<fn>L.</fn>
<sn>Wörner</sn>
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<person>
<fn>P.</fn>
<sn>Wolf</sn>
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<fn>M.</fn>
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<reference>
<bibtype>article</bibtype>
<citeid>seiler_geometric_2021</citeid>
<title>Geometric interpretation of the Clauser-Horne-Shimony-Holt inequality of nonmaximally entangled states</title>
<year>2021</year>
<month>9</month>
<DOI>10.1103/PhysRevA.104.032218</DOI>
<journal>Phys. Rev. A</journal>
<volume>104</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>J.</fn>
<sn>Seiler</sn>
</person>
<person>
<fn>T.</fn>
<sn>Strohm</sn>
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<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
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<reference>
<bibtype>article</bibtype>
<citeid>kling_high-gain_2021</citeid>
<title>High-gain quantum free-electron laser: Long-time dynamics and requirements</title>
<year>2021</year>
<month>9</month>
<DOI>10.1103/PhysRevResearch.3.033232</DOI>
<journal>Phys. Rev. Research</journal>
<volume>3</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>P.</fn>
<sn>Kling</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
<person>
<fn>C. M.</fn>
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<person>
<fn>R.</fn>
<sn>Sauerbrey</sn>
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<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
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</reference>
<reference>
<bibtype>article</bibtype>
<citeid>weisman_diffractive_2021</citeid>
<title>Diffractive Guiding of Waves by a Periodic Array of Slits</title>
<year>2021</year>
<month>7</month>
<day>2</day>
<DOI>10.1103/PhysRevLett.127.014303</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>127</volume>
<note>Publisher: American Physical Society</note>
<authors>
<person>
<fn>D.</fn>
<sn>Weisman</sn>
</person>
<person>
<fn>C. M.</fn>
<sn>Carmesin</sn>
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<person>
<fn>G.G.</fn>
<sn>Rozenman</sn>
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<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
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<person>
<fn>L.</fn>
<sn>Shemer</sn>
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<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>A.</fn>
<sn>Arie</sn>
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<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1063/5.0048806</citeid>
<title>Atom interferometry with quantized light pulses</title>
<year>2021</year>
<month>4</month>
<day>29</day>
<DOI>10.1063/5.0048806</DOI>
<journal>The Journal of Chemical Physics</journal>
<volume>154</volume>
<authors>
<person>
<fn>K.</fn>
<sn>Soukup</sn>
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<person>
<fn>F.</fn>
<sn>Di Pumpo</sn>
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<person>
<fn>T.</fn>
<sn>Aßmann</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
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<person>
<fn>E.</fn>
<sn>Giese</sn>
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<reference>
<bibtype>article</bibtype>
<citeid>Rozenman2021</citeid>
<title>Projectile motion of surface gravity water wave packets: An analogy to quantum mechanics</title>
<abstract>We study phase contributions of wave functions that occur in the evolution of Gaussian surface gravity water wave packets with nonzero initial momenta propagating in the presence and absence of an effective external linear potential. Our approach takes advantage of the fact that in contrast to matter waves, water waves allow us to measure both their amplitudes and phases.</abstract>
<year>2021</year>
<month>4</month>
<day>16</day>
<DOI>10.1140/epjs/s11734-021-00096-y</DOI>
<journal>The European Physical Journal Special Topics</journal>
<volume>230</volume>
<authors>
<person>
<fn>G. G.</fn>
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<person>
<fn>M.</fn>
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<fn>M. A.</fn>
<sn>Efremov</sn>
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<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
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<person>
<fn>W. B.</fn>
<sn>Case</sn>
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<fn>D. M.</fn>
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<fn>L.</fn>
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<person>
<fn>A.</fn>
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<reference>
<bibtype>article</bibtype>
<citeid>lachmann_ultracold_2021</citeid>
<title>Ultracold atom interferometry in space</title>
<abstract>Bose-Einstein condensates ({BECs}) in free fall constitute a promising source for space-borne interferometry. Indeed, {BECs} enjoy a slowly expanding wave function, display a large spatial coherence and can be engineered and probed by optical techniques. Here we explore matter-wave fringes of multiple spinor components of a {BEC} released in free fall employing light-pulses to drive Bragg processes and induce phase imprinting on a sounding rocket. The prevailing microgravity played a crucial role in the observation of these interferences which not only reveal the spatial coherence of the condensates but also allow us to measure differential forces. Our work marks the beginning of matter-wave interferometry in space with future applications in fundamental physics, navigation and earth observation.</abstract>
<year>2021</year>
<month>2</month>
<day>26</day>
<DOI>10.1038/s41467-021-21628-z</DOI>
<journal>Nature Comm.</journal>
<volume>12</volume>
<authors>
<person>
<fn>M.D.</fn>
<sn>Lachmann</sn>
</person>
<person>
<fn>H.</fn>
<sn>Ahlers</sn>
</person>
<person>
<fn>D.</fn>
<sn>Becker</sn>
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<person>
<fn>A. N.</fn>
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<person>
<fn>J.</fn>
<sn>Grosse</sn>
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<fn>V.</fn>
<sn>Schkolnik</sn>
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<person>
<fn>S. T.</fn>
<sn>Seidel</sn>
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<person>
<fn>T.</fn>
<sn>Wendrich</sn>
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<person>
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<fn>B.</fn>
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<fn>E. M.</fn>
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<bibtype>article</bibtype>
<citeid>PhysRevA.103.023305</citeid>
<title>Generalized gravity-gradient mitigation scheme</title>
<year>2021</year>
<month>2</month>
<day>3</day>
<DOI>10.1103/PhysRevA.103.023305</DOI>
<journal>Phys. Rev. A</journal>
<volume>103</volume>
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<fn>C.</fn>
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<bibtype>article</bibtype>
<citeid>frye_bose-einstein_2021</citeid>
<title>The Bose-Einstein Condensate and Cold Atom Laboratory</title>
<abstract>Microgravity eases several constraints limiting experiments with ultracold and condensed atoms on ground. It enables extended times of flight without suspension and eliminates the gravitational sag for trapped atoms. These advantages motivated numerous initiatives to adapt and operate experimental setups on microgravity platforms. We describe the design of the payload, motivations for design choices, and capabilities of the Bose-Einstein Condensate and Cold Atom Laboratory ({BECCAL}), a {NASA}-{DLR} collaboration. {BECCAL} builds on the heritage of previous devices operated in microgravity, features rubidium and potassium, multiple options for magnetic and optical trapping, different methods for coherent manipulation, and will offer new perspectives for experiments on quantum optics, atom optics, and atom interferometry in the unique microgravity environment on board the International Space Station.</abstract>
<year>2021</year>
<month>1</month>
<day>4</day>
<DOI>10.1140/epjqt/s40507-020-00090-8</DOI>
<journal>The European Physical Journal Quantum Technology</journal>
<volume>8</volume>
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<fn>J.</fn>
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<fn>V. A.</fn>
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<fn>J. P.</fn>
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<fn>M.</fn>
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<fn>M.</fn>
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<person>
<fn>H.</fn>
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<fn>H.</fn>
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<person>
<fn>A. M.</fn>
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<person>
<fn>T.</fn>
<sn>Oberschulte</sn>
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<person>
<fn>A.</fn>
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<fn>J.</fn>
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<fn>A.</fn>
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<fn>E. M.</fn>
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<fn>A.</fn>
<sn>Roura</sn>
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<person>
<fn>M.</fn>
<sn>Sbroscia</sn>
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<fn>W. P.</fn>
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<person>
<fn>C.</fn>
<sn>Schubert</sn>
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<fn>C.</fn>
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<fn>D.</fn>
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<fn>B. K.</fn>
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<fn>M.</fn>
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<fn>T.</fn>
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<fn>A.</fn>
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<fn>N.</fn>
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<citeid>PhysRevA.102.063326</citeid>
<title>Atomic Raman scattering: Third-order diffraction in a double geometry</title>
<year>2020</year>
<month>12</month>
<day>22</day>
<DOI>10.1103/PhysRevA.102.063326</DOI>
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<fn>S.</fn>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevResearch.2.043240</citeid>
<title>Atom-interferometric test of the universality of gravitational redshift and free fall</title>
<year>2020</year>
<month>11</month>
<day>16</day>
<DOI>10.1103/PhysRevResearch.2.043240</DOI>
<journal>Phys. Rev. Research</journal>
<volume>2</volume>
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<fn>C.</fn>
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<fn>F.</fn>
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<fn>A.</fn>
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<person>
<fn>A.</fn>
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<abstract>We revisit the pointer-based measurement concept of von Neumann which allows us to model a quantum counterpart of the classical time-of-flight (ToF) momentum. Our approach is based on the Hamiltonian for a particle interacting with two quantum pointers serving as basic measurement devices. The corresponding dynamics leads to a pointer-based ToF observable for the operational momentum of the particle. We can consider single measurements of our quantum pointers and show that this process will result in a state reduction for a single particle being downstream of the time-of-flight setup.</abstract>
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<publisher>American Physical Society</publisher>
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<title>The photon: the role of its mode function in analyzing complementarity</title>
<abstract>We investigate the role of the spatial mode function in a single-photon experiment designed to demonstrate the principle of complementarity. Our approach employs entangled photons created by spontaneous parametric downconversion from a pump mode in a TEM01 mode together with a double slit. Measuring the interference of the signal photons behind the double slit in coincidence with the entangled idler photons at different positions, we select signal photons of different mode functions. When the signal photons belong to the TEM01-like double-hump mode, we obtain almost perfect visibility of the interference fringes, and no ``which slit'' information is available in the idler photon detected before the slits. This result is remarkable because the entangled signal and idler photon pairs are created each time in only one of the two intensity humps. However, when we break the symmetry between the two maxima of the signal photon mode structure, the paths through the slits for these additional photons become distinguishable and the visibility vanishes. It is the mode function of the photons selected by the detection system that decides if interference or ``which slit'' information is accessible in the experiment.</abstract>
<year>2019</year>
<month>6</month>
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<title>High-gain quantum free-electron laser: Emergence and exponential gain</title>
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<year>2019</year>
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<abstract>Since the first proof-of-principle experiments over 25 years ago, atom interferometry has matured to a versatile tool that can be used in fundamental research in particle physics, general relativity and cosmology. At the same time, atom interferometers are currently moving out of the laboratory to be used as ultraprecise quantum sensors in metrology, geophysics, space, civil engineering, oil and minerals exploration, and navigation. This Perspective discusses the associated scientific and technological challenges and highlights recent advances.</abstract>
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<booktitle>Foundations of quantum theory</booktitle>
<volume>197</volume>
<publisher>IOS Press</publisher>
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<series>Proceedings of the International School of Physics "Enrico Fermi"</series>
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<abstract>Atom laser experiments with Bose–Einstein condensates (BECs) performed in ground-based laboratories feature a coherent and directed beam of atoms which is accelerated by gravity. In microgravity the situation is fundamentally different because the dynamics is entirely determined by the repulsive interaction between the atoms and not by the gravitational force. As a result, the output of a space atom laser is a spherical wave slowly expanding away from the initial BEC. We present a thorough theoretical study of this new source of matter waves based on rf outcoupling which exhibits an isotropic distribution both in position and momentum even for an initially anisotropic trap. The unique geometry of such a freely expanding, shell-shaped BEC offers new possibilities for matter waves in microgravity and is complementary to other matter-wave sources prepared by delta-kick collimation or adiabatic expansion. Our work paves the way for the upcoming experimental realization of a space atom laser making use of NASA’s Cold Atom Laboratory on the International Space Station.</abstract>
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<year>2019</year>
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<booktitle>Foundations of quantum theory</booktitle>
<volume>197</volume>
<publisher>IOS Press</publisher>
<address>Amsterdam, Oxford, Tokyo, Washington DC</address>
<series>Proceedings of the International School of Physics "Enrico Fermi"</series>
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<title>Equivalent formulations of the Riemann hypothesis based on lines of constant phase</title>
<abstract>We prove the equivalence of three formulations of the Riemann hypothesis for functions f defined by the four assumptions: (a
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<publisher>{IOP} Publishing</publisher>
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<abstract>We show that the expectation value of the operator  defined by the position and momentum operators  and  with a positive parameter c can serve as a tool to identify quantum non-Gaussian states, that is states that cannot be represented as a mixture of Gaussian states. Our condition can be readily tested employing a highly efficient homodyne detection which unlike quantum-state tomography requires the measurements of only two orthogonal quadratures. We demonstrate that our method is even able to detect quantum non-Gaussian states with positive–definite Wigner functions. This situation cannot be addressed in terms of the negativity of the phase-space distribution. Moreover, we demonstrate that our condition can characterize quantum non-Gaussianity for the class of superposition states consisting of a vacuum and integer multiples of four photons under more than 50 % signal attenuation.</abstract>
<year>2018</year>
<month>2</month>
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<publisher>{IOP} Publishing</publisher>
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<title>Gain in single and paired parametric oscillators</title>
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<title>Light, the universe and everything – 12 Herculean tasks for quantum cowboys and black diamond skiers</title>
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<citeid>Gleisberg_2018</citeid>
<title>Prime factorization of arbitrary integers with a logarithmic energy spectrum</title>
<abstract>We propose an iterative scheme to factor numbers based on the quantum dynamics of an ensemble of interacting bosonic atoms stored in a trap where the single-particle energy spectrum depends logarithmically on the quantum number. When excited by a time-dependent interaction these atoms perform Rabi oscillations between the ground state and an energy state characteristic of the factors. The number to be factored is encoded into the frequency of the sinusoidally modulated interaction. We show that a measurement of the energy of the atoms at a time chosen at random yields the factors with probability one half. We conclude by discussing a protocol to obtain the desired prime factors employing a logarithmic energy spectrum which consists of prime numbers only.</abstract>
<year>2018</year>
<month>1</month>
<DOI>10.1088/1361-6455/aa9957</DOI>
<journal>Journal of Physics B: Atomic, Molecular and Optical Physics</journal>
<volume>51</volume>
<publisher>{IOP} Publishing</publisher>
<pages>035009</pages>
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<title>Quantum optics approach to radiation from atoms falling into a black hole</title>
<abstract>Using a combination of quantum optics and general relativity, we show that the radiation emitted by atoms falling into a black hole looks like, but is different from, Hawking radiation. This analysis also provides insight into the Einstein principle of equivalence between acceleration and gravity.We show that atoms falling into a black hole (BH) emit acceleration radiation which, under appropriate initial conditions, looks to a distant observer much like (but is different from) Hawking BH radiation. In particular, we find the entropy of the acceleration radiation via a simple laser-like analysis. We call this entropy horizon brightened acceleration radiation (HBAR) entropy to distinguish it from the BH entropy of Bekenstein and Hawking. This analysis also provides insight into the Einstein principle of equivalence between acceleration and gravity.</abstract>
<year>2018</year>
<issn>0027-8424</issn>
<DOI>10.1073/pnas.1807703115</DOI>
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<volume>115</volume>
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<citeid>Becker2018</citeid>
<title>Space-borne Bose-Einstein condensation for precision interferometry</title>
<abstract>Owing to the low-gravity conditions in space, space-borne laboratories enable experiments with extended free-fall times. Because Bose-Einstein condensates have an extremely low expansion energy, space-borne atom interferometers based on Bose-Einstein condensation have the potential to have much greater sensitivity to inertial forces than do similar ground-based interferometers. On 23 January 2017, as part of the sounding-rocket mission MAIUS-1, we created Bose-Einstein condensates in space and conducted 110 experiments central to matter-wave interferometry, including laser cooling and trapping of atoms in the presence of the large accelerations experienced during launch. Here we report on experiments conducted during the six minutes of in-space flight in which we studied the phase transition from a thermal ensemble to a Bose-Einstein condensate and the collective dynamics of the resulting condensate. Our results provide insights into conducting cold-atom experiments in space, such as precision interferometry, and pave the way to miniaturizing cold-atom and photon-based quantum information concepts for satellite-based implementation. In addition, space-borne Bose-Einstein condensation opens up the possibility of quantum gas experiments in low-gravity conditions1,2.</abstract>
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<DOI>10.1038/s41586-018-0605-1</DOI>
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<title>Comprehensive classification for Bose-Fermi mixtures</title>
<abstract>We present analytical studies of a trapped boson-fermion mixture at zero temperature with spin-polarized fermions. Using the Thomas–Fermi approximation for bosons and the local-density approximation for fermions, we find a large variety of different density shapes. In the case of continuous density, we obtain analytic conditions for each configuration for attractive as well as repulsive boson-fermion interaction. Furthermore, we analytically show that all the scenarios we describe are minima of the grand-canonical energy functional. Finally, we provide a full classification of all possible ground states in the interpenetrative regime. Our results also apply to binary mixtures of bosons.</abstract>
<year>2017</year>
<month>8</month>
<DOI>10.1088/1367-2630/aa7814</DOI>
<journal>New Journal of Physics</journal>
<volume>19</volume>
<publisher>{IOP} Publishing</publisher>
<pages>085001</pages>
<number>8</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2Faa7814</file_url>
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<fn>C.</fn>
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<fn>M.</fn>
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<fn>A.</fn>
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<person>
<fn>W. P.</fn>
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<citeid>Kim_2017</citeid>
<title>A perfect memory makes the continuous Newton method look ahead</title>
<abstract>Hauser and Nedić (2005 SIAM J. Optim. 15 915) have pointed out an intriguing property of a perturbed flow line generated by the continuous Newton method: it returns to the unperturbed one once the perturbation ceases to exist. We show that this feature is a direct consequence of the phase being constant along any Newton trajectory, that is, once a phase always that phase.</abstract>
<year>2017</year>
<month>7</month>
<DOI>10.1088/1402-4896/aa7ae3</DOI>
<journal>Physica Scripta</journal>
<volume>92</volume>
<publisher>{IOP} Publishing</publisher>
<pages>085201</pages>
<number>8</number>
<file_url>https://doi.org/10.1088%2F1402-4896%2Faa7ae3</file_url>
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<person>
<fn>M. B.</fn>
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<fn>J. W.</fn>
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<citeid>PhysRevA.96.013827</citeid>
<title>Hidden PT symmetry and quantization of a coupled-oscillator model of quantum amplification by superradiant emission of radiation</title>
<year>2017</year>
<month>7</month>
<DOI>10.1103/PhysRevA.96.013827</DOI>
<journal>Phys. Rev. A</journal>
<volume>96</volume>
<publisher>American Physical Society</publisher>
<pages>013827</pages>
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<fn>L.</fn>
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<fn>M. O.</fn>
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<citeid>PhysRevLett.118.154301</citeid>
<title>Diffractive Focusing of Waves in Time and in Space</title>
<year>2017</year>
<month>4</month>
<DOI>10.1103/PhysRevLett.118.154301</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>118</volume>
<publisher>American Physical Society</publisher>
<pages>154301</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.118.154301</file_url>
<authors>
<person>
<fn>D.</fn>
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<bibtype>article</bibtype>
<citeid>Goncalves2017</citeid>
<title>Single-slit focusing and its representations</title>
<abstract>We illustrate the phenomenon of the focusing of a freely propagating rectangular wave packet using three different tools: (1) the time-dependent wave function in position space, (2) the Wigner phase-space approach, and (3) an experiment using laser light.</abstract>
<year>2017</year>
<month>3</month>
<day>30</day>
<issn>1432-0649</issn>
<DOI>10.1007/s00340-017-6675-1</DOI>
<journal>Applied Physics B</journal>
<volume>123</volume>
<pages>121</pages>
<number>4</number>
<file_url>https://doi.org/10.1007/s00340-017-6675-1</file_url>
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<citeid>Zimmermann2017</citeid>
<title>T³-Interferometer for atoms</title>
<abstract>The quantum mechanical propagator of a massive particle in a linear gravitational potential derived already in 1927 by Kennard [2, 3] contains a phase that scales with the third power of the time T during which the particle experiences the corresponding force. Since in conventional atom interferometers the internal atomic states are all exposed to the same acceleration a, this {\$}{\$}T^3{\$}{\$}T3-phase cancels out and the interferometer phase scales as {\$}{\$}T^2{\$}{\$}T2. In contrast, by applying an external magnetic field we prepare two different accelerations {\$}{\$}a{\_}1{\$}{\$}a1and {\$}{\$}a{\_}2{\$}{\$}a2for two internal states of the atom, which translate themselves into two different cubic phases and the resulting interferometer phase scales as {\$}{\$}T^3{\$}{\$}T3. We present the theoretical background for, and summarize our progress towards experimentally realizing such a novel atom interferometer.</abstract>
<year>2017</year>
<month>3</month>
<day>20</day>
<issn>1432-0649</issn>
<DOI>10.1007/s00340-017-6655-5</DOI>
<journal>Applied Physics B</journal>
<volume>123</volume>
<pages>102</pages>
<number>4</number>
<file_url>https://doi.org/10.1007/s00340-017-6655-5</file_url>
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<fn>M.</fn>
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<fn>M. A.</fn>
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<fn>W. P.</fn>
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<person>
<fn>S. A.</fn>
<sn>DeSavage</sn>
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<fn>S. A.</fn>
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<fn>E. M.</fn>
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<citeid>MEISTER2017375</citeid>
<title>Chapter Six - Efficient Description of Bose–Einstein Condensates in Time-Dependent Rotating Traps</title>
<abstract>Quantum sensors based on matter-wave interferometry are promising candidates for high-precision gravimetry and inertial sensing in space. The favorable sources for the coherent matter waves in these devices are Bose–Einstein condensates. A reliable prediction of their dynamics, which is governed by the Gross–Pitaevskii equation, requires suitable analytical and numerical methods, which take into account the center-of-mass motion of the condensate, its rotation, and its spatial expansion by many orders of magnitude. In this chapter, we present an efficient way to study their dynamics in time-dependent rotating traps that meet this objective. Both an approximate analytical solution for condensates in the Thomas–Fermi regime and dedicated numerical simulations on a variable adapted grid are discussed. We contrast and relate our approach to previous alternative methods and provide further results, such as analytical expressions for the one- and two-dimensional spatial density distributions and the momentum distribution in the long-time limit that are of immediate interest to experimentalists working in this field of research.</abstract>
<year>2017</year>
<issn>1049-250X</issn>
<DOI>https://doi.org/10.1016/bs.aamop.2017.03.006</DOI>
<volume>66</volume>
<publisher>Academic Press</publisher>
<series>Advances In Atomic, Molecular, and Optical Physics</series>
<editor>Ennio Arimondo and Chun C. Lin and Susanne F. Yelin</editor>
<pages>375 - 438</pages>
<keywords>Bose–Einstein condensate, Gross–Pitaevskii equation, Thomas–Fermi approximation, Scaling approach, Time-dependent rotating trap, Numerical simulation, Hamiltonian formalism, Integrated density distribution</keywords>
<file_url>http://www.sciencedirect.com/science/article/pii/S1049250X17300174</file_url>
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<person>
<fn>M.</fn>
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<fn>St.</fn>
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<citeid>doi:10.1002/prop.201700015</citeid>
<title>The beginning of time observed in quantum jumps</title>
<abstract>The phenomenon of quantum jumps observed in a single ion stored in a trap brings to light intimate connections between three different concepts of quantum physics: (i) quantum state trajectories, (ii) Gamow states, and (iii) the arrow of time. In particular, it allows us to identify the starting time of the semigroup time evolution.</abstract>
<year>2017</year>
<DOI>10.1002/prop.201700015</DOI>
<journal>Fortschritte der Physik</journal>
<volume>65</volume>
<pages>1700015</pages>
<number>6-8</number>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/prop.201700015</file_url>
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<citeid>doi:10.1002/prop.201600092</citeid>
<title>Working in phase-space with Wigner and Weyl</title>
<abstract>Quantum phase-space distributions offer a royal road into the fascinating quantum–classical interface; the Wigner function being the first and best example. However, the subject is frequent with subtleties and textbook-level misinformation; e.g. “The Wigner distribution can give wrong answers for some operator expectation values” . Since the Wigner distribution is just another representation of the density matrix, it must yield correct answers. To that end, Marlan Scully has asked at several international conferences (the 2015 Prague conference being one of them) the following question: “Starting with the density matrix (not the Moyal characteristic function), could you give me a simple direct derivation of the Wigner distribution?” Section contains his answer. In Appendix D, we give a related treatment and make contact with other approaches. We hope that as a result of our studies, the Wigner distribution will become more deeply appreciated.</abstract>
<year>2017</year>
<DOI>10.1002/prop.201600092</DOI>
<journal>Fortschritte der Physik</journal>
<volume>65</volume>
<pages>1600092</pages>
<number>6-8</number>
<keywords>Phase space quantum mechanics, Wigner Weyl distribution, Wigner Weyl symmetric ordering, Weyl and its inverse transform, operator symbol correspondence</keywords>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/prop.201600092</file_url>
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<title>Zum Gedenken an Georg Süßmann – Ein Leben für die Wissenschaft</title>
<year>2017</year>
<journal>Physik Journal</journal>
<volume>16</volume>
<number>8-9</number>
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<person>
<fn>W. P.</fn>
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<citeid>Kling2016</citeid>
<title>Quantum regime of a free-electron laser: relativistic approach</title>
