DOCSLIB.ORG

Atom Interferometry with Laser-Cooled Lithium by Kayleigh Cassella Doctor of Philosophy in Physics University of California, Berkeley Professor Holger M¨Uller,Chair

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Atom Interferometry with Laser-Cooled Lithium by Kayleigh Cassella Doctor of Philosophy in Physics University of California, Berkeley Professor Holger M¨Uller,Chair Hot Beats and Tune Outs: Atom Interferometry with Laser-cooled Lithium by Kayleigh Cassella A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Physics in the Graduate Division of the University of California, Berkeley Committee in charge: Professor Holger M¨uller,Chair Professor Dan Stamper-Kurn Professor Jeffrey Bokor Spring 2018 Hot Beats and Tune Outs: Atom Interferometry with Laser-cooled Lithium Copyright 2018 by Kayleigh Cassella 1 Abstract Hot Beats and Tune Outs: Atom Interferometry with Laser-cooled Lithium by Kayleigh Cassella Doctor of Philosophy in Physics University of California, Berkeley Professor Holger M¨uller,Chair Ushered forth by advances in time and frequency metrology, atom interferometry remains an indispensable measurement tool in atomic physics due to its precision and versatility. A sequence of four π=2 beam splitter pulses can create either an interferometer sensitive to the atom's recoil frequency when the momentum imparted by the light reverses direction between pulse pairs or, when constructed from pulses without such reversal, sensitive to the perturbing potential from an external optical field. Here, we demonstrate the first atom interferometer with laser-cooled lithium, advantageous for its low mass and simple atomic structure. We study both a recoil-sensitive Ramsey-Bord´einterferometer and interferometry sensitive to the dynamic polarizability of the ground state of lithium. Recoil-sensitive Ramsey-Bord´einterferometry benefits from lithium's high recoil fre- quency, a consequence of its low mass. At an interrogation time of 10 ms, a Ramsey-Bord´e lithium interferometer could achieve sensitivities comparable to those realized at much longer times with heavier alkali atoms. However, in contrast with other atoms that are used for atom interferometry, lithium's unresolved excited-state hyperfine structure precludes the the cycling transition necessary for efficient cooling. Without sub-Doppler cooling techniques. As as result, a lithium atomic gas is typically laser cooled to temperatures around 300 µK, above the Doppler limit, and well above the recoil temperature of 6 µK. This higher tem- perature gas expands rapidly during the operation of an atom interferometer, limiting the experimental interrogation time and preventing spatially resolved detection. In this work, a light-pulse lithium matter-wave interferometer is demonstrated in spite of these limitation. Two-photon Raman interferometer pulses coherently couple the atom's spin and momentum and are thus able to spectrally resolve the outputs. These fast pulses drive conjugate interferometers simultaneously which beat with a fast frequency component proportional to the atomic recoil frequency and an envelope modulated by the two-photon detuning of the Raman transition. We detect the summed signal at short experimental times, preventing perturbation of the signal from vibration noise. This demonstration of a sub-recoil measurement with a super-recoil sample opens the door to similar scheme with other particles that are difficult to trap and cool well, like electrons. 2 An interferometer instead composed of π=2-pulses with a single direction of momentum transfer, can be sensitive to the dynamic polarizability of the atomic ground state. By scanning the frequency of an external driving field, such a measurement can be used to determine the atom's tune-out wavelength. This is the wavelength at which the frequency- dependent polarizability vanishes due to compensating ac-Stark shifts from other atomic states. Lithium's simple atomic structure allows for a precise computation of properties with only ab initio wave functions and spectroscopic data. A direct interferometric measurement of lithium's red tune-out wavelength at 670.971626(1) nm, is a precise comparison to existing `all-order' atomic theory computations. It also provides another way to experimentally determine the S− to P − transitions matrix elements, for which large correlations and small values complicate computations. Finally, a future measurement of lithium's ultraviolet tune- out wavelength of at 324.192(2) nm would be sensitive to relativistic approximations in the atomic structure description. Atom interferometry simultaneously verifies existing atomic theory with measurements of atomic properties and searches for exotic physics lurking in plain sight. The techniques devel- oped here broaden the applicability of interferometry and increase measurement sensitivity by simplifying cooling, increasing atom number and reducing the cycle time. Overcom- ing the current experimental limitations on interrogation time would allow for ultra-precise measurements of both the tune-out wavelength and the fine structure constant. i To my mom and step-dad, who filled me with enough resolve to do hard things. To my sisters, who grew with me and tethered me to real things. To my husband, who unfolded all the crumpled parts of me, again and again. To my children, my greatest teachers, who sprinkled light in all the dark places. I dedicate this work to you. ii Contents Contents ii List of Figures vi List of Tables viii 1 Outward bound 1 1.1 Corpuscular and undulatory . 2 1.1.1 Waves of matter . 4 1.2 α, the fine structure constant . 5 h 1.2.1 M measurement . 8 1.3 α, the polarizability . 8 1.3.1 Dynamic polarizability . 10 1.4 Previous measurements . 12 1.4.1 λto measurement . 13 1.5 Overview of this thesis . 15 2 Atom interferometry 16 2.1 Light off . 19 2.1.1 The free evolution phase . 22 2.2 Light on . 23 2.2.1 Raman scattering . 23 2.2.1.1 Dressed states . 28 2.2.2 The interaction phase . 30 2.2.3 The separation phase . 31 2.3 The total phase . 31 π π π π 2.4 Conjugate interferometers with the 2 - 2 - 2 - 2 . 33 2.5 The Ramsey-Bord´einterferometer . 33 2.5.1 cRBI phase computation . 36 2.6 The copropagating interferometer . 38 2.6.1 cCPI phase computation . 41 iii 3 Lithium, the smallest alkali 42 3.1 Lithium, the lightest alkali . 42 3.2 Lithium, the simplest alkali . 45 3.2.1 The Hylleraas basis . 46 3.3 Dynamic polarizability . 48 3.4 Lukewarm Lithium . 50 3.4.1 Lithium atom interferometry in the space domain . 53 3.5 Advantages of light-pulsed interferometry with lithium . 54 4 Experimental Methods 56 4.1 Lithium Spectroscopy . 58 4.1.1 Modulation Transfer Spectroscopy . 59 4.1.2 The cascade of frequency generation . 62 4.1.2.1 Tapered amplifiers . 63 4.2 Cooling and trapping . 64 4.2.1 2D MOT frequency generation . 67 4.2.2 3D MOT frequency generation . 67 4.2.3 Vacuum system and optics . 68 4.2.3.1 2D MOT chamber . 70 4.2.3.2 3D MOT chamber . 72 4.2.4 Experimental sequence . 73 4.3 State preparation . 74 4.3.1 Frequency generation for optical pumping light . 76 4.3.2 Optical pumping optics . 78 4.3.2.1 Quantization axis . 78 4.4 Interferometry . 78 4.4.1 Frequency generation for Raman beams . 78 4.4.2 Raman optics . 82 4.5 Detection . 83 4.5.1 Absorption imaging . 83 4.5.2 Wollaston prism technique . 84 4.5.3 Time-of-flight imaging . 84 5 Hot Beats 87 5.1 Super-recoil lithium . 87 5.1.1 Large bandwidth pulses . 88 5.1.2 k-reversal . 88 5.2 Simultaneous and conjugate . 89 5.3 Overlapped, simultaneous and conjugate . 91 5.3.1 Hot beats . 92 5.3.2 Time-domain fitting . 92 5.3.3 Frequency-domain fitting . 94 iv 5.4 Phase noise . 95 5.5 Outlook . 97 5.5.1 Vibration immunity . 98 6 Tune-outs 100 6.1 Previous polarizability measurements . 101 6.1.1 The differential Stark shift . 101 6.1.2 Space-domain atom interferometry . 102 6.2 Light-pulsed interferometric lithium tune outs . 103 6.2.1 φto, the tune-out phase . 103 6.2.2 The tune-out beam . 106 6.2.3 Experimental Sequence . 106 6.2.4 Detection & Analysis . 108 6.2.4.1 Principal component analysis . 110 6.3 Towards tune-out . 111 6.3.1 Precision . 111 6.3.1.1 Single-photon scattering . 112 6.3.1.2 Beam shaping . 113 6.3.2 Accuracy . 113 6.4 Hyperfine dynamic polarizabilities . 113 7 Conclusion 117 7.1 Outlook for recoil-sensitive interferometry with super-recoil samples . 117 7.1.1 h=me measurement . 117 7.2 Outlook for tune-out interferometric measurements in lithium . 119 7.2.1 Beyond the red . 119 7.2.2 Investigation of nuclear structure between isotopes . 121 7.3 Atom interferometry with lukewarm lithium . 122 7.3.1 Sisyphus cooling . 123 7.3.2 Gray molasses . 123 7.4 Onward . 123 A Properties of lithium 125 A.1 The level spectrum . 129 A.2 Interaction with static fields . 129 A.3 Interaction with dynamic fields . 131 A.3.1 Reduced Matrix Elements in Atomic Transitions . 131 A.4 Clebsch-Gordan coefficients for D{line transitions . ..
Load more