<abstract>In the quantum regime of the free-electron laser, the dynamics of the electrons is not governed by continuous trajectories but by discrete jumps in momentum. In this article, we rederive the two crucial conditions to enter this quantum regime: (1) a large quantum mechanical recoil of the electron caused by the scattering with the laser and the wiggler field and (2) a small energy spread of the electron beam. In contrast to our recent approach based on nonrelativistic quantum mechanics in a co-moving frame of reference, we now pursue a model in the laboratory frame employing relativistic quantum electrodynamics.</abstract>
<year>2016</year>
<month>12</month>
<day>15</day>
<issn>1432-0649</issn>
<DOI>10.1007/s00340-016-6571-0</DOI>
<journal>Applied Physics B</journal>
<volume>123</volume>
<pages>9</pages>
<number>1</number>
<file_url>https://doi.org/10.1007/s00340-016-6571-0</file_url>
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<fn>P.</fn>
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<citeid>PhysRevA.94.063619</citeid>
<title>Light shifts in atomic Bragg diffraction</title>
<year>2016</year>
<month>12</month>
<DOI>10.1103/PhysRevA.94.063619</DOI>
<journal>Phys. Rev. A</journal>
<volume>94</volume>
<publisher>American Physical Society</publisher>
<pages>063619</pages>
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<title>Atom-Chip Fountain Gravimeter</title>
<year>2016</year>
<month>11</month>
<DOI>10.1103/PhysRevLett.117.203003</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>117</volume>
<publisher>American Physical Society</publisher>
<pages>203003</pages>
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<citeid>PhysRevLett.116.173601</citeid>
<title>Double Bragg Interferometry</title>
<year>2016</year>
<month>4</month>
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<journal>Phys. Rev. Lett.</journal>
<volume>116</volume>
<publisher>American Physical Society</publisher>
<pages>173601</pages>
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<citeid>Kaltenbaek2016</citeid>
<title>Macroscopic Quantum Resonators (MAQRO): 2015 update</title>
<abstract>Do the laws of quantum physics still hold for macroscopic objects?- this is at the heart of Schrödinger's cat paradox?- or do gravitation or yet unknown effects set a limit for massive particles? What is the fundamental relation between quantum physics and gravity? Ground-based experiments addressing these questions may soon face limitations due to limited free-fall times and the quality of vacuum and microgravity. The proposed mission Macroscopic Quantum Resonators (MAQRO) may overcome these limitations and allow addressing such fundamental questions. MAQRO harnesses recent developments in quantum optomechanics, high-mass matter-wave interferometry as well as state-of-the-art space technology to push macroscopic quantum experiments towards their ultimate performance limits and to open new horizons for applying quantum technology in space. The main scientific goal is to probe the vastly unexplored 'quantum-classical' transition for increasingly massive objects, testing the predictions of quantum theory for objects in a size and mass regime unachievable in ground-based experiments. The hardware will largely be based on available space technology. Here, we present the MAQRO proposal submitted in response to the 4th Cosmic Vision call for a medium-sized mission (M4) in 2014 of the European Space Agency (ESA) with a possible launch in 2025, and we review the progress with respect to the original MAQRO proposal for the 3rd Cosmic Vision call for a medium-sized mission (M3) in 2010. In particular, the updated proposal overcomes several critical issues of the original proposal by relying on established experimental techniques from high-mass matter-wave interferometry and by introducing novel ideas for particle loading and manipulation. Moreover, the mission design was improved to better fulfill the stringent environmental requirements for macroscopic quantum experiments.</abstract>
<year>2016</year>
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<DOI>10.1140/epjqt/s40507-016-0043-7</DOI>
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<volume>3</volume>
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<fn>S.</fn>
<sn>Reynaud</sn>
</person>
<person>
<fn>C. J.</fn>
<sn>Riedel</sn>
</person>
<person>
<fn>M.</fn>
<sn>Rodrigues</sn>
</person>
<person>
<fn>L.</fn>
<sn>Rondin</sn>
</person>
<person>
<fn>A.</fn>
<sn>Roura</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>J.</fn>
<sn>Schmiedmayer</sn>
</person>
<person>
<fn>T.</fn>
<sn>Schuldt</sn>
</person>
<person>
<fn>K. C.</fn>
<sn>Schwab</sn>
</person>
<person>
<fn>M.</fn>
<sn>Tajmar</sn>
</person>
<person>
<fn>G. M.</fn>
<sn>Tino</sn>
</person>
<person>
<fn>H.</fn>
<sn>Ulbricht</sn>
</person>
<person>
<fn>R.</fn>
<sn>Ursin</sn>
</person>
<person>
<fn>V.</fn>
<sn>Vedral</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<citeid>Schleich2016</citeid>
<title>Wave-Particle Dualism in Action</title>
<abstract>The wave-particle dualism, that is the wave nature of particles and the particle nature of light together with the uncertainty relation of Werner Heisenberg and the principle of complementarity formulated by Niels Bohr represent pillars of quantum theory. We provide an introduction into these fascinating yet strange aspects of the microscopic world and summarize key experiments confirming these concepts so alien to our daily life.</abstract>
<year>2016</year>
<isbn>978-3-319-31903-2</isbn>
<DOI>10.1007/978-3-319-31903-2_19</DOI>
<publisher>Springer International Publishing</publisher>
<address>Cham</address>
<editor>M. D. Al-Amri, M. El-Gomati and M. S. Zubairy</editor>
<pages>483--504</pages>
<file_url>https://doi.org/10.1007/978-3-319-31903-2_19</file_url>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Kling_2015</citeid>
<title>What defines the quantum regime of the free-electron laser?</title>
<abstract>The quantum regime of the free-electron laser (FEL) emerges when the discreteness of the momentum of the electron plays a dominant role in the interaction with the laser and the wiggler field. Motivated by a heuristic phase space approach we pursue two different routes to define the transition from the classical FEL to the quantum domain: (i) standard perturbation theory and (ii) the method of averaging. Moreover, we discuss the experimental requirements for realizing a Quantum FEL and connect them to today's capabilities.</abstract>
<year>2015</year>
<month>12</month>
<DOI>10.1088/1367-2630/17/12/123019</DOI>
<journal>New Journal of Physics</journal>
<volume>17</volume>
<publisher>{IOP} Publishing</publisher>
<pages>123019</pages>
<number>12</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F17%2F12%2F123019</file_url>
<authors>
<person>
<fn>P.</fn>
<sn>Kling</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
<person>
<fn>R.</fn>
<sn>Endrich</sn>
</person>
<person>
<fn>P.</fn>
<sn>Preiss</sn>
</person>
<person>
<fn>R.</fn>
<sn>Sauerbrey</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Neuberger_2015</citeid>
<title>The Riemann hypothesis illuminated by the Newton flow of ζ*</title>
<abstract>We analyze the Newton flow of the Riemann zeta function ζ and rederive in an elementary way the Riemann–von Mangoldt estimate of the number of non-trivial zeros below a given imaginary part. The representation of the flow on the Riemann sphere highlights the importance of the North pole as the starting and turning point of the separatrices, that is of the continental divides of the Newton flow. We argue that the resulting patterns may lead to deeper insight into the Riemann hypothesis. For this purpose we also compare and contrast the Newton flow of ζ with that of a function which in many ways is similar to ζ, but violates the Riemann hypothesis.</abstract>
<year>2015</year>
<month>10</month>
<DOI>10.1088/0031-8949/90/10/108015</DOI>
<journal>Physica Scripta</journal>
<volume>90</volume>
<publisher>{IOP} Publishing</publisher>
<pages>108015</pages>
<number>10</number>
<file_url>https://doi.org/10.1088%2F0031-8949%2F90%2F10%2F108015</file_url>
<authors>
<person>
<fn>J. W.</fn>
<sn>Neuberger</sn>
</person>
<person>
<fn>C.</fn>
<sn>Feiler</sn>
</person>
<person>
<fn>H.</fn>
<sn>Maier</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Paul_2015</citeid>
<title>The Stefan-Boltzmann law: two classical laws give a quantum one</title>
<abstract>Due to the universality of blackbody radiation the constant in the Stefan–Boltzmann law connecting the energy density and temperature of blackbody radiation is either a universal constant, or built out of several universal constants. Since the Stefan–Boltzmann law follows from thermodynamics and classical electrodynamics this constant must involve the speed of light and the Boltzmann constant. However, a dimensional analysis points to the existence of an additional universal constant not present in the two classical theories giving birth to the Stefan–Boltzmann law. In the most elementary version this constant has the dimension of an action and is thereby proportional to Planck’s constant. We point out this unusual phenomenon of the combination of two classical laws creating a quantum law and speculate about its deeper origin.</abstract>
<year>2015</year>
<month>10</month>
<DOI>10.1088/0031-8949/2015/t165/014027</DOI>
<journal>Physica Scripta</journal>
<volume>T165</volume>
<publisher>{IOP} Publishing</publisher>
<pages>014027</pages>
<file_url>https://doi.org/10.1088%2F0031-8949%2F2015%2Ft165%2F014027</file_url>
<authors>
<person>
<fn>D. M.</fn>
<sn>Greenberger</sn>
</person>
<person>
<fn>S. T.</fn>
<sn>Stenholm</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Schleich_2015</citeid>
<title>A wave equation interpolating between classical and quantum mechanics</title>
<abstract>We derive a ‘master’ wave equation for a family of complex-valued waves  whose phase dynamics is dictated by the Hamilton–Jacobi equation for the classical action . For a special choice of the dynamics of the amplitude R which eliminates all remnants of classical mechanics associated with  our wave equation reduces to the Schrödinger equation. In this case the amplitude satisfies a Schrödinger equation analogous to that of a charged particle in an electromagnetic field where the roles of the scalar and the vector potentials are played by the classical energy and the momentum, respectively. In general this amplitude is complex and thereby creates in addition to the classical phase  a quantum phase. Classical statistical mechanics, as described by a classical matter wave, follows from our wave equation when we choose the dynamics of the amplitude such that it remains real for all times. Our analysis shows that classical and quantum matter waves are distinguished by two different choices of the dynamics of their amplitudes rather than two values of Planck’s constant.</abstract>
<year>2015</year>
<month>9</month>
<DOI>10.1088/0031-8949/90/10/108009</DOI>
<journal>Physica Scripta</journal>
<volume>90</volume>
<publisher>{IOP} Publishing</publisher>
<pages>108009</pages>
<number>10</number>
<file_url>https://doi.org/10.1088%2F0031-8949%2F90%2F10%2F108009</file_url>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>D. M.</fn>
<sn>Greenberger</sn>
</person>
<person>
<fn>D. H.</fn>
<sn>Kobe</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Leuchs_2015</citeid>
<title>Intensity-intensity correlations determined by dimension of quantum state in phase space: P-distribution</title>
<abstract>We use the P-distribution to show that the familiar values 1, 2 and 3 of the normalized second order correlation function at equal times  corresponding to a coherent state, a thermal state and a highly squeezed vacuum are a consequence of the number of dimensions these states take up in quantum phase space. Whereas the thermal state exhibits rotational symmetry and thus extends over two dimensions, the squeezed vacuum factorizes into two independent one-dimensional phase space variables, and in the limit of large squeezing is therefore a one-dimensional object. The coherent state is a point in the phase space of the P-distribution and thus has zero dimensions. The fact that for photon number states the P-distribution is even narrower than that of the zero-dimensional coherent state suggests the notion of ‘negative’ dimensions.</abstract>
<year>2015</year>
<month>9</month>
<DOI>10.1088/0031-8949/90/10/108007</DOI>
<journal>Physica Scripta</journal>
<volume>90</volume>
<publisher>{IOP} Publishing</publisher>
<pages>108007</pages>
<number>10</number>
<file_url>https://doi.org/10.1088%2F0031-8949%2F90%2F10%2F108007</file_url>
<authors>
<person>
<fn>G.</fn>
<sn>Leuchs</sn>
</person>
<person>
<fn>R. J.</fn>
<sn>Glauber</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Leuchs_2015</citeid>
<title>Dimension of quantum phase space measured by photon correlations</title>
<abstract>We show that the different values 1, 2 and 3 of the normalized second-order correlation function  corresponding to a coherent state, a thermal state and a highly squeezed vacuum originate from the different dimensionality of these states in phase space. In particular, we derive an exact expression for  in terms of the ratio of the moments of the classical energy evaluated with the Wigner function of the quantum state of interest and corrections proportional to the reciprocal of powers of the average number of photons. In this way we establish a direct link between  and the shape of the state in phase space. Moreover, we illuminate this connection by demonstrating that in the semi-classical limit the familiar photon statistics of a thermal state arise from an area in phase space weighted by a two-dimensional Gaussian, whereas those of a highly squeezed state are governed by a line-integral of a one-dimensional Gaussian.</abstract>
<year>2015</year>
<month>6</month>
<DOI>10.1088/0031-8949/90/7/074066</DOI>
<journal>Physica Scripta</journal>
<volume>90</volume>
<publisher>{IOP} Publishing</publisher>
<pages>074066</pages>
<number>7</number>
<file_url>https://doi.org/10.1088%2F0031-8949%2F90%2F7%2F074066</file_url>
<authors>
<person>
<fn>G.</fn>
<sn>Leuchs</sn>
</person>
<person>
<fn>R. J.</fn>
<sn>Glauber</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Feiler_2015</citeid>
<title>Dirichlet series as interfering probability amplitudes for quantum measurements</title>
<abstract>We show that all Dirichlet series, linear combinations of them and their analytical continuations represent probability amplitudes for measurements on time-dependent quantum systems. In particular, we connect an arbitrary Dirichlet series to the time evolution of an appropriately prepared quantum state in a non-linear oscillator with logarithmic energy spectrum. However, the realization of a superposition of two Dirichlet sums and its analytical continuation requires two quantum systems which are entangled, and a joint measurement. We illustrate our approach of implementing arbitrary Dirichlet series in quantum systems using the example of the Riemann zeta function and relate its non-trivial zeros to the interference of two quantum states reminiscent of a Schrödinger cat.</abstract>
<year>2015</year>
<month>6</month>
<DOI>10.1088/1367-2630/17/6/063040</DOI>
<journal>New Journal of Physics</journal>
<volume>17</volume>
<publisher>{IOP} Publishing</publisher>
<pages>063040</pages>
<number>6</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F17%2F6%2F063040</file_url>
<authors>
<person>
<fn>C.</fn>
<sn>Feiler</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevLett.114.063002</citeid>
<title>Composite-Light-Pulse Technique for High-Precision Atom Interferometry</title>
<year>2015</year>
<month>2</month>
<DOI>10.1103/PhysRevLett.114.063002</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>114</volume>
<publisher>American Physical Society</publisher>
<pages>063002</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.114.063002</file_url>
<authors>
<person>
<fn>P.</fn>
<sn>Berg</sn>
</person>
<person>
<fn>S.</fn>
<sn>Abend</sn>
</person>
<person>
<fn>G.</fn>
<sn>Tackmann</sn>
</person>
<person>
<fn>C.</fn>
<sn>Schubert</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>F. A.</fn>
<sn>Narducci</sn>
</person>
<person>
<fn>W.</fn>
<sn>Ertmer</sn>
</person>
<person>
<fn>E. M.</fn>
<sn>Rasel</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>D_m_t_r_2015</citeid>
<title>Scattering of a particle with internal structure from a single slit: exact numerical solutions</title>
<abstract>Scattering of a quantum particle with internal structure is fundamentally different from that of a point particle and shows quantum effects such as the modification of transmission due to tunnelling and trapping of the particle. As in a preceding paper (Shore et al 2014 New J. Phys. 17 013046) we consider a model of a symmetric, rigid rotor travelling through an aperture in a thin but impenetrable screen which is perpendicular to both the direction of motion and the rotation axis. We determine the quantum mechanical properties of this two-dimensional geometrical model using a quasi one-dimensional scattering problem with unconventional boundaries. Our calculations rely on finding the Green's function, which has a direct connection to the scattering matrix. Evaluated on a discrete lattice the Hamiltonian is ‘dressed’ by a self-energy correction that takes into account the open boundary conditions in an exact way. We find that the passage through the aperture can be suppressed or enhanced as a result of the rotational motion. These effects manifest themselves through resonances in the transmission probability as a function of incident energy and symmetry of the incident wavefunction. We determine the density-of-states to reveal the mode structure of resonant states and to exhibit the lifetimes of temporary trapping within the aperture.</abstract>
<year>2015</year>
<month>2</month>
<DOI>10.1088/1367-2630/17/2/023044</DOI>
<journal>New Journal of Physics</journal>
<volume>17</volume>
<publisher>{IOP} Publishing</publisher>
<pages>023044</pages>
<number>2</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F17%2F2%2F023044</file_url>
<authors>
<person>
<fn>P.</fn>
<sn>Dömötör</sn>
</person>
<person>
<fn>P.</fn>
<sn>Földi</sn>
</person>
<person>
<fn>M. G.</fn>
<sn>Benedict</sn>
</person>
<person>
<fn>B. W.</fn>
<sn>Shore</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>GLEISBERG20152556</citeid>
<title>Factorization with a logarithmic energy spectrum of a two-dimensional potential</title>
<abstract>We propose a method to factor numbers using a single particle caught in a separable two-dimensional potential with a logarithmic energy spectrum. The particle initially prepared in the ground state is excited with high probability by a sinusoidally time-dependent perturbation into a state whose two quantum numbers represent the factors of a number encoded in the frequency of the perturbation. We discuss the limitations of our method arising from off-resonant transitions and from decoherence.</abstract>
<year>2015</year>
<issn>0375-9601</issn>
<DOI>https://doi.org/10.1016/j.physleta.2015.05.038</DOI>
<journal>Physics Letters A</journal>
<volume>379</volume>
<pages>2556 - 2560</pages>
<number>40</number>
<keywords>Number theory, Trapped particle, Factorization protocol</keywords>
<file_url>http://www.sciencedirect.com/science/article/pii/S0375960115005137</file_url>
<authors>
<person>
<fn>F.</fn>
<sn>Gleisberg</sn>
</person>
<person>
<fn>M.</fn>
<sn>Volpp</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>report</bibtype>
<title>Perspektiven der Quantentechnologien</title>
<year>2015</year>
<isbn>978-3-8047-3343-5</isbn>
<booktitle>Perspektiven der Quantentechnologien</booktitle>
<publisher>Nationale Akademie der Wissenschaften Leopoldina, acatech - Deutsche Akademie der Technikwissenschaften, Union der deutschen Akademien der Wissenschaften</publisher>
<address>Halle (Saale)</address>
<pages>64</pages>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>KLEINERT20151</citeid>
<title>Representation-free description of light-pulse atom interferometry including non-inertial effects</title>
<abstract>Light-pulse atom interferometers rely on the wave nature of matter and its manipulation with coherent laser pulses. They are used for precise gravimetry and inertial sensing as well as for accurate measurements of fundamental constants. Reaching higher precision requires longer interferometer times which are naturally encountered in microgravity environments such as drop-tower facilities, sounding rockets and dedicated satellite missions aiming at fundamental quantum physics in space. In all those cases, it is necessary to consider arbitrary trajectories and varying orientations of the interferometer set-up in non-inertial frames of reference. Here we provide a versatile representation-free description of atom interferometry entirely based on operator algebra to address this general situation. We show how to analytically determine the phase shift as well as the visibility of interferometers with an arbitrary number of pulses including the effects of local gravitational accelerations, gravity gradients, the rotation of the lasers and non-inertial frames of reference. Our method conveniently unifies previous results and facilitates the investigation of novel interferometer geometries.</abstract>
<year>2015</year>
<issn>0370-1573</issn>
<DOI>https://doi.org/10.1016/j.physrep.2015.09.004</DOI>
<journal>Physics Reports</journal>
<volume>605</volume>
<pages>1 - 50</pages>
<keywords>Atom interferometry, Quantum optics</keywords>
<file_url>http://www.sciencedirect.com/science/article/pii/S0370157315003968</file_url>
<note>Representation-free description of light-pulse atom interferometry including non-inertial effects</note>
<authors>
<person>
<fn>S.</fn>
<sn>Kleinert</sn>
</person>
<person>
<fn>E.</fn>
<sn>Kajari</sn>
</person>
<person>
<fn>A.</fn>
<sn>Roura</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Shore_2015</citeid>
<title>Scattering of a particle with internal structure from a single slit</title>
<abstract>Classically, rigid objects with elongated shapes can fit through apertures only when properly aligned. Quantum-mechanical particles which have internal structure (e.g. a diatomic molecule) also are affected during attempts to pass through small apertures, but there are interesting differences with classical structured particles. We illustrate here some of these differences for ultra-slow particles. Notably, we predict resonances that correspond to prolonged delays of the rotor within the aperture—a trapping phenomenon not found classically.</abstract>
<year>2015</year>
<month>1</month>
<DOI>10.1088/1367-2630/17/1/013046</DOI>
<journal>New Journal of Physics</journal>
<volume>17</volume>
<publisher>{IOP} Publishing</publisher>
<pages>013046</pages>
<number>1</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F17%2F1%2F013046</file_url>
<authors>
<person>
<fn>B. W.</fn>
<sn>Shore</sn>
</person>
<person>
<fn>P.</fn>
<sn>Dömötör</sn>
</person>
<person>
<fn>E.</fn>
<sn>Sadurní</sn>
</person>
<person>
<fn>G.</fn>
<sn>Süßmann</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Roura_2014</citeid>
<title>Overcoming loss of contrast in atom interferometry due to gravity gradients</title>
<abstract>Long-time atom interferometry is instrumental to various high-precision measurements of fundamental physical properties, including tests of the equivalence principle. Due to rotations and gravity gradients, the classical trajectories characterizing the motion of the wave packets for the two branches of the interferometer do not close in phase space, an effect which increases significantly with the interferometer time. The relative displacement between the interfering wave packets in such open interferometers leads to a fringe pattern in the density profile at each exit port and a loss of contrast in the oscillations of the integrated particle number as a function of the phase shift. Paying particular attention to gravity gradients, we present a simple mitigation strategy involving small changes in the timing of the laser pulses which is very easy to implement. A useful representation-free description of the state evolution in an atom interferometer is introduced and employed to analyze the loss of contrast and mitigation strategy in the general case. (As a by-product, a remarkably compact derivation of the phase-shift in a general light-pulse atom interferometer is provided.) Furthermore, exact results are obtained for (pure and mixed) Gaussian states which allow a simple interpretation in terms of the alignment of Wigner functions in phase-space. Analytical results are also obtained for expanding Bose–Einstein condensates within the time-dependent Thomas–Fermi approximation. Finally, a combined strategy for rotations and nonaligned gravity gradients is considered as well.</abstract>
<year>2014</year>
<month>12</month>
<DOI>10.1088/1367-2630/16/12/123012</DOI>
<journal>New Journal of Physics</journal>
<volume>16</volume>
<publisher>{IOP} Publishing</publisher>
<pages>123012</pages>
<number>12</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F16%2F12%2F123012</file_url>
<authors>
<person>
<fn>A.</fn>
<sn>Roura</sn>
</person>
<person>
<fn>W.</fn>
<sn>Zeller</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Neuberger_2014</citeid>
<title>Newton flow of the Riemann zeta function: separatrices control the appearance of zeros</title>
<abstract>A great many phenomena in physics can be traced back to the zeros of a function or a functional. Eigenvalue or variational problems prevalent in classical as well as quantum mechanics are examples illustrating this statement. Continuous descent methods taken with respect to the proper metric are efficient ways to attack such problems. In particular, the continuous Newton method brings out the lines of constant phase of a complex-valued function. Although the patterns created by the Newton flow are reminiscent of the field lines of electrostatics and magnetostatics they cannot be realized in this way since in general they are not curl-free. We apply the continuous Newton method to the Riemann zeta function and discuss the emerging patterns emphasizing especially the structuring of the non-trivial zeros by the separatrices. This approach might open a new road toward the Riemann hypothesis.</abstract>
<year>2014</year>
<month>10</month>
<DOI>10.1088/1367-2630/16/10/103023</DOI>
<journal>New Journal of Physics</journal>
<volume>16</volume>
<publisher>{IOP} Publishing</publisher>
<pages>103023</pages>
<number>10</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F16%2F10%2F103023</file_url>
<authors>
<person>
<fn>J. W.</fn>
<sn>Neuberger</sn>
</person>
<person>
<fn>C.</fn>
<sn>Feiler</sn>
</person>
<person>
<fn>H.</fn>
<sn>Maier</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevLett.112.203002</citeid>
<title>Quantum Test of the Universality of Free Fall</title>
<year>2014</year>
<month>5</month>
<DOI>10.1103/PhysRevLett.112.203002</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>112</volume>
<publisher>American Physical Society</publisher>
<pages>203002</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.112.203002</file_url>
<authors>
<person>
<fn>D.</fn>
<sn>Schlippert</sn>
</person>
<person>
<fn>J.</fn>
<sn>Hartwig</sn>
</person>
<person>
<fn>H.</fn>
<sn>Albers</sn>
</person>
<person>
<fn>L. L.</fn>
<sn>Richardson</sn>
</person>
<person>
<fn>C.</fn>
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<abstract>The theory of general relativity describes macroscopic phenomena driven by the influence of gravity while quantum mechanics brilliantly accounts for microscopic effects. Despite their tremendous individual success, a complete unification of fundamental interactions is missing and remains one of the most challenging and important quests in modern theoretical physics. The spacetime explorer and quantum equivalence principle space test satellite mission, proposed as a medium-size mission within the Cosmic Vision program of the European Space Agency (ESA), aims for testing general relativity with high precision in two experiments by performing a measurement of the gravitational redshift of the Sun and the Moon by comparing terrestrial clocks, and by performing a test of the universality of free fall of matter waves in the gravitational field of Earth comparing the trajectory of two Bose–Einstein condensates of 85Rb and 87Rb. The two ultracold atom clouds are monitored very precisely thanks to techniques of atom interferometry. This allows to reach down to an uncertainty in the Eötvös parameter of at least 2 × 10−15. In this paper, we report about the results of the phase A mission study of the atom interferometer instrument covering the description of the main payload elements, the atomic source concept, and the systematic error sources.</abstract>
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<month>5</month>
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<volume>31</volume>
<publisher>{IOP} Publishing</publisher>
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<abstract>We propose a method to factor numbers based on the quantum dynamics of two interacting bosonic atoms where the single-particle energy spectrum depends logarithmically on the quantum number. We show that two atoms initially prepared in the ground state are preferentially excited by a time-dependent interaction into a two-particle energy state characterized by the factors. Hence, a measurement of the energy of one of the two atoms yields the factors. The number to be factored is encoded in the frequency of a sinusoidally modulated interaction. We also discuss the influence of off-resonant transitions and the limitation of the number to be factored imposed by experimental conditions.</abstract>
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<fn>T.</fn>
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<reference>
<bibtype>article</bibtype>
<citeid>Schleich_2013</citeid>
<title>A representation-free description of the Kasevich-Chu interferometer: a resolution of the redshift controversy</title>
<abstract>Motivated by a recent claim by Müller et al (2010 Nature
463 926–9) that an atom interferometer can serve as an atom clock to measure the gravitational redshift with an unprecedented accuracy, we provide a representation-free description of the Kasevich–Chu interferometer based on operator algebra. We use this framework to show that the operator product determining the number of atoms at the exit ports of the interferometer is a c-number phase factor whose phase is the sum of only two phases: one is due to the acceleration of the phases of the laser pulses and the other one is due to the acceleration of the atom. This formulation brings out most clearly that this interferometer is an accelerometer or a gravimeter. Moreover, we point out that in different representations of quantum mechanics such as the position or the momentum representation the phase shift appears as though it originates from different physical phenomena. Due to this representation dependence conclusions concerning an enhanced accuracy derived in a specific representation are unfounded.</abstract>
<year>2013</year>
<month>1</month>
<DOI>10.1088/1367-2630/15/1/013007</DOI>
<journal>New Journal of Physics</journal>
<volume>15</volume>
<publisher>{IOP} Publishing</publisher>
<pages>013007</pages>
<number>1</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F15%2F1%2F013007</file_url>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>D. M.</fn>
<sn>Greenberger</sn>
</person>
<person>
<fn>E. M.</fn>
<sn>Rasel</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1080/09500340.2012.746400</citeid>
<title>A two-photon double-slit experiment</title>
<year>2013</year>
<DOI>10.1080/09500340.2012.746400</DOI>
<journal>Journal of Modern Optics</journal>
<volume>60</volume>
<publisher>Taylor & Francis</publisher>
<pages>86-94</pages>
<number>1</number>
<authors>
<person>
<fn>R.</fn>
<sn>Menzel</sn>
</person>
<person>
<fn>A.</fn>
<sn>Heuer</sn>
</person>
<person>
<fn>D.</fn>
<sn>Puhlmann</sn>
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<person>
<fn>K.</fn>
<sn>Dechoum</sn>
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<person>
<fn>M.</fn>
<sn>Hillery</sn>
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<fn>M. J. A.</fn>
<sn>Spähn</sn>
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<fn>W. P.</fn>
<sn>Schleich</sn>
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<citeid>PhysRevA.87.013627</citeid>
<title>Berry phase in atom optics</title>
<year>2013</year>
<month>1</month>
<DOI>10.1103/PhysRevA.87.013627</DOI>
<journal>Phys. Rev. A</journal>
<volume>87</volume>
<publisher>American Physical Society</publisher>
<pages>013627</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.87.013627</file_url>
<authors>
<person>
<fn>P. V.</fn>
<sn>Mironova</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
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<fn>W. P.</fn>
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</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Kazemi_2013</citeid>
<title>Quantum carpets: a tool to observe decoherence</title>
<abstract>Quantum carpets—the spatio-temporal de Broglie density profiles—woven by an atom or an electron in the near-field region of a diffraction grating bring to light, in real time, the decoherence of each individual component of the interference term of the Wigner function characteristic of superposition states. The proposed experiments are feasible with present-day technology.</abstract>
<year>2013</year>
<month>1</month>
<DOI>10.1088/1367-2630/15/1/013052</DOI>
<journal>New Journal of Physics</journal>
<volume>15</volume>
<publisher>{IOP} Publishing</publisher>
<pages>013052</pages>
<number>1</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F15%2F1%2F013052</file_url>
<authors>
<person>
<fn>P.</fn>
<sn>Kazemi</sn>
</person>
<person>
<fn>S.</fn>
<sn>Chaturvedi</sn>
</person>
<person>
<fn>I.</fn>
<sn>Marzoli</sn>
</person>
<person>
<fn>R. F.</fn>
<sn>O'Connell</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.87.014102</citeid>
<title>Reconstruction of Bohm trajectories and wave functions from interferometric measurements</title>
<year>2013</year>
<month>1</month>
<DOI>10.1103/PhysRevA.87.014102</DOI>
<journal>Phys. Rev. A</journal>
<volume>87</volume>
<publisher>American Physical Society</publisher>
<pages>014102</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.87.014102</file_url>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>M. S.</fn>
<sn>Zubairy</sn>
</person>
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</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevLett.110.010401</citeid>
<title>Redshift Controversy in Atom Interferometry: Representation Dependence of the Origin of Phase Shift</title>
<year>2013</year>
<month>1</month>
<DOI>10.1103/PhysRevLett.110.010401</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>110</volume>
<publisher>American Physical Society</publisher>
<pages>010401</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.110.010401</file_url>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>D. M.</fn>
<sn>Greenberger</sn>
</person>
<person>
<fn>E. M.</fn>
<sn>Rasel</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Schleich5374</citeid>
<title>Schrödinger equation revisited</title>
<abstract>The time-dependent Schrödinger equation is a cornerstone of quantum physics and governs all phenomena of the microscopic world. However, despite its importance, its origin is still not widely appreciated and properly understood. We obtain the Schrödinger equation from a mathematical identity by a slight generalization of the formulation of classical statistical mechanics based on the Hamilton{\textendash}Jacobi equation. This approach brings out most clearly the fact that the linearity of quantum mechanics is intimately connected to the strong coupling between the amplitude and phase of a quantum wave.</abstract>
<year>2013</year>
<issn>0027-8424</issn>
<DOI>10.1073/pnas.1302475110</DOI>
<journal>Proceedings of the National Academy of Sciences</journal>
<volume>110</volume>
<publisher>National Academy of Sciences</publisher>
<pages>5374--5379</pages>
<number>14</number>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>D. M.</fn>
<sn>Greenberger</sn>
</person>
<person>
<fn>D. H.</fn>
<sn>Kobe</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
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<reference>
<bibtype>inproceedings</bibtype>
<title>Theory of the quantum FEL in a nutshell</title>
<year>2013</year>
<journal>Proceedings of FEL 2013, Nara, Japan</journal>
<publisher>JACoW</publisher>
<editor>T. Tanaka and V. R. W. Schaa</editor>
<authors>
<person>
<fn>P.</fn>
<sn>Preiss</sn>
</person>
<person>
<fn>R.</fn>
<sn>Sauerbrey</sn>
</person>
<person>
<fn>M. S.</fn>
<sn>Zubairy</sn>
</person>
<person>
<fn>R.</fn>
<sn>Endrich</sn>
</person>
<person>
<fn>E.</fn>
<sn>Giese</sn>
</person>
<person>
<fn>P.</fn>
<sn>Kling</sn>
</person>
<person>
<fn>M.</fn>
<sn>Knobl</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>HEIM20131822</citeid>
<title>Tunneling of an energy eigenstate through a parabolic barrier viewed from Wigner phase space</title>
<abstract>We analyze the tunneling of a particle through a repulsive potential resulting from an inverted harmonic oscillator in the quantum mechanical phase space described by the Wigner function. In particular, we solve the partial differential equations in phase space determining the Wigner function of an energy eigenstate of the inverted oscillator. The reflection or transmission coefficients R or T are then given by the total weight of all classical phase-space trajectories corresponding to energies below, or above the top of the barrier given by the Wigner function.</abstract>
<year>2013</year>
<issn>0375-9601</issn>
<DOI>10.1016/j.physleta.2013.05.017</DOI>
<journal>Physics Letters A</journal>
<volume>377</volume>
<pages>1822 - 1825</pages>
<number>31</number>
<keywords>Tunneling, Inverted oscillator, Wigner function</keywords>
<file_url>http://www.sciencedirect.com/science/article/pii/S0375960113004878</file_url>
<authors>
<person>
<fn>D. M.</fn>
<sn>Heim</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>P. M.</fn>
<sn>Alsing</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
<person>
<fn>S.</fn>
<sn>Varro</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Buser_2013</citeid>
<title>Visualization of the Gödel universe</title>
<abstract>The standard model of modern cosmology, which is based on the Friedmann–Lemaître–Robertson–Walker metric, allows the definition of an absolute time. However, there exist (cosmological) models consistent with the theory of general relativity for which such a definition cannot be given since they offer the possibility for time travel. The simplest of these models is the cosmological solution discovered by Kurt Gödel, which describes a homogeneous, rotating universe. Disregarding the paradoxes that come along with the abolishment of causality in such space–times, we are interested in the purely academic question of how an observer would visually perceive the time travel of an object in Gödel's universe. For this purpose, we employ the technique of ray tracing, a standard tool in computer graphics, and visualize various scenarios to bring out the optical effects experienced by an observer located in this universe. In this way, we provide a new perspective on the space–time structure of Gödel's model.</abstract>
<year>2013</year>
<month>1</month>
<DOI>10.1088/1367-2630/15/1/013063</DOI>
<journal>New Journal of Physics</journal>
<volume>15</volume>
<publisher>{IOP} Publishing</publisher>
<pages>013063</pages>
<number>1</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F15%2F1%2F013063</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Buser</sn>
</person>
<person>
<fn>E.</fn>
<sn>Kajari</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Case:12</citeid>
<title>A diffractive mechanism of focusing</title>
<abstract>We examine the free time evolution of a rectangular one dimensional Schr\"{o}dinger wave packet of constant phase during the early stage which in the paraxial wave approximation is identical to the diffraction of a scalar field from a single slit. Our analysis, based on numerics and the Cornu spiral reveals considerable intricate detail behavior in the density and phase of the wave. We also point out a concentration of the intensity that occurs on axis and propose a new measure of width that expresses this concentration.</abstract>
<year>2012</year>
<month>12</month>
<DOI>10.1364/OE.20.027253</DOI>
<journal>Opt. Express</journal>
<volume>20</volume>
<publisher>OSA</publisher>
<pages>27253--27262</pages>
<number>25</number>
<keywords>Diffraction; Diffraction theory; Diffraction limit; Evanescent waves; Light fields; Phase space analysis methods; Ptychography; Talbot effect</keywords>
<file_url>http://www.opticsexpress.org/abstract.cfm?URI=oe-20-25-27253</file_url>
<authors>
<person>
<fn>W. B.</fn>
<sn>Case</sn>
</person>
<person>
<fn>E.</fn>
<sn>Sadurní</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.86.063622</citeid>
<title>Relativistic effects in atom and neutron interferometry and the differences between them</title>
<year>2012</year>
<month>12</month>
<DOI>10.1103/PhysRevA.86.063622</DOI>
<journal>Phys. Rev. A</journal>
<volume>86</volume>
<publisher>American Physical Society</publisher>
<pages>063622</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.86.063622</file_url>
<authors>
<person>
<fn>D. M.</fn>
<sn>Greenberger</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>E. M.</fn>
<sn>Rasel</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Plimak_2012</citeid>
<title>Operator ordering and causality</title>
<abstract>A formal implementation of the concepts of mesoscopic electromagnetic interaction and of the propagating wave in quantum electrodynamics beyond the rotating wave approximation is discussed. Used as a guide, these concepts lead to a natural resolution of a long-standing controversy: causality violations in the Glauber–Kelley–Kleiner photodetection theory. The Glauber–Kelley–Kleiner definition of the time-normal operator ordering must be amended without the rotating wave approximation, which eliminates all causality problems.</abstract>
<year>2012</year>
<month>2</month>
<DOI>10.1088/0031-8949/2012/t147/014026</DOI>
<journal>Physica Scripta</journal>
<volume>T147</volume>
<publisher>{IOP} Publishing</publisher>
<pages>014026</pages>
<file_url>https://doi.org/10.1088%2F0031-8949%2F2012%2Ft147%2F014026</file_url>
<authors>
<person>
<fn>L. I.</fn>
<sn>Plimak</sn>
</person>
<person>
<fn>S. T.</fn>
<sn>Stenholm</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>W_lk_2012</citeid>
<title>Factorization of numbers with Gauss sums: III. Algorithms with entanglement</title>
<abstract>We propose two algorithms to factor numbers using Gauss sums and entanglement: (i) in a Shor-like algorithm we encode the standard Gauss sum in one of two entangled states and (ii) in an interference algorithm we create a superposition of Gauss sums in the probability amplitudes of two entangled states. These schemes are rather efficient provided that there exists a fast algorithm that can detect a period of a function hidden in its zeros.</abstract>
<year>2012</year>
<month>1</month>
<DOI>10.1088/1367-2630/14/1/013049</DOI>
<journal>New Journal of Physics</journal>
<volume>14</volume>
<publisher>{IOP} Publishing</publisher>
<pages>013049</pages>
<number>1</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F14%2F1%2F013049</file_url>
<authors>
<person>
<fn>S.</fn>
<sn>Wölk</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Tamma2012</citeid>
<title>Prime Number Decomposition, the Hyperbolic Function and Multi-Path Michelson Interferometers</title>
<abstract>The phase $\phi$ of any wave is determined by the ratio x/$\lambda$ consisting of the distance x propagated by the wave and its wavelength $\lambda$. Hence, the dependence of $\phi$ on $\lambda$ constitutes an analogue system for the mathematical operation of division, that is to obtain the hyperbolic function f($\xi$)≡1/$\xi$. We take advantage of this observation to decompose integers into primes and implement this approach towards factorization of numbers in a multi-path Michelson interferometer. This work is part of a larger program geared towards unraveling the connections between quantum mechanics and number theory. We briefly summarize this aspect.</abstract>
<year>2012</year>
<month>1</month>
<day>01</day>
<issn>1572-9516</issn>
<DOI>10.1007/s10701-010-9522-3</DOI>
<journal>Foundations of Physics</journal>
<volume>42</volume>
<pages>111--121</pages>
<number>1</number>
<file_url>https://doi.org/10.1007/s10701-010-9522-3</file_url>
<authors>
<person>
<fn>V.</fn>
<sn>Tamma</sn>
</person>
<person>
<fn>C. O.</fn>
<sn>Alley</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>Y. H.</fn>
<sn>Shih</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<citeid>Woelk2012</citeid>
<title>Quantum Carpets: Factorization with Degeneracies</title>
<abstract>In this paper, we connect our approach of factoring numbers using the continuous truncated Gauss sum (W{"o}lk et al., J. Mod. Optic, 2009) with the phenomenon of quantum carpets. In particular, we demonstrate that the degree of degeneracy of the ratio ℓ ∕ N translates into a crossing of the canals and ridges contained in the design of quantum carpets. In this way, quantum carpets represent an experimental implementation of our idea of factorization with degeneracies.</abstract>
<year>2012</year>
<isbn>978-1-4419-6624-7</isbn>
<DOI>10.1007/978-1-4419-6624-7_18</DOI>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>L. Cohen, H. V. Poor and M. O. Scully</editor>
<pages>259--269</pages>
<file_url>https://doi.org/10.1007/978-1-4419-6624-7_18</file_url>
<authors>
<person>
<fn>S.</fn>
<sn>Wölk</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Menzel9314</citeid>
<title>Wave-particle dualism and complementarity unraveled by a different mode</title>
<abstract>The precise knowledge of one of two complementary experimental outcomes prevents us from obtaining complete information about the other one. This formulation of Niels Bohr{\textquoteright}s principle of complementarity when applied to the paradigm of wave-particle dualism{\textemdash}that is, to Young{\textquoteright}s double-slit experiment{\textemdash}implies that the information about the slit through which a quantum particle has passed erases interference. In the present paper we report a double-slit experiment using two photons created by spontaneous parametric down-conversion where we observe interference in the signal photon despite the fact that we have located it in one of the slits due to its entanglement with the idler photon. This surprising aspect of complementarity comes to light by our special choice of the TEM01 pump mode. According to quantum field theory the signal photon is then in a coherent superposition of two distinct wave vectors giving rise to interference fringes analogous to two mechanical slits.</abstract>
<year>2012</year>
<issn>0027-8424</issn>
<DOI>10.1073/pnas.1201271109</DOI>
<journal>Proceedings of the National Academy of Sciences</journal>
<volume>109</volume>
<publisher>National Academy of Sciences</publisher>
<pages>9314--9319</pages>
<number>24</number>
<authors>
<person>
<fn>R.</fn>
<sn>Menzel</sn>
</person>
<person>
<fn>D.</fn>
<sn>Puhlmann</sn>
</person>
<person>
<fn>A.</fn>
<sn>Heuer</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Sorrentino_2011</citeid>
<title>The Space Atom Interferometer project: status and prospects</title>
<abstract>This paper presents the current status and future prospects of the Space Atom Interferometer project (SAI), funded by the European Space Agency. Atom interferometry provides extremely sensitive and accurate tools for the measurement of inertial forces. Operation of atom interferometers in microgravity is expected to enhance the performance of such sensors. Main goal of SAI is to demonstrate the possibility of placing atom interferometers in space. The resulting drop-tower compatible atom interferometry acceleration sensor prototype is described. Expected performance limits and potential scientific applications in a micro-gravity environment are also discussed.</abstract>
<year>2011</year>
<month>12</month>
<DOI>10.1088/1742-6596/327/1/012050</DOI>
<journal>Journal of Physics: Conference Series</journal>
<volume>327</volume>
<publisher>{IOP} Publishing</publisher>
<pages>012050</pages>
<file_url>https://doi.org/10.1088%2F1742-6596%2F327%2F1%2F012050</file_url>
<authors>
<person>
<fn>F.</fn>
<sn>Sorrentino</sn>
</person>
<person>
<fn>K.</fn>
<sn>Bongs</sn>
</person>
<person>
<fn>P.</fn>
<sn>Bouyer</sn>
</person>
<person>
<fn>L.</fn>
<sn>Cacciapuoti</sn>
</person>
<person>
<fn>M.</fn>
<sn>Angelis</sn>
</person>
<person>
<fn>H.</fn>
<sn>Dittus</sn>
</person>
<person>
<fn>W.</fn>
<sn>Ertmer</sn>
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<person>
<fn>J.</fn>
<sn>Hartwig</sn>
</person>
<person>
<fn>M.</fn>
<sn>Hauth</sn>
</person>
<person>
<fn>S.</fn>
<sn>Herrmann</sn>
</person>
<person>
<fn>K.</fn>
<sn>Huang</sn>
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<fn>M.</fn>
<sn>Inguscio</sn>
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<person>
<fn>E.</fn>
<sn>Kajari</sn>
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<fn>T.</fn>
<sn>Könemann</sn>
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<fn>C.</fn>
<sn>Lämmerzahl</sn>
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<person>
<fn>A.</fn>
<sn>Landragin</sn>
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<fn>G.</fn>
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<sn>Santos</sn>
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<fn>M.</fn>
<sn>Prevedelli</sn>
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<fn>E. M.</fn>
<sn>Rasel</sn>
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<fn>W. P.</fn>
<sn>Schleich</sn>
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<person>
<fn>M.</fn>
<sn>Schmidt</sn>
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<person>
<fn>A.</fn>
<sn>Senger</sn>
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<person>
<fn>K.</fn>
<sn>Sengstock</sn>
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<fn>G.</fn>
<sn>Stern</sn>
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<fn>G. M.</fn>
<sn>Tino</sn>
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<sn>Valenzuela</sn>
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<fn>R.</fn>
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<fn>P.</fn>
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<reference>
<bibtype>article</bibtype>
<citeid>W_lk_2011</citeid>
<title>Factorization of numbers with Gauss sums: I. Mathematical background</title>
<abstract>We use the periodicity properties of generalized Gauss sums to factor numbers. Moreover, we derive rules for finding the factors and illustrate this factorization scheme for various examples. This algorithm relies solely on interference and scales exponentially.</abstract>
<year>2011</year>
<month>10</month>
<DOI>10.1088/1367-2630/13/10/103007</DOI>
<journal>New Journal of Physics</journal>
<volume>13</volume>
<publisher>{IOP} Publishing</publisher>
<pages>103007</pages>
<number>10</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F13%2F10%2F103007</file_url>
<authors>
<person>
<fn>S.</fn>
<sn>Wölk</sn>
</person>
<person>
<fn>W.</fn>
<sn>Merkel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>I. Sh.</fn>
<sn>Averbukh</sn>
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<person>
<fn>B.</fn>
<sn>Girard</sn>
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<reference>
<bibtype>article</bibtype>
<citeid>Merkel_2011</citeid>
<title>Factorization of numbers with Gauss sums: II. Suggestions for implementation with chirped laser pulses</title>
<abstract>We propose three implementations of the Gauss sum factorization schemes discussed in part I of this series (Wölk et al 2011 New J. Phys. 13 103007): (i) a two-photon transition in a multi-level ladder system induced by a chirped laser pulse, (ii) a chirped one-photon transition in a two-level atom with a periodically modulated excited state and (iii) a linearly chirped one-photon transition driven by a sequence of ultrashort pulses. For each of these quantum systems, we show that the excitation probability amplitude is given by an appropriate Gauss sum. We provide rules on how to encode the number N to be factored in our system and how to identify the factors of N in the fluorescence signal of the excited state.</abstract>
<year>2011</year>
<month>10</month>
<DOI>10.1088/1367-2630/13/10/103008</DOI>
<journal>New Journal of Physics</journal>
<volume>13</volume>
<publisher>{IOP} Publishing</publisher>
<pages>103008</pages>
<number>10</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F13%2F10%2F103008</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Merkel</sn>
</person>
<person>
<fn>S.</fn>
<sn>Wölk</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>I. Sh.</fn>
<sn>Averbukh</sn>
</person>
<person>
<fn>B.</fn>
<sn>Girard</sn>
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<person>
<fn>G. G.</fn>
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<reference>
<bibtype>article</bibtype>
<citeid>Rudolph2011</citeid>
<title>Degenerate Quantum Gases in Microgravity</title>
<abstract>Clouds of ultra-cold atoms and especially Bose--Einstein condensates (BEC) provide a source for coherent matter-waves in numerous earth bound experiments. Analogous to optical interferometry, matter-wave interferometers can be used for precision measurements allowing for a sensitivity orders of magnitude above their optical counterparts. However, in some respects the presence of gravitational forces in the lab limits experimental possibilities. In this article, we report about a compact and robust experiment generating Bose--Einstein condensates in the drop tower facility in Bremen, Germany. We also present the progress of building the succeeding experiment in which a two species atom interferometer will be implemented to test the weak equivalence principle with quantum matter.</abstract>
<year>2011</year>
<month>6</month>
<day>01</day>
<issn>1875-0494</issn>
<DOI>10.1007/s12217-010-9247-0</DOI>
<journal>Microgravity Science and Technology</journal>
<volume>23</volume>
<pages>287--292</pages>
<number>3</number>
<file_url>https://doi.org/10.1007/s12217-010-9247-0</file_url>
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<fn>W.</fn>
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<citeid>PhysRevA.83.051602</citeid>
<title>Quantum-noise quenching in atomic tweezers</title>
<year>2011</year>
<month>5</month>
<DOI>10.1103/PhysRevA.83.051602</DOI>
<journal>Phys. Rev. A</journal>
<volume>83</volume>
<publisher>American Physical Society</publisher>
<pages>051602</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.83.051602</file_url>
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<fn>S.</fn>
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<fn>B.</fn>
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<reference>
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<citeid>PhysRevA.83.020304</citeid>
<title>Factoring numbers with a single interferogram</title>
<year>2011</year>
<month>2</month>
<DOI>10.1103/PhysRevA.83.020304</DOI>
<journal>Phys. Rev. A</journal>
<volume>83</volume>
<publisher>American Physical Society</publisher>
<pages>020304</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.83.020304</file_url>
<authors>
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<fn>V.</fn>
<sn>Tamma</sn>
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<fn>X.</fn>
<sn>He</sn>
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<fn>A.</fn>
<sn>Garuccio</sn>
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<fn>W. P.</fn>
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<fn>Y.</fn>
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<reference>
<bibtype>inproceedings</bibtype>
<citeid>Wolk:11</citeid>
<title>Quantum Mechanics Meets Number Theory</title>
<abstract>We suggest a way to determine the Riemann zeta function with the help of quantum mechanics. Furthermore, we discuss the factoring abilities of Gauss sums and introduce a way to calculate them with the help of entanglement.</abstract>
<year>2011</year>
<DOI>10.1364/ICQI.2011.QMC1</DOI>
<booktitle>International Conference on Quantum Information</booktitle>
<journal>International Conference on Quantum Information</journal>
<publisher>Optical Society of America</publisher>
<pages>QMC1</pages>
<keywords>Quantum optics; Quantum information and processing ; Beam splitters; Bose Einstein condensates; Cavity quantum electrodynamics; Cold atoms; Destructive interference; Quantum electronics</keywords>
<file_url>http://www.osapublishing.org/abstract.cfm?URI=ICQI-2011-QMC1</file_url>
<authors>
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<fn>S.</fn>
<sn>Wölk</sn>
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<person>
<fn>C.</fn>
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<reference>
<bibtype>article</bibtype>
<citeid>Sorrentino2010</citeid>
<title>A Compact Atom Interferometer for Future Space Missions</title>
<abstract>Atom interferometry represents a quantum leap in the technology for the ultra-precise monitoring of accelerations and rotations and, therefore, for the science that relies on these quantities. These sensors evolved from a new kind of optics based on matter-waves rather than light-waves and might result in an advancement of the fundamental detection limits by several orders of magnitude. This paper describes the current status of the Space Atom Interferometer project (SAI), funded by the European Space Agency. In a multi-pronged approach, SAI aims to investigate both experimentally and theoretically the various aspects of placing atom interferometers in space: the equipment needs, the realistically expected performance limits and potential scientific applications in a micro-gravity environment considering all aspects of quantum, relativistic and metrological sciences. A drop-tower compatible atom interferometry acceleration sensor prototype has been designed, and the manufacturing of its subsystems has been started. A compact modular laser system for cooling and trapping rubidium atoms has been assembled. A compact Raman laser module, featuring outstandingly low phase noise, has been realized. Possible schemes to implement coherent atomic sources in the atom interferometer have been experimentally demonstrated.</abstract>
<year>2010</year>
<month>10</month>
<day>01</day>
<issn>1875-0494</issn>
<DOI>10.1007/s12217-010-9240-7</DOI>
<journal>Microgravity Science and Technology</journal>
<volume>22</volume>
<pages>551--561</pages>
<number>4</number>
<file_url>https://doi.org/10.1007/s12217-010-9240-7</file_url>
<authors>
<person>
<fn>F.</fn>
<sn>Sorrentino</sn>
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<fn>K.</fn>
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<fn>C.</fn>
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<citeid>Glauber_2010</citeid>
<title>Field fluctuations measured by interferometry</title>
<abstract>We derive the complete photon count statistics of an interferometer based on two beam splitters. As a special case we consider a joint intensity–electric field measurement. Our approach is based on the transformation properties of state vectors as well as field operators at a beam splitter.</abstract>
<year>2010</year>
<month>9</month>
<DOI>10.1088/0031-8949/2010/t140/014002</DOI>
<journal>Physica Scripta</journal>
<volume>T140</volume>
<publisher>{IOP} Publishing</publisher>
<pages>014002</pages>
<file_url>https://doi.org/10.1088%2F0031-8949%2F2010%2Ft140%2F014002</file_url>
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<person>
<fn>R. J.</fn>
<sn>Glauber</sn>
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<fn>L. A.</fn>
<sn>Orozco</sn>
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<fn>K.</fn>
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<citeid>PhysRevA.82.032119</citeid>
<title>Riemann ζ function from wave-packet dynamics</title>
<year>2010</year>
<month>9</month>
<DOI>10.1103/PhysRevA.82.032119</DOI>
<journal>Phys. Rev. A</journal>
<volume>82</volume>
<publisher>American Physical Society</publisher>
<pages>032119</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.82.032119</file_url>
<authors>
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<fn>R.</fn>
<sn>Mack</sn>
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<fn>J. P.</fn>
<sn>Dahl</sn>
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<bibtype>article</bibtype>
<citeid>Kajari2010</citeid>
<title>Inertial and gravitational mass in quantum mechanics</title>
<abstract>We show that in complete agreement with classical mechanics, the dynamics of any quantum mechanical wave packet in a linear gravitational potential involves the gravitational and the inertial mass only as their ratio. In contrast, the spatial modulation of the corresponding energy wave function is determined by the third root of the product of the two masses. Moreover, the discrete energy spectrum of a particle constrained in its motion by a linear gravitational potential and an infinitely steep wall depends on the inertial as well as the gravitational mass with different fractional powers. This feature might open a new avenue in quantum tests of the universality of free fall.</abstract>
<year>2010</year>
<month>7</month>
<day>01</day>
<issn>1432-0649</issn>
<DOI>10.1007/s00340-010-4085-8</DOI>
<journal>Applied Physics B</journal>
<volume>100</volume>
<pages>43--60</pages>
<number>1</number>
<file_url>https://doi.org/10.1007/s00340-010-4085-8</file_url>
<authors>
<person>
<fn>E.</fn>
<sn>Kajari</sn>
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<person>
<fn>N. L.</fn>
<sn>Harshman</sn>
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<person>
<fn>E. M.</fn>
<sn>Rasel</sn>
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<fn>S.</fn>
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<person>
<fn>G.</fn>
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<reference>
<bibtype>article</bibtype>
<citeid>Schmidt_Kaler_2010</citeid>
<title>Focus on Atom Optics and its Applications</title>
<abstract>Atom optics employs the modern techniques of quantum optics and laser cooling to enable applications which often outperform current standard technologies. Atomic matter wave interferometers allow for ultra-precise sensors; metrology and clocks are pushed to an extraordinary accuracy of 17 digits using single atoms. Miniaturization and integration are driven forward for both atomic clocks and atom optical circuits. With the miniaturization of information-storage and -processing devices, the scale of single atoms is approached in solid state devices, where the laws of quantum physics lead to novel, advantageous features and functionalities. An upcoming branch of atom optics is the control of single atoms, potentially allowing solid state devices to be built atom by atom; some of which would be applicable in future quantum information processing devices. Selective manipulation of individual atoms also enables trace analysis of extremely rare isotopes. Additionally, sources of neutral atoms with high brightness are being developed and, if combined with photo ionization, even novel focused ion beam sources are within reach. Ultracold chemistry is fertilized by atomic techniques, when reactions of chemical constituents are investigated between ions, atoms, molecules, trapped or aligned in designed fields and cooled to ultra-low temperatures such that the reaction kinetics can be studied in a completely state-resolved manner.
Focus on Atom Optics and its Applications Contents
Sensitive gravity-gradiometry with atom interferometry: progress towards an improved determination of the gravitational constant
F Sorrentino, Y-H Lien, G Rosi, L Cacciapuoti, M Prevedelli and G M Tino
A single-atom detector integrated on an atom chip: fabrication, characterization and application
D Heine, W Rohringer, D Fischer, M Wilzbach, T Raub, S Loziczky, XiYuan Liu, S Groth, B Hessmo and J Schmiedmayer
Interaction of a propagating guided matter wave with a localized potential
G L Gattobigio, A Couvert, B Georgeot and D Guéry-Odelin
Analysis of the entanglement between two individual atoms using global Raman rotations
A Gaëtan, C Evellin, J Wolters, P Grangier, T Wilk and A Browaeys
Spin polarization transfer in ground and metastable helium atom collisions
D Vrinceanu and H R Sadeghpour
A fiber Fabry–Perot cavity with high finesse
D Hunger, T Steinmetz, Y Colombe, C Deutsch, T W Hänsch and J Reichel
Atomic wave packets in amplitude-modulated vertical optical lattices
A Alberti, G Ferrari, V V Ivanov, M L Chiofalo and G M Tino
Atom interferometry with trapped Bose–Einstein condensates: impact of atom–atom interactions
Julian Grond, Ulrich Hohenester, Igor Mazets and Jörg Schmiedmayer
Storage of protonated water clusters in a biplanar multipole rf trap
C Greve, M Kröner, S Trippel, P Woias, R Wester and M Weidemüller
Single-atom detection on a chip: from realization to application
A Stibor, H Bender, S Kühnhold, J Fortágh, C Zimmermann and A Günther
Ultracold atoms as a target: absolute scattering cross-section measurements
P Würtz, T Gericke, A Vogler and H Ott
Entanglement-assisted atomic clock beyond the projection noise limit
Anne Louchet-Chauvet, Jürgen Appel, Jelmer J Renema, Daniel Oblak, Niels Kjaergaard and Eugene S Polzik
Towards the realization of atom trap trace analysis for 39Ar
J Welte, F Ritterbusch, I Steinke, M Henrich, W Aeschbach-Hertig and M K Oberthaler
Resonant superfluidity in an optical lattice
I Titvinidze, M Snoek and W Hofstetter
Interference of interacting matter waves
Mattias Gustavsson, Elmar Haller, Manfred J Mark, Johann G Danzl, Russell Hart, Andrew J Daley and Hanns-Christoph Nägerl
Magnetic trapping of NH molecules with 20 s lifetimes
E Tsikata, W C Campbell, M T Hummon, H-I Lu and J M Doyle
Imprinting patterns of neutral atoms in an optical lattice using magnetic resonance techniques
Michal Karski, Leonid Förster, Jai-Min Choi, Andreas Steffen, Noomen Belmechri, Wolfgang Alt, Dieter Meschede and Artur Widera
Frequency stability of optical lattice clocks
Jérôme Lodewyck, Philip G Westergaard, Arnaud Lecallier, Luca Lorini and Pierre Lemonde
Ultracold quantum gases in triangular optical lattices
C Becker, P Soltan-Panahi, J Kronjäger, S Dörscher, K Bongs and K Sengstock
Cold atoms near superconductors: atomic spin coherence beyond the Johnson noise limit
B Kasch, H Hattermann, D Cano, T E Judd, S Scheel, C Zimmermann, R Kleiner, D Koelle and J Fortágh
Focusing a deterministic single-ion beam
Wolfgang Schnitzler, Georg Jacob, Robert Fickler, Ferdinand Schmidt-Kaler and Kilian Singer
Tuning the structural and dynamical properties of a dipolar Bose–Einstein condensate: ripples and instability islands
M Asad-uz-Zaman and D Blume
Double-resonance lineshapes in a cell with wall coating and buffer gas
Svenja Knappe and Hugh G Robinson
Transport and interaction blockade of cold bosonic atoms in a triple-well potential
P Schlagheck, F Malet, J C Cremon and S M Reimann
Fabrication of a planar micro Penning trap and numerical investigations of versatile ion positioning protocols
M Hellwig, A Bautista-Salvador, K Singer, G Werth and F Schmidt-Kaler
Laser cooling of a magnetically guided ultracold atom beam
A Aghajani-Talesh, M Falkenau, V V Volchkov, L E Trafford, T Pfau and A Griesmaier
Creation efficiency of nitrogen-vacancy centres in diamond
S Pezzagna, B Naydenov, F Jelezko, J Wrachtrup and J Meijer
Top-down pathways to devices with few and single atoms placed to high precision
Jessica A Van Donkelaar, Andrew D Greentree, Andrew D C Alves, Lenneke M Jong, Lloyd C L Hollenberg and David N Jamieson
Enhanced electric field sensitivity of rf-dressed Rydberg dark states
M G Bason, M Tanasittikosol, A Sargsyan, A K Mohapatra, D Sarkisyan, R M Potvliege and C S Adams</abstract>
<year>2010</year>
<month>6</month>
<DOI>10.1088/1367-2630/12/6/065014</DOI>
<journal>New Journal of Physics</journal>
<volume>12</volume>
<publisher>{IOP} Publishing</publisher>
<pages>065014</pages>
<number>6</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F12%2F6%2F065014</file_url>
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<citeid>PhysRevB.81.054514</citeid>
<title>Coherent superpositions of single semifluxon states in a 0−π Josephson junction</title>
<year>2010</year>
<month>2</month>
<DOI>10.1103/PhysRevB.81.054514</DOI>
<journal>Phys. Rev. B</journal>
<volume>81</volume>
<publisher>American Physical Society</publisher>
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<title>Bose-Einstein Condensation in Microgravity</title>
<abstract>Two pillars of modern physics are quantum mechanics and general relativity. So far, both have remained apart with no quantum mechanical description of gravity available. Van Zoest et al. (p. 1540; see the Perspective by Nussenzveig and Barata) present work with a macroscopic quantum mechanical system{\textemdash}a Bose-Einstein condensate (BEC) of rubidium atoms in which the cloud of atoms is cooled into a collective quantum state{\textemdash}in microgravity. By dropping the BEC down a 146-meter-long drop chamber and monitoring the expansion of the quantum gas under these microgravity conditions, the authors provide a proof-of-principle demonstration of a technique that can probe the boundary of quantum mechanics and general relativity and perhaps offer the opportunity to reconcile the two experimentally.Albert Einstein{\textquoteright}s insight that it is impossible to distinguish a local experiment in a {\textquotedblleft}freely falling elevator{\textquotedblright} from one in free space led to the development of the theory of general relativity. The wave nature of matter manifests itself in a striking way in Bose-Einstein condensates, where millions of atoms lose their identity and can be described by a single macroscopic wave function. We combine these two topics and report the preparation and observation of a Bose-Einstein condensate during free fall in a 146-meter-tall evacuated drop tower. During the expansion over 1 second, the atoms form a giant coherent matter wave that is delocalized on a millimeter scale, which represents a promising source for matter-wave interferometry to test the universality of free fall with quantum matter.</abstract>
<year>2010</year>
<issn>0036-8075</issn>
<DOI>10.1126/science.1189164</DOI>
<journal>Science</journal>
<volume>328</volume>
<publisher>American Association for the Advancement of Science</publisher>
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<title>Conformal mapping and bound states in bent waveguides</title>
<year>2010</year>
<DOI>10.1063/1.3537857</DOI>
<journal>AIP Conference Proceedings</journal>
<volume>1323</volume>
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<number>1</number>
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<fn>E.</fn>
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<citeid>doi:10.1080/09500340.2010.486873</citeid>
<title>Correlations in phase space and the creation of focusing wave packets</title>
<year>2010</year>
<DOI>10.1080/09500340.2010.486873</DOI>
<journal>Journal of Modern Optics</journal>
<volume>57</volume>
<publisher>Taylor & Francis</publisher>
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<person>
<fn>R.</fn>
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<citeid>VOGEL2010133</citeid>
<title>Optimally focusing wave packets</title>
<abstract>An appropriately prepared real-valued wave packet moving in one space dimension will focus during a brief period of time even in the absence of any force. We illustrate this phenomenon by considering the time evolution of the elementary superposition of the ground state and the second excited state of a harmonic oscillator. Moreover, we show that a variation of the superposition parameter leads us from a domain of enhanced spreading via a point of suppressed spreading to a region where the wave packets focuses before it spreads again. We determine the points of maximal spreading and optimal focusing. Our analysis of this unusual behavior of a free quantum particle rests on the time dependence of (i) the average separation of the wave packet from the origin, (ii) the probability density in position space, and (iii) the Wigner phase space distribution. We conclude our search for optimally focusing wave packets by solving the corresponding variational problem with respect to a family of measures expressing the width of the wave packet.</abstract>
<year>2010</year>
<issn>0301-0104</issn>
<DOI>https://doi.org/10.1016/j.chemphys.2010.07.002</DOI>
<journal>Chemical Physics</journal>
<volume>375</volume>
<pages>133 - 143</pages>
<number>2</number>
<keywords>Focusing wave packets, Wigner function</keywords>
<file_url>http://www.sciencedirect.com/science/article/pii/S0301010410003137</file_url>
<note>Stochastic processes in Physics and Chemistry (in honor of Peter Hänggi)</note>
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<fn>K.</fn>
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<citeid>SCHLEICH2010786</citeid>
<title>Wigner function for a free particle in two dimensions: A tale of interference</title>
<abstract>The familiar wave function for a free particle in two dimensions and in a state with definite values of energy and angular momentum shows some unusual effects. We identify the origin of these subtleties as interference in two-dimensional space where Huygens’ principle breaks down. Our arguments are based upon the corresponding Wigner function.</abstract>
<year>2010</year>
<issn>0030-4018</issn>
<DOI>https://doi.org/10.1016/j.optcom.2009.10.055</DOI>
<journal>Optics Communications</journal>
<volume>283</volume>
<pages>786 - 789</pages>
<number>5</number>
<file_url>http://www.sciencedirect.com/science/article/pii/S0030401809010475</file_url>
<note>Quo vadis Quantum Optics?</note>
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<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
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<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
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<citeid>Feiler2009</citeid>
<title>New Frontiers at the Interface of General Relativity and Quantum Optics</title>
<abstract>In the present paper we follow three major themes: (i) concepts of rotation in general relativity, (ii) effects induced by these generalized rotations, and (iii) their measurement using interferometry. Our journey takes us from the Foucault pendulum via the Sagnac interferometer to manifestations of gravito-magnetism in double binary pulsars and in G{"o}del's Universe. Throughout our article we emphasize the emerging role of matter wave interferometry based on cold atoms or Bose--Einstein condensates leading to superior inertial sensors. In particular, we advertise recent activities directed towards the operation of a coherent matter wave interferometer in an extended free fall.</abstract>
<year>2009</year>
<month>12</month>
<day>01</day>
<issn>1572-9672</issn>
<DOI>10.1007/s11214-009-9613-7</DOI>
<journal>Space Science Reviews</journal>
<volume>148</volume>
<pages>123--147</pages>
<number>1</number>
<file_url>https://doi.org/10.1007/s11214-009-9613-7</file_url>
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<fn>C.</fn>
<sn>Feiler</sn>
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<fn>M.</fn>
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<citeid>PhysRevD.80.103002</citeid>
<title>The Gödel universe: Exact geometrical optics and analytical investigations on motion</title>
<year>2009</year>
<month>11</month>
<DOI>10.1103/PhysRevD.80.103002</DOI>
<journal>Phys. Rev. D</journal>
<volume>80</volume>
<publisher>American Physical Society</publisher>
<pages>103002</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevD.80.103002</file_url>
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<citeid>PhysRevB.80.134515</citeid>
<title>Theory of fractional vortex escape in a long Josephson junction</title>
<year>2009</year>
<month>10</month>
<DOI>10.1103/PhysRevB.80.134515</DOI>
<journal>Phys. Rev. B</journal>
<volume>80</volume>
<publisher>American Physical Society</publisher>
<pages>134515</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevB.80.134515</file_url>
<authors>
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<fn>K.</fn>
<sn>Vogel</sn>
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<citeid>PhysRevA.80.033624</citeid>
<title>Commuting Heisenberg operators as the quantum response problem: Time-normal averages in the truncated Wigner representation</title>
<year>2009</year>
<month>9</month>
<DOI>10.1103/PhysRevA.80.033624</DOI>
<journal>Phys. Rev. A</journal>
<volume>80</volume>
<publisher>American Physical Society</publisher>
<pages>033624</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.80.033624</file_url>
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<fn>B.</fn>
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<citeid>PhysRevA.80.022714</citeid>
<title>Efimov states in atom-molecule collisions</title>
<year>2009</year>
<month>8</month>
<DOI>10.1103/PhysRevA.80.022714</DOI>
<journal>Phys. Rev. A</journal>
<volume>80</volume>
<publisher>American Physical Society</publisher>
<pages>022714</pages>
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<fn>M. A.</fn>
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<bibtype>article</bibtype>
<citeid>Ertmer2009</citeid>
<title>Matter wave explorer of gravity (MWXG)</title>
<abstract>In response to ESA's Call for proposals of 5 March 2007 of the COSMIC VISION 2015--2025 plan of the ESA science programme, we propose a M-class satellite mission to test of the Equivalence Principle in the quantum domain by investigating the extended free fall of matter waves instead of macroscopic bodies as in the case of GAUGE, MICROSCOPE or STEP. The satellite, called Matter Wave Explorer of Gravity, will carry an experiment to test gravity, namely the measurement of the equal rate of free fall with various isotopes of distinct atomic species with precision cold atom interferometry in the vicinity of the earth. This will allow for a first quantum test the Equivalence Principle with spin polarised particles and with pure fermionic and bosonic atomic ensembles. Due to the space conditions, the free fall of Rubidium and Potassium isotopes will be compared with a maximum accelerational sensitivity of 5{\textperiodcentered}10{\thinspace}−{\thinspace}16 m/s2 corresponding to an accuracy of the test of the Equivalence Principle of 1 part in 1016. Besides the primary scientific goal, the quantum test of the Equivalence Principle, the mission can be extended to provide additional information about the gravitational field of the earth or for testing theories of fundamental processes of decoherence which are investigated by various theory groups in the context of quantum gravity phenomenology. In this proposal we present in detail the mission objectives and the technical aspects of the proposed mission.</abstract>
<year>2009</year>
<month>3</month>
<day>01</day>
<issn>1572-9508</issn>
<DOI>10.1007/s10686-008-9125-6</DOI>
<journal>Experimental Astronomy</journal>
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<file_url>https://doi.org/10.1007/s10686-008-9125-6</file_url>
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<title>State operator, constants of the motion, and Wigner functions: The two-dimensional isotropic harmonic oscillator</title>
<year>2009</year>
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<title>The granularity of weakly occupied bosonic fields beyond the local density approximation</title>
<abstract>We examine ground state correlations for repulsive, quasi one-dimensional bosons in a harmonic trap. In particular, we focus on the few particle limit N=2, 3, 4, …, where exact numerical solutions of the many particle Schrödinger equation are available, by employing the multi-configuration time-dependent Hartree method. Our numerical results for the inhomogeneous system are modeled with the analytical solution of the homogeneous problem using the Bethe ansatz and the local density approximation. Tuning the interaction strength from the weakly correlated Gross–Pitaevskii to the strongly correlated Tonks–Girardeau regime reveals finite particle number effects in the second-order correlation function beyond the local density approximation.</abstract>
<year>2009</year>
<month>2</month>
<DOI>10.1088/1367-2630/11/2/023010</DOI>
<journal>New Journal of Physics</journal>
<volume>11</volume>
<publisher>{IOP} Publishing</publisher>
<pages>023010</pages>
<number>2</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F11%2F2%2F023010</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Eckart</sn>
</person>
<person>
<fn>R.</fn>
<sn>Walser</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>S.</fn>
<sn>Zöllner</sn>
</person>
<person>
<fn>P.</fn>
<sn>Schmelcher</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<title>Factorization</title>
<year>2009</year>
<booktitle>Mathematical Analysis of Evolution, Information, and Complexity</booktitle>
<publisher>Wiley VCH</publisher>
<address>Weinheim</address>
<editor>W. Arendt and W. Schleich</editor>
<pages>395-431</pages>
<authors>
<person>
<fn>R.</fn>
<sn>Mack</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>D.</fn>
<sn>Haase</sn>
</person>
<person>
<fn>H.</fn>
<sn>Maier</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1080/09500340903194625</citeid>
<title>Factorization of numbers with truncated Gauss sums at rational arguments</title>
<year>2009</year>
<DOI>10.1080/09500340903194625</DOI>
<journal>Journal of Modern Optics</journal>
<volume>56</volume>
<publisher>Taylor & Francis</publisher>
<pages>2118-2124</pages>
<number>18-19</number>
<authors>
<person>
<fn>S.</fn>
<sn>Wölk</sn>
</person>
<person>
<fn>C.</fn>
<sn>Feiler</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>In memoriam of Jürgen Ehlers</title>
<year>2009</year>
<booktitle>Atom Optics and Space Physics</booktitle>
<journal>Proceedings of the International School of Physics "Enrico Fermi"</journal>
<publisher>IOS Press</publisher>
<address>Amsterdam, Oxford, Tokyo, Washington DC</address>
<editor>E. Arimondo, W. Ertmer, E. M. Rasel, and W. P. Schleich</editor>
<pages>IX-XI</pages>
<authors>
<person>
<fn>E.</fn>
<sn>Arimondo</sn>
</person>
<person>
<fn>W.</fn>
<sn>Ertmer</sn>
</person>
<person>
<fn>E. M.</fn>
<sn>Rasel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>Preface</title>
<year>2009</year>
<booktitle>Atom Optics and Space Physics</booktitle>
<journal>Proceedings of the International School of Physics "Enrico Fermi"</journal>
<publisher>IOS Press</publisher>
<address>Amsterdam, Oxford, Tokyo, Washington DC</address>
<editor>E. Arimondo, W. Ertmer, E.M. Rasel and W.P. Schleich</editor>
<pages>XXIII-XVI</pages>
<authors>
<person>
<fn>E.</fn>
<sn>Arimondo</sn>
</person>
<person>
<fn>W.</fn>
<sn>Ertmer</sn>
</person>
<person>
<fn>E. M.</fn>
<sn>Rasel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<title>Preface</title>
<year>2009</year>
<booktitle>Mathematical Analysis of Evolution, Information, and Complexity</booktitle>
<publisher>Wiley VCH</publisher>
<address>Weinheim</address>
<editor>W. Arendt and W. Schleich</editor>
<pages>XXIII-XXIX</pages>
<authors>
<person>
<fn>W.</fn>
<sn>Arendt</sn>
</person>
<person>
<fn>D.</fn>
<sn>Mugnolo</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>Rotation in Relativity and the Propagation of Light</title>
<year>2009</year>
<booktitle>Atom Optics and Space Physics</booktitle>
<journal>Proceedings of the International School of Physics "Enrico Fermi"</journal>
<publisher>IOS Press</publisher>
<address>Amsterdam, Oxford, Tokyo, Washington DC</address>
<editor>E. Arimondo, W. Ertmer, E. M. Rasel, and W. P. Schleich</editor>
<pages>45-148</pages>
<authors>
<person>
<fn>E.</fn>
<sn>Kajari</sn>
</person>
<person>
<fn>M.</fn>
<sn>Buser</sn>
</person>
<person>
<fn>C.</fn>
<sn>Feiler</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Theoretical Femtosecond Physics</title>
<year>2009</year>
<journal>Physik Journal</journal>
<volume>8</volume>
<pages>53</pages>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>_tefa_k_2008</citeid>
<title>Factorization with exponential sums</title>
<abstract>We generalize the concept of factorization using truncated Gauss sums to exponential sums where the phase increases with the jth power of the summation index. For such sums the number of terms needed to suppress ghost factors of N scales as . Unfortunately, this advantageous scaling law is accompanied by a disadvantage: the gap between factors and non-factors decreases rapidly with increasing power j and as a consequence it gets more difficult to identify factors. This feature serves as our motivation to study sums with an exponential phase. Our numerical simulations indicate that in this case the scaling law is logarithmic and that we retain a significant gap between factors and non-factors.</abstract>
<year>2008</year>
<month>7</month>
<DOI>10.1088/1751-8113/41/30/304024</DOI>
<journal>Journal of Physics A: Mathematical and Theoretical</journal>
<volume>41</volume>
<publisher>{IOP} Publishing</publisher>
<pages>304024</pages>
<number>30</number>
<file_url>https://doi.org/10.1088%2F1751-8113%2F41%2F30%2F304024</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Štefaňák</sn>
</person>
<person>
<fn>D.</fn>
<sn>Haase</sn>
</person>
<person>
<fn>W.</fn>
<sn>Merkel</sn>
</person>
<person>
<fn>M. S.</fn>
<sn>Zubairy</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Eckart_2008</citeid>
<title>Exploring the growth of correlations in a quasi one-dimensional trapped Bose gas</title>
<abstract>Phase correlations, density fluctuations and three-body loss rates are relevant for many experiments in quasi one-dimensional geometries. Extended mean-field theory is used to evaluate correlation functions up to third order for a quasi one-dimensional trapped Bose gas at zero and finite temperature. At zero temperature and in the homogeneous limit, we also study the transition from the weakly correlated Gross–Pitaevskii regime to the strongly correlated Tonks–Girardeau regime analytically. We compare our results with the exact Lieb–Liniger solution for the homogeneous case and find good agreement up to the cross-over regime.</abstract>
<year>2008</year>
<month>4</month>
<DOI>10.1088/1367-2630/10/4/045024</DOI>
<journal>New Journal of Physics</journal>
<volume>10</volume>
<publisher>{IOP} Publishing</publisher>
<pages>045024</pages>
<number>4</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F10%2F4%2F045024</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Eckart</sn>
</person>
<person>
<fn>R.</fn>
<sn>Walser</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Walser_2008</citeid>
<title>Semifluxons in superconductivity and cold atomic gases</title>
<abstract>Josephson junctions (JJs) and junction arrays are well-studied devices in superconductivity. With external magnetic fields one can modulate the phase in a long junction and create traveling, solitonic waves of magnetic flux, called fluxons. Today, it is also possible to devise two different types of junctions: depending on the sign of the critical current density , they are called 0- or π-junctions. In turn, a 0–π junction is formed by joining two of these junctions. As a result, one obtains a pinned Josephson vortex of fractional magnetic flux, at the 0–π boundary. Here, we analyze this arrangement of superconducting junctions in the context of an atomic bosonic quantum gas, where two-state atoms in a double well trap are coupled in an analogous fashion. There, an all-optical 0–π JJ is created by the phase of a complex valued Rabi frequency and we derive a discrete four-mode model for this situation, which qualitatively resembles a semifluxon.</abstract>
<year>2008</year>
<month>4</month>
<DOI>10.1088/1367-2630/10/4/045020</DOI>
<journal>New Journal of Physics</journal>
<volume>10</volume>
<publisher>{IOP} Publishing</publisher>
<pages>045020</pages>
<number>4</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F10%2F4%2F045020</file_url>
<authors>
<person>
<fn>R.</fn>
<sn>Walser</sn>
</person>
<person>
<fn>E.</fn>
<sn>Goldobin</sn>
</person>
<person>
<fn>O.</fn>
<sn>Crasser</sn>
</person>
<person>
<fn>D.</fn>
<sn>Koelle</sn>
</person>
<person>
<fn>R.</fn>
<sn>Kleiner</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevLett.100.030202</citeid>
<title>Factorization of Numbers with the Temporal Talbot Effect: Optical Implementation by a Sequence of Shaped Ultrashort Pulses</title>
<year>2008</year>
<month>1</month>
<DOI>10.1103/PhysRevLett.100.030202</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>100</volume>
<publisher>American Physical Society</publisher>
<pages>030202</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.100.030202</file_url>
<authors>
<person>
<fn>D.</fn>
<sn>Bigourd</sn>
</person>
<person>
<fn>B.</fn>
<sn>Chatel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>B.</fn>
<sn>Girard</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Fraktionale Flussquanten, Steuerbare "Atome" im Supraleiter</title>
<year>2008</year>
<booktitle>Themenheft Forschung</booktitle>
<journal>Quantenmaterie</journal>
<volume>5</volume>
<publisher>Universität Stuttgart</publisher>
<pages>22-31</pages>
<authors>
<person>
<fn>E.</fn>
<sn>Goldobin</sn>
</person>
<person>
<fn>R.</fn>
<sn>Kleiner</sn>
</person>
<person>
<fn>D.</fn>
<sn>Kölle</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>R.</fn>
<sn>Walser</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevLett.100.030201</citeid>
<title>Gauss Sum Factorization with Cold Atoms</title>
<year>2008</year>
<month>1</month>
<DOI>10.1103/PhysRevLett.100.030201</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>100</volume>
<publisher>American Physical Society</publisher>
<pages>030201</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.100.030201</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Gilowski</sn>
</person>
<person>
<fn>T.</fn>
<sn>Wendrich</sn>
</person>
<person>
<fn>T.</fn>
<sn>Müller</sn>
</person>
<person>
<fn>Ch.</fn>
<sn>Jentsch</sn>
</person>
<person>
<fn>W.</fn>
<sn>Ertmer</sn>
</person>
<person>
<fn>E. M.</fn>
<sn>Rasel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Nachruf auf Willis Eugene Lamb</title>
<year>2008</year>
<journal>Physik Journal</journal>
<volume>7</volume>
<pages>127</pages>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>NMR implementation of exponential sums for integer factorization</title>
<year>2008</year>
<journal>Contemporary Physics: Proceedings of the International Symposium , National Centre for Physics Islamabad, Pakistan 26-30 March 2007</journal>
<publisher>World Scientific</publisher>
<address>Singapore</address>
<editor>J. Aslam, F. Hussain and Riazuddin</editor>
<pages>87-94</pages>
<authors>
<person>
<fn>M.</fn>
<sn>Štefaňák</sn>
</person>
<person>
<fn>W.</fn>
<sn>Merkel</sn>
</person>
<person>
<fn>M.</fn>
<sn>Mehring</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>incollection</bibtype>
<title>Publikationsverhalten in der Physik</title>
<year>2008</year>
<booktitle>Publikationsverhalten in unterschiedlichen Disziplinen, Beiträge zur Beurteilung von Forschungsleistungen</booktitle>
<volume>12</volume>
<series>Diskussionspapiere der Alexander von Humboldt-Stiftung</series>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1002/prop.200810535</citeid>
<title>Quantum carpets of a slightly relativistic particle</title>
<abstract>Abstract We analyze the structures emerging in the spacetime representation of the probability density woven by a slightly relativistic particle caught in a one-dimensional box. In particular, we evaluate the relativistic effects on the revival time and the specific changes produced in the intermode traces, which quantum carpets consist of. Moreover, we present a detailed mathematical analysis of such quantum carpets pursuing the approach of a kernel. Here we represent the probability distribution as a superposition of interfering Airy function-type structures along straight world lines. We also show that this phenomenon can be enhanced by many orders of magnitude in semiconductors with narrow band-gap (e.g. as in InSb) and small effective mass of the electron, whereby due to the strong nonparabolicity of the semiconductor conduction band, the electron energy vs momentum dispersion relation behaves in a pseudo-relativistic way.</abstract>
<year>2008</year>
<DOI>10.1002/prop.200810535</DOI>
<journal>Fortschritte der Physik</journal>
<volume>56</volume>
<pages>967-992</pages>
<number>10</number>
<keywords>wave packets, one-dimensional box, Talbot effect, Green function</keywords>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/prop.200810535</file_url>
<authors>
<person>
<fn>I.</fn>
<sn>Marzoli</sn>
</person>
<person>
<fn>A. E.</fn>
<sn>Kaplan</sn>
</person>
<person>
<fn>F.</fn>
<sn>Saif</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Zum Gedenken an John Archibald Wheeler</title>
<year>2008</year>
<journal>Physik Journal</journal>
<volume>7</volume>
<pages>126</pages>
<authors>
<person>
<fn>H.</fn>
<sn>Pfister</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Koenemann2007</citeid>
<title>A freely falling magneto-optical trap drop tower experiment</title>
<abstract>We experimentally demonstrate the possibility of preparing ultracold atoms in the environment of weightlessness at the earth-bound short-term microgravity laboratory Drop Tower Bremen, a facility of ZARM -- University of Bremen. Our approach is based on a freely falling magneto-optical trap (MOT) drop tower experiment performed within the ATKAT collaboration (``Atom-Catapult'') as a preliminary part of the QUANTUS pilot project (``Quantum Systems in Weightlessness'') pursuing a Bose--Einstein condensate (BEC) in microgravity at the drop tower [1, 2].</abstract>
<year>2007</year>
<month>12</month>
<day>01</day>
<issn>1432-0649</issn>
<DOI>10.1007/s00340-007-2863-8</DOI>
<journal>Applied Physics B</journal>
<volume>89</volume>
<pages>431--438</pages>
<number>4</number>
<file_url>https://doi.org/10.1007/s00340-007-2863-8</file_url>
<authors>
<person>
<fn>T.</fn>
<sn>Könemann</sn>
</person>
<person>
<fn>W.</fn>
<sn>Brinkmann</sn>
</person>
<person>
<fn>E.</fn>
<sn>Göklü</sn>
</person>
<person>
<fn>C.</fn>
<sn>Lämmerzahl</sn>
</person>
<person>
<fn>H.</fn>
<sn>Dittus</sn>
</person>
<person>
<fn>T.</fn>
<sn>Zoest</sn>
</person>
<person>
<fn>E. M.</fn>
<sn>Rasel</sn>
</person>
<person>
<fn>W.</fn>
<sn>Ertmer</sn>
</person>
<person>
<fn>W.</fn>
<sn>Lewoczko-Adamczyk</sn>
</person>
<person>
<fn>M.</fn>
<sn>Schiemangk</sn>
</person>
<person>
<fn>A.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>G.</fn>
<sn>Johannsen</sn>
</person>
<person>
<fn>S.</fn>
<sn>Wildfang</sn>
</person>
<person>
<fn>K.</fn>
<sn>Bongs</sn>
</person>
<person>
<fn>K.</fn>
<sn>Sengstock</sn>
</person>
<person>
<fn>E.</fn>
<sn>Kajari</sn>
</person>
<person>
<fn>G.</fn>
<sn>Nandi</sn>
</person>
<person>
<fn>R.</fn>
<sn>Walser</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.76.063617</citeid>
<title>Dropping cold quantum gases on Earth over long times and large distances</title>
<year>2007</year>
<month>12</month>
<DOI>10.1103/PhysRevA.76.063617</DOI>
<journal>Phys. Rev. A</journal>
<volume>76</volume>
<publisher>American Physical Society</publisher>
<pages>063617</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.76.063617</file_url>
<authors>
<person>
<fn>G.</fn>
<sn>Nandi</sn>
</person>
<person>
<fn>R.</fn>
<sn>Walser</sn>
</person>
<person>
<fn>E.</fn>
<sn>Kajari</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>_tefa_k_2007</citeid>
<title>Factorization with Gauss sums: scaling properties of ghost factors</title>
<abstract>Recent experiments have shown that truncated Gauss sums allow us to find the factors of an integer N. This method relies on the fact that for a factor the absolute value of the Gauss sum is unity. However, for every integer N there exist integers which are not factors, but where the Gauss sum reaches a value which is arbitrarily close to unity. In order to distinguish such ghost factors from real factors we need to amplify this difference. We show that a proper choice of the truncation parameter of the Gauss sum suppresses the ghost factors below a threshold value. We derive the scaling law of the truncation parameter on the number to be factored. Moreover, we show that this scaling law is also necessary for the success of our factorization scheme, even if we relax the threshold or allow limited error tolerance.</abstract>
<year>2007</year>
<month>10</month>
<DOI>10.1088/1367-2630/9/10/370</DOI>
<journal>New Journal of Physics</journal>
<volume>9</volume>
<publisher>{IOP} Publishing</publisher>
<pages>370--370</pages>
<number>10</number>
<file_url>https://doi.org/10.1088%2F1367-2630%2F9%2F10%2F370</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Štefaňák</sn>
</person>
<person>
<fn>W.</fn>
<sn>Merkel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>D.</fn>
<sn>Haase</sn>
</person>
<person>
<fn>H.</fn>
<sn>Maier</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.76.023417</citeid>
<title>Chirping a two-photon transition in a multistate ladder</title>
<year>2007</year>
<month>8</month>
<DOI>10.1103/PhysRevA.76.023417</DOI>
<journal>Phys. Rev. A</journal>
<volume>76</volume>
<publisher>American Physical Society</publisher>
<pages>023417</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.76.023417</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Merkel</sn>
</person>
<person>
<fn>H.</fn>
<sn>Mack</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>G. G.</fn>
<sn>Paulus</sn>
</person>
<person>
<fn>B.</fn>
<sn>Girard</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Grupp_2007</citeid>
<title>Resonant Feshbach scattering of fermions in one-dimensional optical lattices</title>
<abstract>We consider Feshbach scattering of fermions in a one-dimensional optical lattice. By formulating the scattering theory in the crystal momentum basis, one can exploit the lattice symmetry and factorize the scattering problem in terms of centre-of-mass and relative momentum in the reduced Brillouin zone scheme. Within a single-band approximation, we can tune the position of a Feshbach resonance with the centre-of-mass momentum due to the non-parabolic form of the energy band.</abstract>
<year>2007</year>
<month>6</month>
<DOI>10.1088/0953-4075/40/13/014</DOI>
<journal>Journal of Physics B: Atomic, Molecular and Optical Physics</journal>
<volume>40</volume>
<publisher>{IOP} Publishing</publisher>
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<number>13</number>
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<abstract>Abstract The results on non-spreading Michelangelo wave packets [7, 8] are generalized to the case of a semi-open two-level system when some fraction of atoms falls back to the lower state due to spontaneous transitions. The proposed approach is based on the solution of the Generalized Optical Bloch Equations for the atomic density matrix. The spatial features of arising nonspreading wave packets as well as the atomic momentum distribution are compared with the case of an open two-level system. (© 2006 by Astro, Ltd. Published exclusively by WILEY-VCH Verlag GmbH \& Co. KGaA)</abstract>
<year>2006</year>
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<number>1</number>
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<title>Factorization of numbers with physical systems</title>
<abstract>Abstract The periodicity properties of Gauss sums allow us to factor integer numbers. We show that the excitation probability amplitudes of appropriate quantum systems interacting with specific laser fields are determined by Gauss sums. The resulting probabilities are experimentally accessible by measuring the fluorescence from this level. In particular, we discuss a two-photon transition in a ladder system driven by a chirped laser pulse. In addition, we consider two realizations of laser driven one-photon transitions. For each quantum system we demonstrate the power of this factorization scheme using numerical examples.</abstract>
<year>2006</year>
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<journal>Fortschritte der Physik</journal>
<volume>54</volume>
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<number>8‐10</number>
<keywords>Gauss sums, chirped pulses, factorization of numbers</keywords>
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<title>Quantized Field Effects</title>
<abstract>The electromagnetic field appears almost everywhere in physics. Following the introduction of Maxwell's equations in 1864, Max Planck initiated quantum theory when he discovered h{\thinspace}={\thinspace}2$\pi$ℏ in the laws of black-body radiation. In 1905 Albert Einstein explained the photoelectric effect on the hypothesis of a corpuscular nature of radiation and in 1917 this paradigm led to a description of the interaction between atoms and electromagnetic radiation.</abstract>
<year>2006</year>
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<publisher>Springer</publisher>
<address>New York, NY</address>
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<title>Quantum dynamics of atomic coherence in a spin-1 condensate: Mean-field versus many-body simulation</title>
<abstract>We analyse and numerically simulate the full many-body quantum dynamics of a spin-1 condensate in the single spatial mode approximation. Initially, the condensate is in a “ferromagnetic” state with all spins aligned along the y axis and the magnetic field pointing along the z axis. In the course of evolution the spinor condensate undergoes a characteristic change of symmetry, which in a real experiment could be a signature of spin-mixing many-body interactions. The results of our simulations are conveniently visualised within the picture of irreducible tensor operators.</abstract>
<year>2006</year>
<issn>0030-4018</issn>
<DOI>https://doi.org/10.1016/j.optcom.2006.03.074</DOI>
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<DOI>10.1007/978-3-540-47008-3_2</DOI>
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<title>Observation of Nonspreading Wave Packets in an Imaginary Potential</title>
<year>2005</year>
<month>9</month>
<DOI>10.1103/PhysRevLett.95.110405</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>95</volume>
<publisher>American Physical Society</publisher>
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<title>Formation of two-dimensional nonspreading atomic wave packets in the field of two standing light waves</title>
<abstract>The formation of two-dimensional nonspreading atomic wave packets produced in the interaction of a beam of two-level atoms with two standing light waves polarised in the same plane is considered. The mechanism providing a dispersionless particle dynamics is the balance of two processes: a rapid decay of the atomic wave function away from the field nodes due to spontaneous transitions to nonresonance states and the quantum broadening of the wave packets formed in the close vicinity of field nodes. Coordinate-dependent amplitudes and phases of the two-dimensional wave packets were found for the jg=0 ↔ je=1 transition.</abstract>
<year>2005</year>
<month>8</month>
<DOI>10.1070/qe2005v035n08abeh009145</DOI>
<journal>Quantum Electronics</journal>
<volume>35</volume>
<publisher>{IOP} Publishing</publisher>
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<citeid>PhysRevB.72.054527</citeid>
<title>Quantum tunneling of semifluxons in a 0-π-0 long Josephson junction</title>
<year>2005</year>
<month>8</month>
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<journal>Phys. Rev. B</journal>
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<title>Extracting atoms on demand with lasers</title>
<year>2005</year>
<month>5</month>
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<journal>Phys. Rev. A</journal>
<volume>71</volume>
<publisher>American Physical Society</publisher>
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<title>Motional stability of the quantum kicked rotor: A fidelity approach</title>
<year>2005</year>
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<year>2005</year>
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<title>Sagnac Effect of Gödel's Universe</title>
<abstract>We present exact expressions for the Sagnac effect of G{"o}del's Universe. For this purpose we first derive a formula for the Sagnac time delay along a circular path in the presence of an arbitrary stationary metric in cylindrical coordinates. We then apply this result to G{"o}del's metric for two different experimental situations: First, the light source and the detector are at rest relative to the matter generating the gravitational field. In this case we find an expression that is formally equivalent to the familiar nonrelativistic Sagnac time delay. Second, the light source and the detector are rotating relative to the matter. Here we show that for a special rotation rate of the detector the Sagnac time delay vanishes. Finally we propose a formulation of the Sagnac time delay in terms of invariant physical quantities. We show that this result is very close to the analogous formula of the Sagnac time delay of a rotating coordinate system in Minkowski spacetime.</abstract>
<year>2004</year>
<month>10</month>
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<citeid>Fedorov2003</citeid>
<title>Dynamics of spontaneous radiation of atoms scattered by a resonance standing light wave</title>
<abstract>The scattering of atoms by a resonance standing light wave is considered under conditions when the lower of two resonance levels is metastable, while the upper level rapidly decays due to mainly spontaneous radiative transitions to the nonresonance levels of an atom. The diffraction scattering regime is studied, when the Rabi frequency is sufficiently high and many diffraction maxima are formed due to scattering. The dynamics of spontaneous radiation of an atom is investigated. It is shown that scattering slows down substantially the radiative decay of the atom. The regions and characteristics of the power and exponential decay are determined. The adiabatic and nonadiabatic scattering regimes are studied. It is shown that the wave packets of atoms in the metastable and resonance excited states narrow down during scattering. A limiting (minimal) size of the wave packets is found, which is achieved upon nonadiabatic scattering in the case of a sufficiently long interaction time.</abstract>
<year>2003</year>
<month>9</month>
<day>01</day>
<issn>1090-6509</issn>
<DOI>10.1134/1.1618338</DOI>
<journal>Journal of Experimental and Theoretical Physics</journal>
<volume>97</volume>
<pages>522--538</pages>
<number>3</number>
<file_url>https://doi.org/10.1134/1.1618338</file_url>
<authors>
<person>
<fn>M. V.</fn>
<sn>Fedorov</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
</person>
<person>
<fn>V. P.</fn>
<sn>Yakovlev</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
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<citeid>PhysRevLett.91.010401</citeid>
<title>Fresnel Representation of the Wigner Function: An Operational Approach</title>
<year>2003</year>
<month>6</month>
<DOI>10.1103/PhysRevLett.91.010401</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>91</volume>
<publisher>American Physical Society</publisher>
<pages>010401</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.91.010401</file_url>
<authors>
<person>
<fn>P.</fn>
<sn>Lougovski</sn>
</person>
<person>
<fn>E.</fn>
<sn>Solano</sn>
</person>
<person>
<fn>Z. M.</fn>
<sn>Zhang</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
<person>
<fn>H.</fn>
<sn>Mack</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Botero2003</citeid>
<title>Geometry, commutation relations and the quantum fictitious force</title>
<abstract>We express the commutation relation between the operators of the momentum and the radial unit vectors in D dimensions in differential and integral form. We connect this commutator with the quantum fictitious potential emerging in the radial Schr{"o}dinger equation of an s-wave.</abstract>
<year>2003</year>
<month>2</month>
<day>01</day>
<issn>1432-0649</issn>
<DOI>10.1007/s00340-003-1113-y</DOI>
<journal>Applied Physics B</journal>
<volume>76</volume>
<pages>129--133</pages>
<number>2</number>
<file_url>https://doi.org/10.1007/s00340-003-1113-y</file_url>
<authors>
<person>
<fn>J.</fn>
<sn>Botero</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Cirone</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
<person>
<fn>F.</fn>
<sn>Straub</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>article</citeid>
<title>A Photon Viewed from Wigner Phase Space</title>
<year>2003</year>
<DOI>10.1201/9781420044256.ch5</DOI>
<journal>Optics and Photonics News</journal>
<volume>14</volume>
<pages>28-35</pages>
<authors>
<person>
<fn>H.</fn>
<sn>Mack</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1002/prop.200310007</citeid>
<title>An elementary aspect of the Weyl-Wigner representation</title>
<abstract>Abstract It is an elementary aspect of the Weyl-Wigner representation of quantum mechanics that the dynamical phase-space function corresponding to the square of a quantum-mechanical operator is, in general, different from the square of the function representing the operator itself. We call attention to some conceptual consequences of this fact.</abstract>
<year>2003</year>
<DOI>10.1002/prop.200310007</DOI>
<journal>Fortschritte der Physik</journal>
<volume>51</volume>
<pages>85-91</pages>
<number>2‐3</number>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/prop.200310007</file_url>
<authors>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<title>Dynamical Suppression of Radiative Decay via Atomic Deflection by a Standing Light Wave</title>
<year>2003</year>
<journal>Laser Physics</journal>
<volume>13</volume>
<pages>995-1003</pages>
<number>7</number>
<authors>
<person>
<fn>M. A.</fn>
<sn>Efremov</sn>
</person>
<person>
<fn>M.</fn>
<sn>Fedorov</sn>
</person>
<person>
<fn>V. P.</fn>
<sn>Yakovlev</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
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<reference>
<bibtype>inbook</bibtype>
<citeid>doi:10.1142/9789812704634_0039</citeid>
<title>Entanglement, Kinetic Energy and the Quantum Fictitious Potential</title>
<abstract>We discuss the average kinetic energy of N non-interacting quantum particles in its dependence on N. For a peculiar entangled state, the kinetic energy increases quadratically with N, in contrast to its behavior in simple thermodynamics.</abstract>
<year>2003</year>
<DOI>10.1142/9789812704634_0039</DOI>
<booktitle>The Physics of Communication</booktitle>
<journal>Proceedings of XXII Solvay Conference on Physics</journal>
<publisher>World Scientific</publisher>
<address>Singapore</address>
<editor>I. Antoniou, V. A. Sadovnichy and H. Walther</editor>
<pages>568-575</pages>
<authors>
<person>
<fn>J.</fn>
<sn>Botero</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Cirone</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
<person>
<fn>A.</fn>
<sn>Delgado</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1002/prop.200310065</citeid>
<title>Kicked rotor in Wigner phase space</title>
<abstract>Abstract We develop the Wigner phase space representation of a kicked particle for an arbitrary but periodic kicking potential. We use this formalism to illustrate quantum resonances and anti-resonances.</abstract>
<year>2003</year>
<DOI>10.1002/prop.200310065</DOI>
<journal>Fortschritte der Physik</journal>
<volume>51</volume>
<pages>474-486</pages>
<number>4‐5</number>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/prop.200310065</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Bienert</sn>
</person>
<person>
<fn>F.</fn>
<sn>Haug</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. G.</fn>
<sn>Raizen</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<title>Volles Engagement für die Universität Ulm, Emeritiert: Wolfgang Witschel</title>
<year>2003</year>
<journal>uni ulm intern, Das Ulmer Universitätsmagazin</journal>
<volume>261</volume>
<pages>25-27</pages>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Bia_lslash_ynicki_Birula_2002</citeid>
<title>Attractive and repulsive quantum forces from dimensionality of space</title>
<abstract>Two particles of identical mass attract and repel each other even when there exist
no classical external forces and their average relative momentum vanishes. This
quantum force depends crucially on the number of dimensions of space.</abstract>
<year>2002</year>
<month>8</month>
<DOI>10.1088/1464-4266/4/4/326</DOI>
<journal>Journal of Optics B: Quantum and Semiclassical Optics</journal>
<volume>4</volume>
<publisher>{IOP} Publishing</publisher>
<pages>S393--S396</pages>
<number>4</number>
<file_url>https://doi.org/10.1088%2F1464-4266%2F4%2F4%2F326</file_url>
<authors>
<person>
<fn>I.</fn>
<sn>Białynicki-Birula</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Cirone</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
<person>
<fn>R. F.</fn>
<sn>O'Connell</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevLett.89.060404</citeid>
<title>In- and Outbound Spreading of a Free-Particle s-Wave</title>
<year>2002</year>
<month>7</month>
<DOI>10.1103/PhysRevLett.89.060404</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>89</volume>
<publisher>American Physical Society</publisher>
<pages>060404</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.89.060404</file_url>
<authors>
<person>
<fn>I.</fn>
<sn>Białynicki-Birula</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Cirone</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
<person>
<fn>M.</fn>
<sn>Fedorov</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevLett.89.050403</citeid>
<title>State Reconstruction of the Kicked Rotor</title>
<year>2002</year>
<month>7</month>
<DOI>10.1103/PhysRevLett.89.050403</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>89</volume>
<publisher>American Physical Society</publisher>
<pages>050403</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.89.050403</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Bienert</sn>
</person>
<person>
<fn>F.</fn>
<sn>Haug</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. G.</fn>
<sn>Raizen</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>Delgado_2002</citeid>
<title>Quantum gyroscopes and Gödel's universe: entanglement opens a new testing ground for cosmology</title>
<abstract>Some exact solutions of Einstein's field equations represent a
rotating universe. One example is Gödel's cosmological model.
Bianchi solutions generalize the Gödel metric and include the
expansion of the universe. We propose a measurement of the
cosmic rotation using a light or matter wave interferometer
based on the Sagnac effect. Entanglement between the quanta
employed in this quantum gyroscope enhances the accuracy,
thereby coming closer to the more-than-challenging requirements
of such  experiments.</abstract>
<year>2002</year>
<month>6</month>
<DOI>10.1088/1367-2630/4/1/337</DOI>
<journal>New Journal of Physics</journal>
<volume>4</volume>
<publisher>{IOP} Publishing</publisher>
<pages>37--37</pages>
<file_url>https://doi.org/10.1088%2F1367-2630%2F4%2F1%2F337</file_url>
<authors>
<person>
<fn>A.</fn>
<sn>Delgado</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>G.</fn>
<sn>Süßmann</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.65.052109</citeid>
<title>Dimensional enhancement of kinetic energies</title>
<year>2002</year>
<month>4</month>
<DOI>10.1103/PhysRevA.65.052109</DOI>
<journal>Phys. Rev. A</journal>
<volume>65</volume>
<publisher>American Physical Society</publisher>
<pages>052109</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.65.052109</file_url>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.65.052110</citeid>
<title>Localization and diffusion in Ising-type quantum networks</title>
<year>2002</year>
<month>4</month>
<DOI>10.1103/PhysRevA.65.052110</DOI>
<journal>Phys. Rev. A</journal>
<volume>65</volume>
<publisher>American Physical Society</publisher>
<pages>052110</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.65.052110</file_url>
<authors>
<person>
<fn>P.</fn>
<sn>Törmä</sn>
</person>
<person>
<fn>I.</fn>
<sn>Jex</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Meneghini_2002</citeid>
<title>Reshaping of atomic waves with two-dimensional optical crystals</title>
<abstract>We study the dynamics of atomic waves in a two-dimensional light crystal formed
by two crossed standing laser fields. The longitudinal modulation of the crystal
with the Doppler frequency significantly influences the transversal spatial
modulation of the atomic wave. Near the doppleron resonance the atomic density
shows a fractional space period. In this case a normally incident wave gives rise to
an almost perfect conversion into the first momentum components and the light
crystal acts as a highly efficient beamsplitter. The crossing angle, determining
the Doppler frequency, is the easy-to-control parameter of the system.</abstract>
<year>2002</year>
<month>4</month>
<DOI>10.1088/1464-4266/4/3/301</DOI>
<journal>Journal of Optics B: Quantum and Semiclassical Optics</journal>
<volume>4</volume>
<publisher>{IOP} Publishing</publisher>
<pages>165--171</pages>
<number>3</number>
<file_url>https://doi.org/10.1088%2F1464-4266%2F4%2F3%2F301</file_url>
<authors>
<person>
<fn>S.</fn>
<sn>Meneghini</sn>
</person>
<person>
<fn>I.</fn>
<sn>Jex</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>V. P.</fn>
<sn>Yakovlev</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>KONDRASHIN2002319</citeid>
<title>Anomalous kinetics of heavy particles in light media</title>
<abstract>We use anomalous kinetics to create a narrow non-zero atomic velocity distribution. Moreover, we propose a method to control the anomalous transport of atoms in an optical lattice using a polarization gradient. We derive the threshold for this behavior by two different methods.</abstract>
<year>2002</year>
<issn>0301-0104</issn>
<DOI>https://doi.org/10.1016/S0301-0104(02)00555-4</DOI>
<journal>Chemical Physics</journal>
<volume>284</volume>
<pages>319 - 330</pages>
<number>1</number>
<keywords>Anomalous transport, Lévi flights, Optical lattice</keywords>
<file_url>http://www.sciencedirect.com/science/article/pii/S0301010402005554</file_url>
<note>Strange Kinetics</note>
<authors>
<person>
<fn>M. P.</fn>
<sn>Kondrashin</sn>
</person>
<person>
<fn>S.</fn>
<sn>Schaufler</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>V. P.</fn>
<sn>Yakovlev</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.65.022109</citeid>
<title>Concepts of radial and angular kinetic energies</title>
<year>2002</year>
<month>1</month>
<DOI>10.1103/PhysRevA.65.022109</DOI>
<journal>Phys. Rev. A</journal>
<volume>65</volume>
<publisher>American Physical Society</publisher>
<pages>022109</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.65.022109</file_url>
<authors>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<citeid>Riedel2002</citeid>
<title>Control of Dynamical Localization by Additional Quantum Degrees</title>
<abstract>The phenomenon of localization manifests itself in many quantum mechanical systems ranging from the localization of light in a random medium via Anderson localization of an electronic wave to the motion of atoms in time-dependent laser fields. In all these cases the underlying classical system is chaotic and shows diffusion as a function of time. In contrast, the quantum mechanical counterpart has a localized wave function whose width is governed by the classical diffusion and Planck's constant. In this paper we show that there exists an additional quantum parameter that controls the localization length. In the system of a two-level ion stored in a Paul trap and interacting with a standing wave it is the detuning between the transition frequency and the laser field. We also discuss the effect of decoherence in form of spontaneous emission.</abstract>
<year>2002</year>
<isbn>978-0-306-47097-4</isbn>
<DOI>10.1007/0-306-47097-7_43</DOI>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>P. Kumar, G. M. D'Ariano and O. Hirota</editor>
<pages>321--330</pages>
<file_url>https://doi.org/10.1007/0-306-47097-7_43</file_url>
<authors>
<person>
<fn>K.</fn>
<sn>Riedel</sn>
</person>
<person>
<fn>P.</fn>
<sn>Törmä</sn>
</person>
<person>
<fn>V.</fn>
<sn>Savichev</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
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<reference>
<bibtype>inbook</bibtype>
<title>Quantum Estimation with Finite Resources</title>
<year>2002</year>
<booktitle>Quantum Information Technology</booktitle>
<publisher>VCH-Wiley</publisher>
<address>Weinheim</address>
<editor>G. Leuchs and Th. Beth</editor>
<authors>
<person>
<fn>Th. C.</fn>
<sn>Bschorr</sn>
</person>
<person>
<fn>D. G.</fn>
<sn>Fischer</sn>
</person>
<person>
<fn>H.</fn>
<sn>Mack</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>quantumfictious</citeid>
<title>Quantum Fictitious Forces</title>
<abstract>Abstract We present Heisenberg's equation of motion for the radial variable of a free non-relativistic particle in D dimensions. The resulting radial force consists of three contributions: (i) the quantum fictitious force which is either attractive or repulsive depending on the number of dimensions, (ii) a singular quantum force located at the origin, and (iii) the centrifugal force associated with non-vanishing angular momentum. Moreover, we use Heisenberg's uncertainty relation to introduce a lower bound for the kinetic energy of an ensemble of neutral particles. This bound is quadratic in the number of atoms and can be traced back to the repulsive quantum fictitious potential. All three forces arise for a free particle: “Force without force”.</abstract>
<year>2002</year>
<DOI>10.1002/1521-3978(200205)50:5/7<599::AID-PROP599>3.0.CO;2-G</DOI>
<journal>Fortschritte der Physik</journal>
<volume>50</volume>
<pages>599-607</pages>
<number>5‐7</number>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/1521-3978%28200205%2950%3A5/7%3C599%3A%3AAID-PROP599%3E3.0.CO%3B2-G</file_url>
<authors>
<person>
<fn>I.</fn>
<sn>Białynicki-Birula</sn>
</person>
<person>
<fn>M. A.</fn>
<sn>Cirone</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
<person>
<fn>T. H.</fn>
<sn>Seligman</sn>
</person>
<person>
<fn>F.</fn>
<sn>Straub</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
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<reference>
<bibtype>inbook</bibtype>
<title>Wave Packet Dynamics and Factorization of Numbers</title>
<year>2002</year>
<DOI>10.3254/978-1-61499-004-8-369</DOI>
<booktitle>Experimental Quantum Computation and Information</booktitle>
<volume>148</volume>
<publisher>IOS Press</publisher>
<address>Amsterdam, Oxford, Tokyo, Washington DC</address>
<series>Proceedings of the International School of Physics "Enrico Fermi"</series>
<editor>F. De Martini and C. Monroe</editor>
<pages>369-384</pages>
<authors>
<person>
<fn>H.</fn>
<sn>Mack</sn>
</person>
<person>
<fn>M.</fn>
<sn>Bienert</sn>
</person>
<person>
<fn>F.</fn>
<sn>Haug</sn>
</person>
<person>
<fn>F.</fn>
<sn>Straub</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>wavepackets</citeid>
<title>Wave Packets Can Factorize Numbers</title>
<abstract>Abstract We draw attention to various aspects of number theory emerging in the time evolution of elementary quantum systems with quadratic phases. Such model systems can be realized in actual experiments. Our analysis paves the way to a new, promising and effective method to factorize numbers.</abstract>
<year>2002</year>
<DOI>10.1002/1521-3951(200210)233:3<408::AID-PSSB408>3.0.CO;2-N</DOI>
<journal>physica status solidi (b)</journal>
<volume>233</volume>
<pages>408-415</pages>
<number>3</number>
<keywords>03.67.–a, 42.25.–p, 42.25.Hz</keywords>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/1521-3951%28200210%29233%3A3%3C408%3A%3AAID-PSSB408%3E3.0.CO%3B2-N</file_url>
<authors>
<person>
<fn>H.</fn>
<sn>Mack</sn>
</person>
<person>
<fn>M.</fn>
<sn>Bienert</sn>
</person>
<person>
<fn>F.</fn>
<sn>Haug</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Cirone_2001</citeid>
<title>Huygens' principle, the free Schrödinger particle and the quantum anti-centrifugal force</title>
<abstract>Huygens' principle following from the d'Alembert wave equation
is not valid in two-dimensional space. A Schrödinger particle
of vanishing angular momentum moving freely in two dimensions
experiences an attractive force - the quantum anti-centrifugal
force - towards its centre. We connect these two phenomena by
comparing and contrasting the radial propagators of the
d'Alembert wave equation and of a free non-relativistic quantum
mechanical particle in two and three dimensions.</abstract>
<year>2001</year>
<month>12</month>
<DOI>10.1088/0953-4075/35/1/314</DOI>
<journal>Journal of Physics B: Atomic, Molecular and Optical Physics</journal>
<volume>35</volume>
<publisher>{IOP} Publishing</publisher>
<pages>191--203</pages>
<number>1</number>
<file_url>https://doi.org/10.1088%2F0953-4075%2F35%2F1%2F314</file_url>
<authors>
<person>
<fn>M. A.</fn>
<sn>Cirone</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dahl</sn>
</person>
<person>
<fn>M.</fn>
<sn>Fedorov</sn>
</person>
<person>
<fn>D. M.</fn>
<sn>Greenberger</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.65.022101</citeid>
<title>Quantum anticentrifugal force</title>
<year>2001</year>
<month>12</month>
<DOI>10.1103/PhysRevA.65.022101</DOI>
<journal>Phys. Rev. A</journal>
<volume>65</volume>
<publisher>American Physical Society</publisher>
<pages>022101</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.65.022101</file_url>
<authors>
<person>
<fn>M. A.</fn>
<sn>Cirone</sn>
</person>
<person>
<fn>K.</fn>
<sn>Rza̧żewski</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>F.</fn>
<sn>Straub</sn>
</person>
<person>
<fn>J. A.</fn>
<sn>Wheeler</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Gleisberg_2001</citeid>
<title>Friedel oscillations in phase space: Wigner function of trapped interacting fermions</title>
<abstract>The Wigner function W(z,k) for a model of interacting one-dimensional
fermions confined to a harmonic trap is evaluated at zero temperature. The
model considers two hyperfine states of the same fermionic species and
treats the dominant interactions between the two using the bosonization
method. Interactions substantially modify the shape of the Wigner
function. Irrespective of the sign of the coupling constant, the Friedel
oscillations inherent in the Wigner function are enhanced in the
k-direction and suppressed in the z-direction.</abstract>
<year>2001</year>
<month>11</month>
<DOI>10.1088/0953-4075/34/23/309</DOI>
<journal>Journal of Physics B: Atomic, Molecular and Optical Physics</journal>
<volume>34</volume>
<publisher>{IOP} Publishing</publisher>
<pages>4645--4651</pages>
<number>23</number>
<file_url>https://doi.org/10.1088%2F0953-4075%2F34%2F23%2F309</file_url>
<authors>
<person>
<fn>F.</fn>
<sn>Gleisberg</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>W.</fn>
<sn>Wonneberger</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Berry_2001</citeid>
<title>Quantum carpets, carpets of light</title>
<abstract>In 1836 Henry Fox Talbot, an inventor of photography, published the results of some experiments in optics that he had previously demonstrated at a British Association meeting in Bristol (figure 1a). “It was very curious to observe that though the grating was greatly out of the focus of the lens...the appearance of the bands was perfectly distinct and well defined...the experiments are communicated in the hope that they may prove interesting to the cultivators of optical science.”</abstract>
<year>2001</year>
<month>6</month>
<DOI>10.1088/2058-7058/14/6/30</DOI>
<journal>Physics World</journal>
<volume>14</volume>
<publisher>{IOP} Publishing</publisher>
<pages>39--46</pages>
<number>6</number>
<file_url>https://doi.org/10.1088%2F2058-7058%2F14%2F6%2F30</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Berry</sn>
</person>
<person>
<fn>I.</fn>
<sn>Marzoli</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.63.065601</citeid>
<title>Spatiotemporal interferometry for trapped atomic Bose-Einstein condensates</title>
<year>2001</year>
<month>5</month>
<DOI>10.1103/PhysRevA.63.065601</DOI>
<journal>Phys. Rev. A</journal>
<volume>63</volume>
<publisher>American Physical Society</publisher>
<pages>065601</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.63.065601</file_url>
<authors>
<person>
<fn>K.</fn>
<sn>Burnett</sn>
</person>
<person>
<fn>O. M.</fn>
<sn>Friesch</sn>
</person>
<person>
<fn>B.</fn>
<sn>Kneer</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.63.043613</citeid>
<title>Interference of a Bose-Einstein condensate in a hard-wall trap: From the nonlinear Talbot effect to the formation of vorticity</title>
<year>2001</year>
<month>3</month>
<DOI>10.1103/PhysRevA.63.043613</DOI>
<journal>Phys. Rev. A</journal>
<volume>63</volume>
<publisher>American Physical Society</publisher>
<pages>043613</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.63.043613</file_url>
<authors>
<person>
<fn>J.</fn>
<sn>Ruostekoski</sn>
</person>
<person>
<fn>B.</fn>
<sn>Kneer</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>G.</fn>
<sn>Rempe</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1063/1.1369661</citeid>
<title>Molecular quantum dynamics in a thermal system: Fractional wave packet revivals probed by random-phase fluorescence interferometry</title>
<year>2001</year>
<DOI>10.1063/1.1369661</DOI>
<journal>The Journal of Chemical Physics</journal>
<volume>114</volume>
<pages>9901-9910</pages>
<number>22</number>
<authors>
<person>
<fn>Ch.</fn>
<sn>Warmuth</sn>
</person>
<person>
<fn>A.</fn>
<sn>Tortschanoff</sn>
</person>
<person>
<fn>F.</fn>
<sn>Milota</sn>
</person>
<person>
<fn>M.</fn>
<sn>Leibscher</sn>
</person>
<person>
<fn>M.</fn>
<sn>Shapiro</sn>
</person>
<person>
<fn>Y.</fn>
<sn>Prior</sn>
</person>
<person>
<fn>I. Sh.</fn>
<sn>Averbukh</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>W.</fn>
<sn>Jakubetz</sn>
</person>
<person>
<fn>H. F.</fn>
<sn>Kauffmann</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<title>Unusual Bound or Localized States</title>
<year>2001</year>
<DOI>10.1515/zna-2001-0109</DOI>
<journal>Zeitschrift für Naturforschung A</journal>
<volume>56</volume>
<pages>48-60</pages>
<number>1-2</number>
<authors>
<person>
<fn>M. A.</fn>
<sn>Cirone</sn>
</person>
<person>
<fn>G.</fn>
<sn>Metikas</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Saif_2000</citeid>
<title>Quantum revivals in a periodically driven gravitational cavity</title>
<abstract>Quantum revivals are investigated for the dynamics of
an atom in a driven gravitational cavity. It is demonstrated
that the external driving field influences the revival time
significantly. Analytical expressions are presented which are
based on second-order perturbation theory and semiclassical
secular theory. These analytical results explain the dependence
of the revival time on the characteristic parameters of the
problem quantitatively in a simple way. They are in excellent
agreement with numerical results.</abstract>
<year>2000</year>
<month>10</month>
<DOI>10.1088/1464-4266/2/5/315</DOI>
<journal>Journal of Optics B: Quantum and Semiclassical Optics</journal>
<volume>2</volume>
<publisher>{IOP} Publishing</publisher>
<pages>668--671</pages>
<number>5</number>
<file_url>https://doi.org/10.1088%2F1464-4266%2F2%2F5%2F315</file_url>
<authors>
<person>
<fn>F.</fn>
<sn>Saif</sn>
</person>
<person>
<fn>G.</fn>
<sn>Alber</sn>
</person>
<person>
<fn>V.</fn>
<sn>Savichev</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Meneghini2000</citeid>
<title>Atomic focusing and near field imaging: A combination for producing small-period nanostructures</title>
<abstract>We present a scheme which combines focusing of atomic de Broglie waves by standing light waves and fractional Talbot imaging to produce nanostructures. Masking of the incoming atomic wave by an absorptive grating is used to eliminate atom-optical aberrations that would otherwise wash out the fractional Talbot images. The scheme allows the creation of structures of very small feature size as well as small period.</abstract>
<year>2000</year>
<month>5</month>
<day>01</day>
<issn>1432-0649</issn>
<DOI>10.1007/s003400050880</DOI>
<journal>Applied Physics B</journal>
<volume>70</volume>
<pages>675--682</pages>
<number>5</number>
<file_url>https://doi.org/10.1007/s003400050880</file_url>
<authors>
<person>
<fn>S.</fn>
<sn>Meneghini</sn>
</person>
<person>
<fn>V. I.</fn>
<sn>Savichev</sn>
</person>
<person>
<fn>K. A. H.</fn>
<sn>van Leeuwen</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Friesch_2000</citeid>
<title>Quantum carpets woven by Wigner functions</title>
<abstract>The dynamics of many different quantum systems is characterized by a regular net of minima and maxima of probability stretching out in a spacetime representation. We offer an explanation to this phenomenon in terms of the Wigner function. This approach illustrates very clearly the crucial role played by interference.</abstract>
<year>2000</year>
<month>3</month>
<DOI>10.1088/1367-2630/2/1/004</DOI>
<journal>New Journal of Physics</journal>
<volume>2</volume>
<publisher>{IOP} Publishing</publisher>
<pages>4--4</pages>
<file_url>https://doi.org/10.1088%2F1367-2630%2F2%2F1%2F004</file_url>
<authors>
<person>
<fn>O. M.</fn>
<sn>Friesch</sn>
</person>
<person>
<fn>I.</fn>
<sn>Marzoli</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
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<bibtype>article</bibtype>
<citeid>PhysRevA.61.032101</citeid>
<title>Multimode interference: Highly regular pattern formation in quantum wave-packet evolution</title>
<year>2000</year>
<month>2</month>
<DOI>10.1103/PhysRevA.61.032101</DOI>
<journal>Phys. Rev. A</journal>
<volume>61</volume>
<publisher>American Physical Society</publisher>
<pages>032101</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.61.032101</file_url>
<authors>
<person>
<fn>A. E.</fn>
<sn>Kaplan</sn>
</person>
<person>
<fn>I.</fn>
<sn>Marzoli</sn>
</person>
<person>
<fn>W. E.</fn>
<sn>Lamb</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>inproceedings</bibtype>
<title>Atom Optics and the Discreteness of Photons</title>
<year>2000</year>
<booktitle>Quantum Optics of Small Structures</booktitle>
<publisher>Verh. Nat. Kon. Ned. Akad. van Wetensch</publisher>
<editor>D. Lenstra, T.D. Visser and K.A.H. van Leeuwen</editor>
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<fn>H.</fn>
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<person>
<fn>S.</fn>
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<person>
<fn>W. P.</fn>
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<reference>
<bibtype>article</bibtype>
<title>Atomic Motion in Longitudinally Modulated Light Crystals</title>
<year>2000</year>
<journal>Laser Physics</journal>
<volume>10</volume>
<pages>116-122</pages>
<authors>
<person>
<fn>S.</fn>
<sn>Meneghini</sn>
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<person>
<fn>I.</fn>
<sn>Jex</sn>
</person>
<person>
<fn>K. A. H.</fn>
<sn>van Leeuwen</sn>
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<person>
<fn>M. R.</fn>
<sn>Kasimov</sn>
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<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
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<person>
<fn>V. P.</fn>
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<year>2000</year>
<booktitle>Decoherence: Theoretical, Experimental and Conceptual Problems</booktitle>
<publisher>Springer</publisher>
<address>Heidelberg</address>
<editor>Ph. Blanchard, D. Giulini E. Joos C. Kiefer and I.-O. Stamatescu</editor>
<pages>179-189</pages>
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<fn>F.</fn>
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<person>
<fn>K.</fn>
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<fn>W. P.</fn>
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<fn>B.</fn>
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<citeid>Schleich2000</citeid>
<title>Engineering decoherence</title>
<abstract>The quantum world will always tend towards the classical world through a process known as decoherence. This is a major barrier to the success of quantum computers and quantum communication. New experiments that engineer decoherence in the laboratory throw light on what happens when a quantum system evolves into a classical system.</abstract>
<year>2000</year>
<issn>1476-4687</issn>
<DOI>10.1038/35002223</DOI>
<journal>Nature</journal>
<volume>403</volume>
<pages>256-257</pages>
<number>6767</number>
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<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
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<title>Fractional Dynamics in Phase Space</title>
<year>2000</year>
<journal>Laser Physics</journal>
<volume>10</volume>
<pages>123-126</pages>
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<fn>K.</fn>
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<person>
<fn>K.</fn>
<sn>Wódkiewicz</sn>
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<person>
<fn>W.</fn>
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<citeid>doi:10.1080/09500340008232204</citeid>
<title>Non-dissipative decoherence for quantum carpets</title>
<year>2000</year>
<DOI>10.1080/09500340008232204</DOI>
<journal>Journal of Modern Optics</journal>
<volume>47</volume>
<publisher>Taylor & Francis</publisher>
<pages>2891-2904</pages>
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<fn>R.</fn>
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<person>
<fn>I.</fn>
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<fn>W. P.</fn>
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<title>Quantum Optics with Metastable Helium Atoms</title>
<year>2000</year>
<booktitle>Quantum Optics of Small Structures</booktitle>
<publisher>Verh. Nat. Kon. Ned. Akad. van Wetensch.</publisher>
<editor>D. Lenstra, T.D. Visser and K.A.H. van Leeuwen</editor>
<pages>195-206</pages>
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<person>
<fn>K. A. H.</fn>
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<fn>A. E. A.</fn>
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<person>
<fn>M. J.</fn>
<sn>de Koning</sn>
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<person>
<fn>H. C. W.</fn>
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<title>Storage and Read-Out of Quantum-State Information Via Interference</title>
<year>2000</year>
<booktitle>Trends in Quantum Mechanics</booktitle>
<publisher>World Scientific</publisher>
<address>Singapur</address>
<editor>H.-D. Doebner, S.T. Ali, M. Keyl and R.F. Werner</editor>
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<fn>M.</fn>
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<fn>S. H.</fn>
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<citeid>doi:10.1063/1.481060</citeid>
<title>Studying vibrational wavepacket dynamics by measuring fluorescence interference fluctuations</title>
<year>2000</year>
<DOI>10.1063/1.481060</DOI>
<journal>The Journal of Chemical Physics</journal>
<volume>112</volume>
<pages>5060-5069</pages>
<number>11</number>
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<person>
<fn>Ch.</fn>
<sn>Warmuth</sn>
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<person>
<fn>A.</fn>
<sn>Tortschanoff</sn>
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<person>
<fn>F.</fn>
<sn>Milota</sn>
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<person>
<fn>M.</fn>
<sn>Shapiro</sn>
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<person>
<fn>Y.</fn>
<sn>Prior</sn>
</person>
<person>
<fn>I. Sh.</fn>
<sn>Averbukh</sn>
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<person>
<fn>W.</fn>
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<person>
<fn>W.</fn>
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<person>
<fn>H. F.</fn>
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<citeid>CZIRJAK200029</citeid>
<title>The Wigner function for tunneling in a uniform static electric field1Dedicated to Marlan O. Scully on the occasion of his 60th birthday.1</title>
<abstract>The Wigner function is used to study a simple model system for strong-field induced ionization: an electron tunneling out of a zero-range potential in the presence of a uniform static electric field. We derive an analytic expression for an approximate Wigner function describing a stationary situation where the part lost to ionization is continuously replenished. This approach is well justified by comparison with the true time dependent Wigner function obtained by numerically solving the one-dimensional problem. The three- and one-dimensional Wigner functions both suggest that the electron leaves the tunnel with a non-zero velocity.</abstract>
<year>2000</year>
<issn>0030-4018</issn>
<DOI>https://doi.org/10.1016/S0030-4018(99)00591-X</DOI>
<journal>Optics Communications</journal>
<volume>179</volume>
<pages>29 - 38</pages>
<number>1</number>
<file_url>http://www.sciencedirect.com/science/article/pii/S003040189900591X</file_url>
<authors>
<person>
<fn>A.</fn>
<sn>Czirják</sn>
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<person>
<fn>R.</fn>
<sn>Kopold</sn>
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<person>
<fn>W.</fn>
<sn>Becker</sn>
</person>
<person>
<fn>M.</fn>
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<person>
<fn>W. P.</fn>
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</person>
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<citeid>PhysRevA.61.013410</citeid>
<title>Optical Galton board</title>
<year>1999</year>
<month>12</month>
<DOI>10.1103/PhysRevA.61.013410</DOI>
<journal>Phys. Rev. A</journal>
<volume>61</volume>
<publisher>American Physical Society</publisher>
<pages>013410</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.61.013410</file_url>
<authors>
<person>
<fn>D.</fn>
<sn>Bouwmeester</sn>
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<person>
<fn>I.</fn>
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<person>
<fn>G. P.</fn>
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<fn>W.</fn>
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<citeid>Hall_1999</citeid>
<title>Unravelling quantum carpets: a travelling-wave approach</title>
<abstract>Generic channel and ridge structures are known to appear in the time-dependent position probability distribution of a one-dimensional quantum particle confined to a box. These structures are shown to have a detailed quantitative explanation in terms of a travelling-wave decomposition of the probability density, wherein each contributing term corresponds simultaneously to (i) a real wave propagating at a quantized velocity and (ii) to the time-averaged structure of the position distribution along a quantized direction in spacetime. The approach leads to new predictions of channel locations, widths and depths, and is able to provide more structural details than earlier approaches based on partial interference and Wigner functions. Results are also applicable to light diffracted by a periodic grating, and to the quantum rigid rotator.</abstract>
<year>1999</year>
<month>11</month>
<DOI>10.1088/0305-4470/32/47/307</DOI>
<journal>Journal of Physics A: Mathematical and General</journal>
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<publisher>{IOP} Publishing</publisher>
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<title>Simulation of quantum-state endoscopy</title>
<year>1996</year>
<month>4</month>
<DOI>10.1103/PhysRevA.53.2736</DOI>
<journal>Phys. Rev. A</journal>
<volume>53</volume>
<publisher>American Physical Society</publisher>
<pages>2736--2741</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.53.2736</file_url>
<authors>
<person>
<fn>P. J.</fn>
<sn>Bardroff</sn>
</person>
<person>
<fn>E.</fn>
<sn>Mayr</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>P.</fn>
<sn>Domokos</sn>
</person>
<person>
<fn>M.</fn>
<sn>Brune</sn>
</person>
<person>
<fn>J. M.</fn>
<sn>Raimond</sn>
</person>
<person>
<fn>S.</fn>
<sn>Haroche</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Herkommer_1996</citeid>
<title>Localization of an atom by homodyne measurement</title>
<abstract>We study a continuous homodyne measurement of the field transmitted from an optical cavity. In particular, we investigate the back-action of this measurement onto an atom whose centre-of-mass motion is entangled with the cavity field. Using the method of quantum trajectories we calculate analytically and numerically the time evolution of the entangled quantum state, and demonstrate the localization of the atom relative to the nodes of the cavity field. We compare the quantum trajectory formalism of the continuous homodyne measurement to a projection onto quadrature eigenstates of the field and show that in the long-time limit both descriptions are identical.</abstract>
<year>1996</year>
<month>2</month>
<DOI>10.1088/1355-5111/8/1/014</DOI>
<journal>Quantum and Semiclassical Optics: Journal of the European Optical Society Part B</journal>
<volume>8</volume>
<publisher>{IOP} Publishing</publisher>
<pages>189--203</pages>
<number>1</number>
<file_url>https://doi.org/10.1088%2F1355-5111%2F8%2F1%2F014</file_url>
<authors>
<person>
<fn>A. M.</fn>
<sn>Herkommer</sn>
</person>
<person>
<fn>H. J.</fn>
<sn>Carmichael</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<title>A Simple Quantum Mechanical Model of the Adiabatic-Feedback Measurement Method</title>
<year>1996</year>
<booktitle>Quantum Interferometry II</booktitle>
<publisher>VCH-Verlag</publisher>
<address>Weinheim</address>
<editor>F. De Martini, G. Denardo and Y. Shih</editor>
<pages>451-459</pages>
<authors>
<person>
<fn>M.</fn>
<sn>Schröder</sn>
</person>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>F.</fn>
<sn>De Martini</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Atom-Field Interactions and Dressed Atoms</title>
<year>1996</year>
<DOI>10.1002/phbl.19960520736</DOI>
<journal>Phys. Bl.</journal>
<volume>52</volume>
<pages>736-737</pages>
<number>7-8</number>
<annotation>Review of the book with the same title by G. Compagno, R. Passante, and F. Persico</annotation>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<title>Diffraction of Atomic Waves at a Phase Modulated Standing Light Field</title>
<year>1996</year>
<booktitle>Quantum Interferometry II</booktitle>
<publisher>VCH-Verlag</publisher>
<address>Weinheim</address>
<editor>F. De Martini, G. Denardo and Y. Shih</editor>
<pages>413-427</pages>
<authors>
<person>
<fn>E.</fn>
<sn>Mayr</sn>
</person>
<person>
<fn>V. P.</fn>
<sn>Yakovlev</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Direct and Indirect Measures of Phase</title>
<year>1996</year>
<issn>0323-0465</issn>
<journal>Acta Phys. Slovaca</journal>
<volume>46</volume>
<pages>373-379</pages>
<authors>
<person>
<fn>M. T.</fn>
<sn>Fontenelle</sn>
</person>
<person>
<fn>S. L.</fn>
<sn>Braunstein</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<citeid>10.1007/978-1-4757-9742-8_146</citeid>
<title>Dynamical Localization in Atom Optics</title>
<abstract>We investigate the classical and quantum dynamics of atoms moving in a phase-modulated standing light field.</abstract>
<year>1996</year>
<isbn>978-1-4757-9742-8</isbn>
<DOI>10.1007/978-1-4757-9742-8_146</DOI>
<booktitle>Coherence and Quantum Optics VII</booktitle>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>J. H. Eberly, L. Mandel and E. Wolf</editor>
<pages>547--548</pages>
<authors>
<person>
<fn>E.</fn>
<sn>Mayr</sn>
</person>
<person>
<fn>P. J.</fn>
<sn>Bardroff</sn>
</person>
<person>
<fn>D. S.</fn>
<sn>Krähmer</sn>
</person>
<person>
<fn>P.</fn>
<sn>Stifter</sn>
</person>
<person>
<fn>I.</fn>
<sn>Białynicki-Birula</sn>
</person>
<person>
<fn>V. P.</fn>
<sn>Yakovlev</sn>
</person>
<person>
<fn>G.</fn>
<sn>Kurizki</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<citeid>10.1007/978-1-4757-9742-8_153</citeid>
<title>Fractional Revivals</title>
<abstract>In a coherent superposition of many discrete quantum states, each contributing state evolves independently in time. Nevertheless, for short times, the dynamics of such a quantum system is almost periodic with a period T1 corresponding to the typical energy separation between neighboring eigenstates. However, for times larger than this characteristic time, this periodicity disappears and new features emerge1: At fractions of another characteristic time T2 the system is again periodic, however now, with a period which is a fraction of T1. In this note we present an analytical approach2 towards these so-called fractional revivals.</abstract>
<year>1996</year>
<isbn>978-1-4757-9742-8</isbn>
<DOI>10.1007/978-1-4757-9742-8_153</DOI>
<booktitle>Coherence and Quantum Optics VII</booktitle>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>J. H. Eberly, L. Mandel and E. Wolf</editor>
<pages>561--562</pages>
<authors>
<person>
<fn>C.</fn>
<sn>Leichtle</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>I. Sh.</fn>
<sn>Averbukh</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<citeid>10.1007/978-1-4757-9742-8_144</citeid>
<title>Localization of Atoms by Homodyne Measurement</title>
<abstract>An atom passing through a standing electromagnetic wave inside an optical cavity couples via its dipole moment to the cavity field. The state of the combined system is an entangled state of atom and field; consequently, a measurement on one of the subsystems, on either the atom or the field, will provide information about the other. In particular, the position of the atom in the standing wave becomes strongly correlated with the phase of the field, since in the presence of the field the atom becomes polarized and thus changes the phase of the field through its refractive index; the magnitude of this phase change depends on the local light intensity and hence on the position of the atom. A measurement of the phase change due to the atom traversing the cavity can be made, for example, by balanced homodyne detection, and yields information about the position of the atom relative to the nodes and anti-nodes of the standing wave1,2. The information gain implies a localization of an initially extended atomic wave-packet. We have made a detailed investigation of this measurement-induced localization, where the influence of the measurement on the state of the system is described by the method of quantum trajectories3, which links measurement theory with quantum jump simulations. The quantum trajectory method allowed us to calculate the time evolution of the system wave function, conditioned on the measurement record made by the homodyne detector.</abstract>
<year>1996</year>
<isbn>978-1-4757-9742-8</isbn>
<DOI>10.1007/978-1-4757-9742-8_144</DOI>
<booktitle>Coherence and Quantum Optics VII</booktitle>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>J. H. Eberly, L. Mandel and E. Wolf</editor>
<pages>543--544</pages>
<authors>
<person>
<fn>A. M.</fn>
<sn>Herkommer</sn>
</person>
<person>
<fn>H. J.</fn>
<sn>Carmichael</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
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<reference>
<bibtype>inproceedings</bibtype>
<citeid>10.1007/978-1-4757-9742-8_166</citeid>
<title>Manipulation of Cavity Field States with Multi-Level Atoms</title>
<abstract>Recently, we have proposed two schemes to manipulate a quantum state of a single-mode cavity field in a controlled way by sending two-level atoms through a cavity.1,2 In one of these schemes1 a desired cavity field state is build up step by step starting from the vacuum state. Two-level atoms are prepared in a coherent superposition of the lower state and the upper state. Then the atomic coherence is transfered to the cavity field. As a two-level atom can deposit at most one photon in the cavity, we need N atoms to prepare an arbitrary superposition of N + 1 Fock states. However, probabilities enter because all two-level atoms must be detected in the lower state after they have interacted with the cavity field. In this paper we show that the idea can be generalized to atoms with more than two levels. The main advantage of this generalization is that a single atom can transfer a larger amount of coherence to the cavity field.</abstract>
<year>1996</year>
<isbn>978-1-4757-9742-8</isbn>
<DOI>10.1007/978-1-4757-9742-8_166</DOI>
<booktitle>Coherence and Quantum Optics VII</booktitle>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>J. H. Eberly, L. Mandel and E. Wolf</editor>
<pages>589--590</pages>
<authors>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>G.</fn>
<sn>Kurizki</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Paul Trap Multi-Quantum Interactions</title>
<year>1996</year>
<journal>Acta Phys. Slovaca</journal>
<volume>46</volume>
<pages>231-240</pages>
<authors>
<person>
<fn>P. J.</fn>
<sn>Bardroff</sn>
</person>
<person>
<fn>C.</fn>
<sn>Leichtle</sn>
</person>
<person>
<fn>G.</fn>
<sn>Schrade</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Quantum Control of Chaos Inside a Cavity</title>
<year>1996</year>
<journal>Acta Phys. Slovaca</journal>
<volume>46</volume>
<pages>381-386</pages>
<authors>
<person>
<fn>M.</fn>
<sn>Fortunato</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>G.</fn>
<sn>Kurizki</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Schleich1897</citeid>
<title>Quantum Optics: Optical Coherence and Quantum Optics.</title>
<year>1996</year>
<issn>0036-8075</issn>
<DOI>10.1126/science.272.5270.1897-a</DOI>
<journal>Science</journal>
<volume>272</volume>
<publisher>American Association for the Advancement of Science</publisher>
<pages>1897--1898</pages>
<number>5270</number>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
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<reference>
<bibtype>inproceedings</bibtype>
<citeid>10.1007/978-1-4757-9742-8_29</citeid>
<title>Quantum Phase</title>
<abstract>In June 1960 the first in this series of most successful Rochester conferences on Coherence and Quantum Optics took place. At this meeting devoted to Coherence Properties of Electromagnetic Radiation Joe Weber presented a paper1 with the title ``Phase as a Dynamical Variable''. It is remarkable that 35 years later this question it is still such a hot topic that it is the subject of various invited and contributed papers2,3 at the seventh conference of this series. Indeed over the last years the question of a proper quantum mechanical description of phase has attracted a lot of attention. This is on one hand due to the experimental progress in creating non classical states of light which display phase properties different from those of a coherent state, and on the other hand was triggered by the Pegg-Barnett proposal for a hermitian phase operator. Moreover the recent operational approach by Noh, Foug{\`e}res, and Mandel (NFM) opened a new era in this long standing debate. There are many indications that phase will still be a major topic at the next meeting in the new millennium for which Emil Wolf had us sign up already.</abstract>
<year>1996</year>
<isbn>978-1-4757-9742-8</isbn>
<DOI>10.1007/978-1-4757-9742-8_29</DOI>
<booktitle>Coherence and Quantum Optics VII</booktitle>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>Eberly, Joseph H.
and Mandel, Leonard
and Wolf, Emil</editor>
<pages>239--249</pages>
<authors>
<person>
<fn>M.</fn>
<sn>Heni</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<citeid>ISI:A1996BG84V00008</citeid>
<title>Quantum phase, photon counting and EPR variables</title>
<year>1996</year>
<isbn>0-7503-0394-8</isbn>
<issn>0309-8710</issn>
<organization>Israel Physical Society</organization>
<booktitle>Dilemma of Einstein, Podolsky and Rosen - 60 Years Later</booktitle>
<volume>12</volume>
<series>Annals of the Israel Physical Society</series>
<editor>A. Mann and M. Revzen</editor>
<pages>73-82</pages>
<note>International Symposium on the Dilemma of Einstein, Podolsky and Rosen, in Honour of Nathan Rosen, HAIFA, ISRAEL, MAR, 1995</note>
<authors>
<person>
<fn>M. T.</fn>
<sn>Fontenelle</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>M.</fn>
<sn>Heni</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. S.</fn>
<sn>Zubairy</sn>
</person>
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<reference>
<bibtype>inproceedings</bibtype>
<citeid>10.1007/978-1-4757-9742-8_220</citeid>
<title>Simulation of Quantum State Endoscopy</title>
<abstract>In a recent paper1 we have proposed the method of quantum state endoscopy to measure the complete quantum state of a single mode of the electromagnetic field. In the present article we perform numerical simulations of an experimental realization based on realistic parameters2 to demonstrate the experimental feasibility.</abstract>
<year>1996</year>
<isbn>978-1-4757-9742-8</isbn>
<DOI>10.1007/978-1-4757-9742-8_220</DOI>
<booktitle>Coherence and Quantum Optics VII</booktitle>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>J. H. Eberly, L. Mandel and E. Wolf</editor>
<pages>699--700</pages>
<authors>
<person>
<fn>P. J.</fn>
<sn>Bardroff</sn>
</person>
<person>
<fn>E.</fn>
<sn>Mayr</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>P.</fn>
<sn>Domokos</sn>
</person>
<person>
<fn>M.</fn>
<sn>Brune</sn>
</person>
<person>
<fn>J. M.</fn>
<sn>Raimond</sn>
</person>
<person>
<fn>S.</fn>
<sn>Haroche</sn>
</person>
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<reference>
<bibtype>inbook</bibtype>
<citeid>Scully1996</citeid>
<title>The Correlated Spontaneous Emission Maser Gyroscope</title>
<abstract>We dedicate this paper to our hero Charles Townes in recognition of his pioneering work in maser and laser physics as one of the many spin-offs of his great inventions.</abstract>
<year>1996</year>
<isbn>978-1-4612-2378-8</isbn>
<DOI>10.1007/978-1-4612-2378-8_54</DOI>
<publisher>Springer</publisher>
<address>New York, NY</address>
<editor>Chiao, Raymond Y.</editor>
<pages>573--583</pages>
<file_url>https://doi.org/10.1007/978-1-4612-2378-8_54</file_url>
<authors>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.51.4963</citeid>
<title>Quantum state endoscopy: Measurement of the quantum state in a cavity</title>
<year>1995</year>
<month>6</month>
<DOI>10.1103/PhysRevA.51.4963</DOI>
<journal>Phys. Rev. A</journal>
<volume>51</volume>
<publisher>American Physical Society</publisher>
<pages>4963--4966</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.51.4963</file_url>
<authors>
<person>
<fn>P. J.</fn>
<sn>Bardroff</sn>
</person>
<person>
<fn>E.</fn>
<sn>Mayr</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Freyberger_1995</citeid>
<title>Two-mode quantum phase</title>
<abstract>The authors review the operational quantum phase description of Noh, Fougeres and Mandel (1991-3) (NFM) and show that in the strong local oscillator limit it leads us to a two-mode theory of phase. This two-mode description contains the quantum phase of Paul (1993) as a special case. Furthermore this approach connects directly with a generalized and measurable phase space distribution.</abstract>
<year>1995</year>
<month>6</month>
<DOI>10.1088/1355-5111/7/3/001</DOI>
<journal>Quantum and Semiclassical Optics: Journal of the European Optical Society Part B</journal>
<volume>7</volume>
<publisher>{IOP} Publishing</publisher>
<pages>187--203</pages>
<number>3</number>
<file_url>https://doi.org/10.1088%2F1355-5111%2F7%2F3%2F001</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>M.</fn>
<sn>Heni</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>Schrade_1995</citeid>
<title>Wigner functions in the Paul trap</title>
<abstract>The authors review the theory of the harmonic oscillator with time-dependent frequency by means of an approach based on an operator constant of the motion. With the help of this operator constant we define the ground state, the excited states and a coherent state of the oscillator and discuss the time dependence of these states through their Wigner functions. The authors derive the Wigner function of an arbitrary state at time t evolving in the time-dependent harmonic potential. Moreover, they calculate the correlation coefficient between position and momentum, which appears in the Schrodinger uncertainty relation. The authors illustrate their results for the example of a charged particle in the Paul trap.</abstract>
<year>1995</year>
<month>6</month>
<DOI>10.1088/1355-5111/7/3/009</DOI>
<journal>Quantum and Semiclassical Optics: Journal of the European Optical Society Part B</journal>
<volume>7</volume>
<publisher>IOP Publishing</publisher>
<pages>307--325</pages>
<number>3</number>
<file_url>https://doi.org/10.1088%2F1355-5111%2F7%2F3%2F009</file_url>
<authors>
<person>
<fn>G.</fn>
<sn>Schrade</sn>
</person>
<person>
<fn>V. I.</fn>
<sn>Man'ko</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>R. J.</fn>
<sn>Glauber</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevLett.74.3959</citeid>
<title>Dynamical Localization: Classical vs Quantum Oscillations in Momentum Spread of Cold Atoms</title>
<year>1995</year>
<month>5</month>
<DOI>10.1103/PhysRevLett.74.3959</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>74</volume>
<publisher>American Physical Society</publisher>
<pages>3959--3962</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.74.3959</file_url>
<authors>
<person>
<fn>P. J.</fn>
<sn>Bardroff</sn>
</person>
<person>
<fn>I.</fn>
<sn>Białynicki-Birula</sn>
</person>
<person>
<fn>D. S.</fn>
<sn>Krähmer</sn>
</person>
<person>
<fn>G.</fn>
<sn>Kurizki</sn>
</person>
<person>
<fn>E.</fn>
<sn>Mayr</sn>
</person>
<person>
<fn>P.</fn>
<sn>Stifter</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.51.1792</citeid>
<title>Phase distributions and large-amplitude states</title>
<year>1995</year>
<month>3</month>
<DOI>10.1103/PhysRevA.51.1792</DOI>
<journal>Phys. Rev. A</journal>
<volume>51</volume>
<publisher>American Physical Society</publisher>
<pages>1792--1803</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.51.1792</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Hillery</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
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<reference>
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<citeid>Bestle1995</citeid>
<title>Anti-stealth: WKB grapples with a corner</title>
<abstract>We show how the Wentzel-Kramers-Brillouin (WKB) approximation works for potentials with sharp corners.</abstract>
<year>1995</year>
<month>2</month>
<day>01</day>
<issn>1432-0649</issn>
<DOI>10.1007/BF01135876</DOI>
<journal>Applied Physics B</journal>
<volume>60</volume>
<pages>289--299</pages>
<number>2</number>
<file_url>https://doi.org/10.1007/BF01135876</file_url>
<authors>
<person>
<fn>J.</fn>
<sn>Bestle</sn>
</person>
<person>
<fn>W. P.</fn>
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<publisher>American Physical Society</publisher>
<pages>R30--R33</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.47.R30</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>Quantum State Engineering</title>
<year>1993</year>
<booktitle>Symposium on the Foundations of Modern Physics</booktitle>
<publisher>World Scientific</publisher>
<address>Singapore</address>
<editor>P. Busch, P. Lahti and P. Mittelstaedt</editor>
<pages>369-377</pages>
<authors>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>V. M.</fn>
<sn>Akulin</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Bialynicki_Birula_1993</citeid>
<title>Various measures of quantum phase uncertainty: a comparative study</title>
<abstract>We compare and contrast five measures of phase uncertainty of a quantum state corresponding to a single mode of the electromagnetic field. The basis of this study are the states which minimize a particular measure for a fixed number of Fock states and normalization. We find these optimal states and study their characteristic properties. These optimal states allow us to establish an ordering of the different definitions for phase uncertainty.</abstract>
<year>1993</year>
<month>1</month>
<DOI>10.1088/0031-8949/1993/t48/017</DOI>
<journal>Physica Scripta</journal>
<volume>T48</volume>
<publisher>{IOP} Publishing</publisher>
<pages>113--118</pages>
<file_url>https://doi.org/10.1088%2F0031-8949%2F1993%2Ft48%2F017</file_url>
<authors>
<person>
<fn>I.</fn>
<sn>Białynicki-Birula</sn>
</person>
<person>
<fn>M.</fn>
<sn>Freyberger</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1002/phbl.19930491213</citeid>
<title>Wie konstruiert man einen Quantenzustand?</title>
<abstract>Abstract Ein Forschungsschwerpunkt der Quantenoptik ist die Erzeugung von nichtklassischem Licht und das Studium seiner Eigenschaften. Die Herstellung solcher Zustände beschränkte sich bis jetzt auf einige typische Beispiele. Als Quantenoptiker wünscht man sich zu Weihnachten besonders „schöne”︁ Feldzustände, für die es nicht so ganz klar ist, wie man sie konstruieren kann. Um solchen Wünschen entgegenzukommen, beschreiben wir hier ein Verfahren, das es im Prinzip erlaubt, einen beliebigen Zustand für das elektromagnetische Feld aufzubauen. Wir veranschaulichen diese Methode am Beispiel eines Phasenzustands.</abstract>
<year>1993</year>
<DOI>10.1002/phbl.19930491213</DOI>
<journal>Physikalische Blätter</journal>
<volume>49</volume>
<pages>1111-1112</pages>
<number>12</number>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/phbl.19930491213</file_url>
<authors>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>V. M.</fn>
<sn>Akulin</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevLett.69.3298</citeid>
<title>Quantum demolition measurement of photon statistics by atomic beam deflection</title>
<year>1992</year>
<month>12</month>
<DOI>10.1103/PhysRevLett.69.3298</DOI>
<journal>Phys. Rev. Lett.</journal>
<volume>69</volume>
<publisher>American Physical Society</publisher>
<pages>3298--3301</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevLett.69.3298</file_url>
<authors>
<person>
<fn>A. M.</fn>
<sn>Herkommer</sn>
</person>
<person>
<fn>V. M.</fn>
<sn>Akulin</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.46.5363</citeid>
<title>Unique Bell state</title>
<year>1992</year>
<month>11</month>
<DOI>10.1103/PhysRevA.46.5363</DOI>
<journal>Phys. Rev. A</journal>
<volume>46</volume>
<publisher>American Physical Society</publisher>
<pages>5363--5366</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.46.5363</file_url>
<authors>
<person>
<fn>A.</fn>
<sn>Mann</sn>
</person>
<person>
<fn>M.</fn>
<sn>Revzen</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.46.4110</citeid>
<title>Landau-Zener transition to a decaying level</title>
<year>1992</year>
<month>10</month>
<DOI>10.1103/PhysRevA.46.4110</DOI>
<journal>Phys. Rev. A</journal>
<volume>46</volume>
<publisher>American Physical Society</publisher>
<pages>4110--4113</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.46.4110</file_url>
<authors>
<person>
<fn>V. M.</fn>
<sn>Akulin</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.45.6652</citeid>
<title>Phase from Q function via linear amplification</title>
<year>1992</year>
<month>5</month>
<DOI>10.1103/PhysRevA.45.6652</DOI>
<journal>Phys. Rev. A</journal>
<volume>45</volume>
<publisher>American Physical Society</publisher>
<pages>6652--6654</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.45.6652</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>A.</fn>
<sn>Bandilla</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>AGARWAL1992359</citeid>
<title>Einstein-Podolsky-Rosen correlation - parallelism between the Wigner function and the local hidden variable approaches</title>
<abstract>We show that by using Wigner functions one can develop a treatment of the Einstein-Podolsky-Rosen correlated state of two spin 12 systems in a form similar to that of a local hidden variable model. The quantum mechanical results are exactly reproduced at the cost of allowing the probability distribution function to become negative.</abstract>
<year>1992</year>
<issn>0375-9601</issn>
<DOI>https://doi.org/10.1016/0375-9601(92)90887-R</DOI>
<journal>Physics Letters A</journal>
<volume>170</volume>
<pages>359 - 362</pages>
<number>5</number>
<file_url>http://www.sciencedirect.com/science/article/pii/037596019290887R</file_url>
<authors>
<person>
<fn>G. S.</fn>
<sn>Agarwal</sn>
</person>
<person>
<fn>D.</fn>
<sn>Home</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>From the One-Atom Maser to Schrödinger Cats</title>
<year>1992</year>
<booktitle>Proceedings of the 2nd Wigner Symposium</booktitle>
<publisher>World Scientific</publisher>
<address>Singapur</address>
<editor>H.D. Doebner, W. Scherer and F. Schroeck</editor>
<pages>91-103</pages>
<authors>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>G.</fn>
<sn>Süßmann</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>BENARYEH1992259</citeid>
<title>Inhibition of atomic dipole collapses by squeezed light: a Jaynes-Cummings model treatment</title>
<abstract>We investigate the collapse of the atomic dipole caused by a squeezed vacuum in an ideal one-mode cavity. The difference between the collapse times of the two quadrature components of the dipole moments is increasing with increasing squeezing parameter. This phenomenon predicted by a hamiltonian Jaynes-Cummings model is similar to the inhibition and enhancement of atomic phase decay predicted by Gardiner for a markovian system.</abstract>
<year>1992</year>
<issn>0030-4018</issn>
<DOI>https://doi.org/10.1016/0030-4018(92)90272-S</DOI>
<journal>Optics Communications</journal>
<volume>90</volume>
<pages>259 - 264</pages>
<number>4</number>
<file_url>http://www.sciencedirect.com/science/article/pii/003040189290272S</file_url>
<authors>
<person>
<fn>Y.</fn>
<sn>Ben-Aryeh</sn>
</person>
<person>
<fn>C. A.</fn>
<sn>Miller</sn>
</person>
<person>
<fn>H.</fn>
<sn>Risken</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<title>More on Interference in Phase Space</title>
<year>1992</year>
<booktitle>Fundamental Systems in Quantum Optics</booktitle>
<publisher>Elsevier</publisher>
<address>Amsterdam</address>
<editor>J. Dalibard, J. M. Raimond and J. Zinn-Justin</editor>
<pages>713-765</pages>
<authors>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>New laser gyros for tests of metric gravitation theories.</title>
<year>1992</year>
<month>1</month>
<booktitle>Proceedings of the first William Fairbanks meeting on Relativity and Gravitational Experiments in Space</booktitle>
<publisher>World Scientific</publisher>
<address>Singapur</address>
<editor>R. Ruffini</editor>
<keywords>Gravitation Theory: Tests</keywords>
<authors>
<person>
<fn>H.</fn>
<sn>Heitmann</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.44.7642</citeid>
<title>Phase distribution of a quantum state without using phase states</title>
<year>1991</year>
<month>12</month>
<DOI>10.1103/PhysRevA.44.7642</DOI>
<journal>Phys. Rev. A</journal>
<volume>44</volume>
<publisher>American Physical Society</publisher>
<pages>7642--7646</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.44.7642</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.44.5992</citeid>
<title>Micromaser spectrum</title>
<year>1991</year>
<month>11</month>
<DOI>10.1103/PhysRevA.44.5992</DOI>
<journal>Phys. Rev. A</journal>
<volume>44</volume>
<publisher>American Physical Society</publisher>
<pages>5992--5996</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.44.5992</file_url>
<authors>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
<person>
<fn>G. S.</fn>
<sn>Agarwal</sn>
</person>
<person>
<fn>Tran</fn>
<sn>Quang</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.44.3365</citeid>
<title>Exponential decrease in phase uncertainty</title>
<year>1991</year>
<month>9</month>
<DOI>10.1103/PhysRevA.44.3365</DOI>
<journal>Phys. Rev. A</journal>
<volume>44</volume>
<publisher>American Physical Society</publisher>
<pages>3365--3368</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.44.3365</file_url>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dowling</sn>
</person>
<person>
<fn>R. J.</fn>
<sn>Horowicz</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.44.R1462</citeid>
<title>Deflection of atoms by a quantum field</title>
<year>1991</year>
<month>8</month>
<DOI>10.1103/PhysRevA.44.R1462</DOI>
<journal>Phys. Rev. A</journal>
<volume>44</volume>
<publisher>American Physical Society</publisher>
<pages>R1462--R1465</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.44.R1462</file_url>
<authors>
<person>
<fn>V. M.</fn>
<sn>Akulin</sn>
</person>
<person>
<fn>Fam Le</fn>
<sn>Kien</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.44.2172</citeid>
<title>Nonclassical state from two pseudoclassical states</title>
<year>1991</year>
<month>8</month>
<DOI>10.1103/PhysRevA.44.2172</DOI>
<journal>Phys. Rev. A</journal>
<volume>44</volume>
<publisher>American Physical Society</publisher>
<pages>2172--2187</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.44.2172</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M.</fn>
<sn>Pernigo</sn>
</person>
<person>
<fn>Fam Le</fn>
<sn>Kien</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.43.3854</citeid>
<title>Photon statistics of two-mode squeezed states and interference in four-dimensional phase space</title>
<year>1991</year>
<month>4</month>
<DOI>10.1103/PhysRevA.43.3854</DOI>
<journal>Phys. Rev. A</journal>
<volume>43</volume>
<publisher>American Physical Society</publisher>
<pages>3854--3861</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.43.3854</file_url>
<authors>
<person>
<fn>C. M.</fn>
<sn>Caves</sn>
</person>
<person>
<fn>Ch.</fn>
<sn>Zhu</sn>
</person>
<person>
<fn>G. J.</fn>
<sn>Milburn</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>A Gaussian Measure of Quantum Phase Noise</title>
<year>1991</year>
<booktitle>Proceedings of the Workshop on Squeezed States and Uncertainty Relations</booktitle>
<publisher>Nasa Conference Publication</publisher>
<address>Goddard Space Flight Center</address>
<editor>D. Han, Y.S. Kim and W. W. Zachary</editor>
<pages>299-309</pages>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dowling</sn>
</person>
<person>
<fn>R. J.</fn>
<sn>Horowicz</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>A Jump Shot at the Wigner Distribution</title>
<year>1991</year>
<DOI>10.1063/1.2810308</DOI>
<journal>Phys. Today</journal>
<edition>10</edition>
<volume>44</volume>
<pages>146-148</pages>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>G.</fn>
<sn>Süßmann</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1002/andp.19915030702</citeid>
<title>Interference in Phase Space</title>
<abstract>Abstract A central problem in quantum mechanics is the calculation of the overlap, that is, the scalar product between two quantum states. In the semiclassical limit (Bohr's correspondence principle) we visualize this quantity as the area of overlap between two bands in phase space. In the case of more than one overlap the contributing amplitudes have to be combined with a phase difference again determined by an area in phase space. In this sense the familiar double-slit interference experiment is generalized to an interference in phase space. We derive this concept by the WKB approximation, illustrate it by the example of Franck-Condon transitions in diatomic molecules, and compare it with and contrast it to Wigner's concept of pseudo-probabilities in phase space.</abstract>
<year>1991</year>
<isbn>978-3-540-47901-7</isbn>
<DOI>10.1002/andp.19915030702</DOI>
<booktitle>The Physics of Phase Space Nonlinear Dynamics and Chaos Geometric Quantization, and Wigner Function</booktitle>
<journal>Annalen der Physik</journal>
<volume>503</volume>
<publisher>Springer Berlin Heidelberg</publisher>
<address>Berlin, Heidelberg</address>
<editor>Kim, Y. S.
and Zachary, W. W.</editor>
<pages>423-478</pages>
<number>7</number>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/andp.19915030702</file_url>
<authors>
<person>
<fn>J. P.</fn>
<sn>Dowling</sn>
</person>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>J. A.</fn>
<sn>Wheeler</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1002/phbl.19910470707</citeid>
<title>Vom Ätherwind zu neuem Licht</title>
<abstract>Abstract „Erst die Theorie entscheidet darüber, was man beobachten kann.”︁ Diese Bemerkung richtete Albert Einstein im Frühjahr 1926 an Werner Heisenberg im Anschluß an dessen Kolloquiumsvortrag in Berlin. Damals galt es einen scheinbaren Widerspruch zwischen Theorie und Experiment aufzulösen: Auf der einen Seite verbietet der Formalismus der Quantenmechanik und insbesondere die Kommutatorbeziehung zwischen Ort und Impuls eines Teilchens die Existenz einer Trajektorie. Andererseits beobachtet man diese in einer Wilson-Blasenkammer. Die Auflösung dieses scheinbaren Widerspruchs gelang Heisenberg mit Hilfe der Unbestimmtheitsrelation. – Heute entscheidet die Unbestimmtheitsrelation zwischen elektrischem und magnetischem Feld, d. h. die Fluktuationen in der Amplitude und der Phase des elektromagnetischen Feldes in einem Michelson-Interferometer über die prinzipielle Beobachtbarkeit einer winzigen Gravitationswelleninduzierten Phasenverschiebung. Dies hat die Entwicklung quantenrausch-verminderter Zustände des Strahlungsfeldes, der gequetschten (engl. squeezed) Zustände, motiviert und ein neues Gebiet der Quantenoptik geschaffen. Ähnlich haben die Überlegungen, die Existenz von bevorzugten Bezugsystemen und von Mitführeffekten mittels des Sagnac-Effektes nachweisen zu wollen, auf einen neuen Typ von Laser geführt, der frei von spontaner Emission ist. – In der vorliegenden Arbeit wollen wir diesen Weg vom Sagnac-Effekt, der ursprünglich als Äthernachweis konzipiert war, zu squeezed Zuständen und zum rauschfreien Laser mit korrelierter Spontanemission, d. h. zu neuem Licht nachzeichnen. Die oszillierende Photonenstatistik eines gequetschten Zustandes und ihre Interpretation als Interferenz im Phasenraum bildet den Abschluß unserer Wanderung vom Ätherwind zu neuem Licht.</abstract>
<year>1991</year>
<DOI>10.1002/phbl.19910470707</DOI>
<journal>Physikalische Blätter</journal>
<volume>47</volume>
<pages>595-601</pages>
<number>7</number>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/phbl.19910470707</file_url>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.42.1703</citeid>
<title>Quantum superpositions generated by quantum nondemolition measurements</title>
<year>1990</year>
<month>8</month>
<DOI>10.1103/PhysRevA.42.1703</DOI>
<journal>Phys. Rev. A</journal>
<volume>42</volume>
<publisher>American Physical Society</publisher>
<pages>1703--1711</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.42.1703</file_url>
<authors>
<person>
<fn>B.</fn>
<sn>Yurke</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>D. F.</fn>
<sn>Walls</sn>
</person>
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</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.42.1503</citeid>
<title>Quantum-noise suppression in lasers via memory-correlation effects</title>
<year>1990</year>
<month>8</month>
<DOI>10.1103/PhysRevA.42.1503</DOI>
<journal>Phys. Rev. A</journal>
<volume>42</volume>
<publisher>American Physical Society</publisher>
<pages>1503--1514</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.42.1503</file_url>
<authors>
<person>
<fn>C.</fn>
<sn>Benkert</sn>
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<person>
<fn>M. O.</fn>
<sn>Scully</sn>
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<person>
<fn>W.</fn>
<sn>Schleich</sn>
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<person>
<fn>A. A.</fn>
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<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.41.3950</citeid>
<title>Noise-color-induced quenching of fluctuations in a correlated spontaneous-emission laser model</title>
<year>1990</year>
<month>4</month>
<DOI>10.1103/PhysRevA.41.3950</DOI>
<journal>Phys. Rev. A</journal>
<volume>41</volume>
<publisher>American Physical Society</publisher>
<pages>3950--3959</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.41.3950</file_url>
<authors>
<person>
<fn>R. G. K.</fn>
<sn>Habiger</sn>
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<person>
<fn>H.</fn>
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<person>
<fn>M.</fn>
<sn>James</sn>
</person>
<person>
<fn>F.</fn>
<sn>Moss</sn>
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<person>
<fn>W.</fn>
<sn>Schleich</sn>
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<reference>
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<citeid>doi:10.1002/andp.19905020805</citeid>
<title>A Heuristic Analysis of Quantum Noise Quenching in the Two-Photon Correlated Emission Laser</title>
<abstract>Abstract We demonstrate how the two-photon correlated emission laser (CEL) can be understood from a simple physical picture in a quasirigorous fashion. We use semiclassical arguments to derive correct expressions for the phase and amplitude diffusion in a simple way. We then illustrate how noise suppression is achieved in the two-photon CEL.</abstract>
<year>1990</year>
<DOI>10.1002/andp.19905020805</DOI>
<journal>Annalen der Physik</journal>
<volume>502</volume>
<pages>649-658</pages>
<number>8</number>
<file_url>https://onlinelibrary.wiley.com/doi/abs/10.1002/andp.19905020805</file_url>
<authors>
<person>
<fn>C.</fn>
<sn>Benkert</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<title>Asymptotology in Quantum Optics</title>
<year>1990</year>
<booktitle>New Frontiers in QED and Quantum Optics</booktitle>
<publisher>Plenum Press</publisher>
<address>New York</address>
<editor>A. Barut</editor>
<pages>31-61</pages>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>J. P.</fn>
<sn>Dowling</sn>
</person>
<person>
<fn>R. J.</fn>
<sn>Horowicz</sn>
</person>
<person>
<fn>S.</fn>
<sn>Varro</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Ordnung und Chaos in der Paul-Falle</title>
<year>1990</year>
<journal>Spektrum der Wissenschaft</journal>
<pages>106</pages>
<authors>
<person>
<fn>W.</fn>
<sn>Quint</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<citeid>doi:10.1142/9789812819895_0035</citeid>
<title>Quantum Effects in Single-Atom and Single-Photon Experiments</title>
<abstract> Abstract We review our recent work on the one-atom maser. We propose and analyse an experiment based on this maser and designed to probe the way in which the measurement process, that is, the presence of a detector influences the investigated quantum system. Phase transitions between chaotic and ordered structures of ions stored in a Paul trap are analysed. </abstract>
<year>1990</year>
<isbn>978-1-4684-1342-7</isbn>
<DOI>10.1142/9789812819895_0035</DOI>
<booktitle>Foundations of Quantum Mechanics in the Light of New Technology</booktitle>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>W. Demtröder and M. Inguscio</editor>
<pages>336-346</pages>
<file_url>https://doi.org/10.1007/978-1-4684-1342-7_2</file_url>
<authors>
<person>
<fn>G.</fn>
<sn>Rempe</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>refId0</citeid>
<title>The 1989 Nobel Prize. Ion Traps, an Isolated Electron
and Atomic Clocks</title>
<year>1990</year>
<DOI>10.1051/epn/19902102031</DOI>
<journal>Europhys. News</journal>
<volume>21</volume>
<pages>31-33</pages>
<number>2</number>
<file_url>https://doi.org/10.1051/epn/19902102031</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.40.7405</citeid>
<title>Bifurcation in the phase probability distribution of a highly squeezed state</title>
<year>1989</year>
<month>12</month>
<DOI>10.1103/PhysRevA.40.7405</DOI>
<journal>Phys. Rev. A</journal>
<volume>40</volume>
<publisher>American Physical Society</publisher>
<pages>7405--7408</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.40.7405</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>R. J.</fn>
<sn>Horowicz</sn>
</person>
<person>
<fn>S.</fn>
<sn>Varro</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Qunit_1989</citeid>
<title>Order and chaos with frozen ions</title>
<abstract>A single ion at rest, unperturbed by its environment and forced into such a state for hours – once only a physicist's dream – has now been achieved by the combination of electromagnetic traps and laser technology. The Penning trap and the dynamical Paul trap developed in the 1930s and the late 1950s respectively, provide the experimenter with a unique tool to isolate a single ion from its surroundings. Tunable lasers can then be used to force the ion to fluoresce; simultaneously, as will be described, it is cooled to milli- or even micro-Kelvin temperatures. An ion driven into saturation by a sufficiently high laser intensity so that it spends half of the time in the excited state and half in the ground state, scatters roughly 108 photons per second. This leads to a high detection probability and at the same time to a reduction of the ion's kinetic energy via photon recoil.</abstract>
<year>1989</year>
<month>8</month>
<DOI>10.1088/2058-7058/2/8/22</DOI>
<journal>Physics World</journal>
<volume>2</volume>
<publisher>{IOP} Publishing</publisher>
<pages>30--34</pages>
<number>8</number>
<file_url>https://doi.org/10.1088%2F2058-7058%2F2%2F8%2F22</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Quint</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
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<reference>
<bibtype>inproceedings</bibtype>
<title>A Physical Picture of the Two-Photon Correlated Spontaneous Emission Laser</title>
<year>1989</year>
<booktitle>Proceedings of the Eleventh International Conference on Atomic Physics</booktitle>
<publisher>World Scientific</publisher>
<address>Singapur</address>
<editor>S. Haroche, J.C. Gay and G. Grynberg</editor>
<pages>457-465</pages>
<authors>
<person>
<fn>C.</fn>
<sn>Benkert</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>Area of Overlap and Interference in Phase Space as a Guide to Phase Distribution and Wigner Function in Action-Angle Variables of a Squeezed State</title>
<year>1989</year>
<isbn>978-3-642-74953-7</isbn>
<issn>0930-8989</issn>
<booktitle>Quantum Optics V</booktitle>
<journal>Proceedings of the Fifth International Symposium Rotorua, New Zealand, February 13–17, 1989</journal>
<volume>41</volume>
<publisher>Springer</publisher>
<address>Berlin, Heidelberg</address>
<series>Springer Proceedings in Physics</series>
<editor>J.D. Harvey and D. F. Walls</editor>
<pages>133-142</pages>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>R. J.</fn>
<sn>Horowicz</sn>
</person>
<person>
<fn>S.</fn>
<sn>Varro</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Schleich1989</citeid>
<title>Humpty Dumpty to Moslem art</title>
<year>1989</year>
<issn>1476-4687</issn>
<DOI>10.1038/339257a0</DOI>
<journal>Nature</journal>
<volume>339</volume>
<pages>257-258</pages>
<number>6222</number>
<file_url>https://doi.org/10.1038/339257a0</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>P. V. E.</fn>
<sn>McClintock</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<title>Le piégeage des ions</title>
<year>1989</year>
<journal>La Recherche</journal>
<volume>20</volume>
<pages>1194-1203</pages>
<authors>
<person>
<fn>W.</fn>
<sn>Quint</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<citeid>1989nnds....2..271V</citeid>
<title>Noise in a ring-laser gyroscope</title>
<year>1989</year>
<booktitle>Noise in nonlinear dynamical systems</booktitle>
<volume>2</volume>
<publisher>Cambridge University Press</publisher>
<address>Cambridge and New York</address>
<editor>F. Moss and P.V.E. McClintock</editor>
<pages>271-292</pages>
<keywords>Laser Gyroscopes, Noise Spectra, Ring Lasers, White Noise, Beat Frequencies, Fokker-Planck Equation, Langevin Formula, Laser Interferometry, Wave Propagation</keywords>
<authors>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>H.</fn>
<sn>Risken</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<citeid>Schleich1989</citeid>
<title>Phase Space, Correspondence Principle and Dynamical Phases: Photon Count Probabilities of Coherent and Squeezed States via Interfering Areas in Phase Space</title>
<abstract>Motion of an electron around a nucleus or, in its most elementary version, vibratory motion of a harmonic oscillator viewed in Planck-Bohr-Sommerfeld quantized phase space;1--3 and matching the discrete, microscopic world with the continuous, macroscopic world via Bohr's correspondence principle,4--5 these are the essential ingredients of ``Atommechanik''.4 Combined with the concept of interference - expressed in the familiar double-slit experiment6 - these central ideas of early quantum mechanics provide in the present paper the most vivid sources of insight into the photon count probability, Wm, of a coherent state7--9 shown in Fig. 1 and into the oscillatory10--15 photon statistics16 of a highly squeezed stat17 of a single mode of the electromagnetic field depicted in Fig. 2.</abstract>
<year>1989</year>
<isbn>978-1-4757-6574-8</isbn>
<DOI>10.1007/978-1-4757-6574-8_10</DOI>
<booktitle>Squeezed and Non-Classical Light</booktitle>
<volume>190</volume>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<series>NATO ASI Series (Series B: Physics)</series>
<editor>P. Tombesi and E. R. Pike</editor>
<pages>129--149</pages>
<file_url>https://doi.org/10.1007/978-1-4757-6574-8_10</file_url>
<authors>
<person>
<fn>W. P.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>Phase Transitions of Stored Laser-Cooled Ions</title>
<year>1989</year>
<booktitle>Proceedings of the Eleventh International Conference on Atomic Physics</booktitle>
<publisher>World Scientific</publisher>
<address>Singapur</address>
<editor>S. Haroche, J.C. Gay and G. Grynberg</editor>
<pages>243-259</pages>
<authors>
<person>
<fn>R.</fn>
<sn>Blümel</sn>
</person>
<person>
<fn>J. M.</fn>
<sn>Chen</sn>
</person>
<person>
<fn>F.</fn>
<sn>Diedrich</sn>
</person>
<person>
<fn>E.</fn>
<sn>Peik</sn>
</person>
<person>
<fn>W.</fn>
<sn>Quint</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>Y. R.</fn>
<sn>Shen</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<citeid>Orszag1989</citeid>
<title>The Correlated Spontaneous Emission Laser: Theory and Recent Developments</title>
<abstract>As originally conceived a correlated spontaneous emission laser showed quenching of spontaneous emission quantum fluctuations in the relative phase angle of a two mode laser. It has been shown by several approaches (e.g. quantum noise operator, Fokker-Planck equation, etc.) that such devices can, in principle, have vanishing noise in this relative phase angle. A geometric pictorial analysis along these lines has been given and provides a simple intuitive explanation for this quantum noise quenching which has also been supported by recent experimental investigations.</abstract>
<year>1989</year>
<isbn>978-1-4757-6574-8</isbn>
<DOI>10.1007/978-1-4757-6574-8_21</DOI>
<booktitle>Squeezed and Non-Classical Light</booktitle>
<volume>190</volume>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<series>NATO ASI Series (Series B: Physics)</series>
<editor>P. Tombesi and E. R. Pike</editor>
<pages>287--299</pages>
<file_url>https://doi.org/10.1007/978-1-4757-6574-8_21</file_url>
<authors>
<person>
<fn>M.</fn>
<sn>Orszag</sn>
</person>
<person>
<fn>J.</fn>
<sn>Bergou</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Schleich1988</citeid>
<title>Area in phase space as determiner of transition probability: Bohr-Sommerfeld bands, Wigner ripples, and Fresnel zones</title>
<abstract>We consider an oscillator subjected to a sudden change in equilibrium position or in effective spring constant, or both---to a ``squeeze'' in the language of quantum optics. We analyze the probability of transition from a given initial state to a final state, in its dependence on final-state quantum number. We make use of five sources of insight: Bohr-Sommerfeld quantization via bands in phase space, area of overlap between before-squeeze band and after-squeeze band, interference in phase space, Wigner function as quantum update of B-S band and near-zone Fresnel diffraction as mockup Wigner function.</abstract>
<year>1988</year>
<month>10</month>
<day>01</day>
<issn>1572-9516</issn>
<DOI>10.1007/BF01909932</DOI>
<journal>Found. Phys.</journal>
<volume>18</volume>
<pages>953--968</pages>
<number>10</number>
<file_url>https://doi.org/10.1007/BF01909932</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
<person>
<fn>J. A.</fn>
<sn>Wheeler</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.38.1177</citeid>
<title>Area of overlap and interference in phase space versus Wigner pseudoprobabilities</title>
<year>1988</year>
<month>8</month>
<DOI>10.1103/PhysRevA.38.1177</DOI>
<journal>Phys. Rev. A</journal>
<volume>38</volume>
<publisher>American Physical Society</publisher>
<pages>1177--1186</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.38.1177</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>D. F.</fn>
<sn>Walls</sn>
</person>
<person>
<fn>J. A.</fn>
<sn>Wheeler</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.37.3010</citeid>
<title>Quantum-noise quenching in the correlated spontaneous-emission laser as a multiplicative noise process. II. Rigorous analysis including amplitude noise</title>
<year>1988</year>
<month>4</month>
<DOI>10.1103/PhysRevA.37.3010</DOI>
<journal>Phys. Rev. A</journal>
<volume>37</volume>
<publisher>American Physical Society</publisher>
<pages>3010--3017</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.37.3010</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
<person>
<fn>H.-G.</fn>
<sn>Garssen</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.37.1261</citeid>
<title>Quantum-noise quenching in the correlated spontaneous-emission laser as a multiplicative noise process. I. A geometrical argument</title>
<year>1988</year>
<month>2</month>
<DOI>10.1103/PhysRevA.37.1261</DOI>
<journal>Phys. Rev. A</journal>
<volume>37</volume>
<publisher>American Physical Society</publisher>
<pages>1261--1269</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.37.1261</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Bluemel1988</citeid>
<title>Phase transitions of stored laser-cooled ions</title>
<abstract>Single ions in miniature traps can be imaged by using laser light to stimulate fluorescence radiation. At the same time, radiation pressure can be used to bring them nearly to rest. When a small number of ions are trapped, phase transitions can be observed between a chaotic cloud and an ordered crystalline structure, depending on the degree of laser cooling.</abstract>
<year>1988</year>
<issn>1476-4687</issn>
<DOI>10.1038/334309a0</DOI>
<journal>Nature</journal>
<volume>334</volume>
<pages>309-313</pages>
<number>6180</number>
<file_url>https://doi.org/10.1038/334309a0</file_url>
<authors>
<person>
<fn>R.</fn>
<sn>Blümel</sn>
</person>
<person>
<fn>J. M.</fn>
<sn>Chen</sn>
</person>
<person>
<fn>E.</fn>
<sn>Peik</sn>
</person>
<person>
<fn>W.</fn>
<sn>Quint</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>Y. R.</fn>
<sn>Shen</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>Schleich:87</citeid>
<title>Oscillations in photon distribution of squeezed states</title>
<abstract>We show that the photon distribution of a highly squeezed state exhibits oscillations.</abstract>
<year>1987</year>
<month>10</month>
<DOI>10.1364/JOSAB.4.001715</DOI>
<journal>J. Opt. Soc. Am. B</journal>
<volume>4</volume>
<publisher>OSA</publisher>
<pages>1715--1722</pages>
<number>10</number>
<keywords>Coherent states; Mathematical methods; Phase space analysis methods; Photons; Quantum fluctuations; Squeezed states</keywords>
<file_url>http://josab.osa.org/abstract.cfm?URI=josab-4-10-1715</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>J. A.</fn>
<sn>Wheeler</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.35.4882</citeid>
<title>Locking equation with colored noise: Continued fraction solution versus decoupling theory</title>
<year>1987</year>
<month>6</month>
<DOI>10.1103/PhysRevA.35.4882</DOI>
<journal>Phys. Rev. A</journal>
<volume>35</volume>
<publisher>American Physical Society</publisher>
<pages>4882--4885</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.35.4882</file_url>
<authors>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>Th.</fn>
<sn>Leiber</sn>
</person>
<person>
<fn>H.</fn>
<sn>Risken</sn>
</person>
<person>
<fn>P.</fn>
<sn>Hänggi</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.35.2532</citeid>
<title>Delayed-choice experiments in quantum interference</title>
<year>1987</year>
<month>3</month>
<DOI>10.1103/PhysRevA.35.2532</DOI>
<journal>Phys. Rev. A</journal>
<volume>35</volume>
<publisher>American Physical Society</publisher>
<pages>2532--2541</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.35.2532</file_url>
<authors>
<person>
<fn>T.</fn>
<sn>Hellmuth</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
<person>
<fn>A.</fn>
<sn>Zajonc</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
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<reference>
<bibtype>article</bibtype>
<citeid>doi:10.1063/1.339751</citeid>
<title>Colored noise in the ring‐laser gyroscope: Theory and simulation</title>
<year>1987</year>
<DOI>10.1063/1.339751</DOI>
<journal>J. Appl. Phys.</journal>
<volume>62</volume>
<pages>721-723</pages>
<number>2</number>
<authors>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>H.</fn>
<sn>Risken</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M.</fn>
<sn>James</sn>
</person>
<person>
<fn>F.</fn>
<sn>Moss</sn>
</person>
<person>
<fn>R.</fn>
<sn>Mannella</sn>
</person>
<person>
<fn>P. V. E.</fn>
<sn>McClintock</sn>
</person>
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<reference>
<bibtype>inbook</bibtype>
<citeid>PhaseSpace1987</citeid>
<title>Interference in Phase Space</title>
<year>1987</year>
<isbn>978-3-540-47901-7</isbn>
<DOI>10.1007/3-540-17894-5_346</DOI>
<booktitle>The Physics of Phase Space Nonlinear Dynamics and Chaos Geometric Quantization, and Wigner Function</booktitle>
<volume>278</volume>
<publisher>Springer</publisher>
<address>Berlin, Heidelberg</address>
<series>Lecture Notes in Physics</series>
<editor>Y.S. Kim and W.W. Zachary</editor>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>J. A.</fn>
<sn>Wheeler</sn>
</person>
</authors>
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<reference>
<bibtype>article</bibtype>
<citeid>Schleich1987</citeid>
<title>Oscillations in photon distribution of squeezed states and interference in phase space</title>
<abstract>The drive for both noise-free message transmission1,2 and high precision gravity wave detection3,4 has stimulated immense effort on a key element, a squeezed state5,6 of the electromagnetic field. Such non-classical states have been investigated theoretically in great detail1-7 and have now been realized experimentally in four laboratories in the United States8-13. However, nowhere in the literature have we been able to find the striking feature of a squeezed state which we report here: an oscillatory distribution in photon number14,15. These oscillations, and the conditions which produce them, came to light in the course of an investigation of sudden transitions16 (the Franck-Condon effect in molecular physics17,18) based on the semi-classical description of a quantum state19 as motion of a representative point in the phase space defined by oscillator coordinate and oscillator momentum.</abstract>
<year>1987</year>
<issn>1476-4687</issn>
<DOI>10.1038/326574a0</DOI>
<journal>Nature</journal>
<volume>326</volume>
<pages>574-577</pages>
<number>6113</number>
<file_url>https://doi.org/10.1038/326574a0</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>J. A.</fn>
<sn>Wheeler</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<title>Single Atom and Single Photon Experiments</title>
<year>1987</year>
<booktitle>Foundations of quantum mechanics in the light of new technology, Proceedings of the Second International Symposium on Foundations of Quantum Mechanics</booktitle>
<publisher>Physical Society of Japan</publisher>
<address>Tokyo</address>
<editor>K. Kamiyama</editor>
<pages>25--35</pages>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>H.</fn>
<sn>Walther</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.35.463</citeid>
<title>Skewed probability densities in the ring laser gyroscope: A colored noise effect</title>
<year>1987</year>
<month>1</month>
<DOI>10.1103/PhysRevA.35.463</DOI>
<journal>Phys. Rev. A</journal>
<volume>35</volume>
<publisher>American Physical Society</publisher>
<pages>463--465</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.35.463</file_url>
<authors>
<person>
<fn>K.</fn>
<sn>Vogel</sn>
</person>
<person>
<fn>H.</fn>
<sn>Risken</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M.</fn>
<sn>James</sn>
</person>
<person>
<fn>F.</fn>
<sn>Moss</sn>
</person>
<person>
<fn>P. V. E.</fn>
<sn>McClintock</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<citeid>10.1007/978-3-540-47973-4_35</citeid>
<title>Tests of General Relativity and the Correlated Emission Laser</title>
<abstract>The arena of space-time and metric gravity is a grand playground for modern quantum optical scientists. Work in this field defines the cutting edge of technology, from precision interferometry to the quantum ``limits'' of measurement.</abstract>
<year>1987</year>
<isbn>978-3-540-47973-4</isbn>
<DOI>10.1007/978-3-540-47973-4_35</DOI>
<booktitle>Laser Spectroscopy VIII</booktitle>
<edition>Springer Series in Optical Sciences</edition>
<volume>55</volume>
<publisher>Springer</publisher>
<address>Berlin, Heidelberg</address>
<editor>W. Persson and S. Svanberg</editor>
<pages>139--142</pages>
<authors>
<person>
<fn>J.</fn>
<sn>Gea-Banacloche</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<citeid>pedrotti1985</citeid>
<title>Laser Probes Of General Relativity</title>
<year>1986</year>
<DOI>10.1117/12.976087</DOI>
<booktitle>Proceedings of the Southwest Conference on Optics, Albuquerque 1985</booktitle>
<volume>0540</volume>
<publisher>SPIE</publisher>
<address>Bellingham</address>
<editor>S. Stotlar</editor>
<authors>
<person>
<fn>L. M.</fn>
<sn>Pedrotti</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inbook</bibtype>
<citeid>Schleich1986</citeid>
<title>Nonequilibrium Statistical Physics in a Dithered Ring Laser Gyroscope or Quantum Noise in Pure and Applied Physics</title>
<abstract>In the year 1851 Foucault demonstrated that the slow rotation of the plane of vibration of a pendulum could be used as evidence of the earth's own rotation. Nowadays high precision measurements of the earth's rotation are performed by using radio telescopes in Very Long Baseline interferometry [1]. However, a recent proposal [2] takes advantage of the ultra high sensitivity of a ring laser gyroscope [3] of 10m diameter to monitor changes in earth rate* or Universal time. The underlying principle of such a device is the optical analogue of the Foucault pendulum, the so-called Sagnac effect [5,6]. The frequencies of two counterpropagating waves in a ring interferometer are slightly different when the interferometer is rotating about an axis perpendicular to its plane. Since this frequency difference is proportional to the rotation rate it provides a direct measure of the rotation of the system.</abstract>
<year>1986</year>
<isbn>978-1-4613-2181-1</isbn>
<DOI>10.1007/978-1-4613-2181-1_27</DOI>
<booktitle>Frontiers of Nonequilibrium Statistical Physics</booktitle>
<volume>135</volume>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<series>NATO ASI Series (Series B: Physics)</series>
<editor>G.T. Moore and M. O. Scully</editor>
<pages>385--408</pages>
<file_url>https://doi.org/10.1007/978-1-4613-2181-1_27</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>P.</fn>
<sn>Dobiasch</sn>
</person>
<person>
<fn>V. E.</fn>
<sn>Sanders</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>RevModPhys.57.61</citeid>
<title>The ring laser gyro</title>
<year>1985</year>
<month>1</month>
<DOI>10.1103/RevModPhys.57.61</DOI>
<journal>Rev. Mod. Phys.</journal>
<volume>57</volume>
<publisher>American Physical Society</publisher>
<pages>61--104</pages>
<file_url>https://link.aps.org/doi/10.1103/RevModPhys.57.61</file_url>
<authors>
<person>
<fn>W. W.</fn>
<sn>Chow</sn>
</person>
<person>
<fn>J.</fn>
<sn>Gea-Banacloche</sn>
</person>
<person>
<fn>V. E.</fn>
<sn>Sanders</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<citeid>Scully:1982fn</citeid>
<title>General Relativity and Modern Optics</title>
<year>1984</year>
<booktitle>New Trends in Atomic Physics</booktitle>
<journal>Proceedings of the Les Houches Summer School, Session XXXVIII, 1982</journal>
<publisher>North Holland Physics Publ.</publisher>
<address>Amsterdam</address>
<editor>R. Stora and G. Grynberg</editor>
<pages>995-1124</pages>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>SCHLEICH198463</citeid>
<title>Noise analysis of ring-laser gyroscope with arbitrary dither</title>
<abstract>A “universal” formalism is presented which allows to treat quantum noise in a ring-laser gyroscope in the presence of any arbitrary, periodic and symmetric dither. An exact expression for the mean beat frequency ⤤Æ↩F↩t in terms of infinite matrix continued fractions is obtained. The results are applied to a square-wave dithered gyroscope.</abstract>
<year>1984</year>
<issn>0030-4018</issn>
<DOI>https://doi.org/10.1016/0030-4018(84)90074-9</DOI>
<journal>Opt. Commun.</journal>
<volume>52</volume>
<pages>63 - 68</pages>
<number>1</number>
<file_url>http://www.sciencedirect.com/science/article/pii/0030401884900749</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>P.</fn>
<sn>Dobiasch</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.29.230</citeid>
<title>Quantum noise in a dithered-ring-laser gyroscope</title>
<year>1984</year>
<month>1</month>
<DOI>10.1103/PhysRevA.29.230</DOI>
<journal>Phys. Rev. A</journal>
<volume>29</volume>
<publisher>American Physical Society</publisher>
<pages>230--238</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.29.230</file_url>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>C.-S.</fn>
<sn>Cha</sn>
</person>
<person>
<fn>J. D.</fn>
<sn>Cresser</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>inproceedings</bibtype>
<citeid>10.1007/978-1-4757-0605-5_135</citeid>
<title>Quantum Noise in Ring-Laser Gyroscopes</title>
<abstract>The new generation of ring-laser gyroscopes1 can compete with their mechanical counterparts. They can now operate down to a small fraction of earth rotation rate using rings of 1-m diameter, which makes them interesting for tests of metric gravitation theories.2 They have reached a sensitivity where the noise limit is only due to the quantum fluctuations, which arise from spontaneous emission of the laser atoms. Whereas all kinds of mechanical noise can be circumvented by some ``tricky'' techniques, there is no way around the quantum noise, which stems from the quantization of the electric field in the resonator. The final limitation of ring-laser gyroscopes is thus given by the quantum noise.3 Therefore it is important to understand this effect in detail.</abstract>
<year>1984</year>
<isbn>978-1-4757-0605-5</isbn>
<DOI>10.1007/978-1-4757-0605-5_135</DOI>
<booktitle>Coherence and Quantum Optics V</booktitle>
<publisher>Springer US</publisher>
<address>Boston, MA</address>
<editor>L. Mandel and E. Wolf</editor>
<pages>915--922</pages>
<authors>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
<person>
<fn>V.</fn>
<sn>Sanders</sn>
</person>
</authors>
</reference>
<reference>
<bibtype>article</bibtype>
<citeid>PhysRevA.25.2214</citeid>
<title>Quantum noise in ring-laser gyros. I. Theoretical formulation of problem</title>
<year>1982</year>
<month>4</month>
<DOI>10.1103/PhysRevA.25.2214</DOI>
<journal>Phys. Rev. A</journal>
<volume>25</volume>
<publisher>American Physical Society</publisher>
<pages>2214--2225</pages>
<file_url>https://link.aps.org/doi/10.1103/PhysRevA.25.2214</file_url>
<authors>
<person>
<fn>J. D.</fn>
<sn>Cresser</sn>
</person>
<person>
<fn>W. H.</fn>
<sn>Louisell</sn>
</person>
<person>
<fn>P.</fn>
<sn>Meystre</sn>
</person>
<person>
<fn>W.</fn>
<sn>Schleich</sn>
</person>
<person>
<fn>M. O.</fn>
<sn>Scully</sn>
</person>
</authors>
</reference>
</bib>