Recommended publications
  • Atom Interferometry in an Optical Cavity by Matthew Jaffe a Dissertation Submitted in Partial Satisfaction of the Requirements F
    Atom interferometry in an optical cavity by Matthew Jaffe A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Physics in the Graduate Division of the University of California, Berkeley Committee in charge: Associate Professor Holger Müller, Chair Associate Professor Norman Yao Professor Karl van Bibber Fall 2018 Atom interferometry in an optical cavity Copyright 2018 by Matthew Jaffe 1 Abstract Atom interferometry in an optical cavity by Matthew Jaffe Doctor of Philosophy in Physics University of California, Berkeley Associate Professor Holger Müller, Chair Matter wave interferometry with laser pulses has become a powerful tool for precision measurement. Optical resonators, meanwhile, are an indispensable tool for control of laser beams. We have combined these two components, and built the first atom interferometer inside of an optical cavity. This apparatus was then used to examine interactions between atoms and a small, in-vacuum source mass. We measured the gravitational attraction to the source mass, making it the smallest source body ever probed gravitationally with an atom interferometer. Searching for additional forces due to screened fields, we tightened constraints on certain dark energy models by several orders of magnitude. Finally, we measured a novel force mediated by blackbody radiation for the first time. Utilizing technical benefits of the cavity, we performed interferometry with adiabatic passage. This enabled new interferometer geometries, large momentum transfer, and in- terferometers with up to one hundred pulses. Performing a trapped interferometer to take advantage of the clean wavefronts within the optical cavity, we performed the longest du- ration spatially-separated atom interferometer to date: over ten seconds, after which the atomic wavefunction was coherently recombined and read out as interference to measure gravity.
    [Show full text]
  • An Interferometer for Atoms by David William Keith B.Sc Physics
    1 An Interferometer for Atoms by David William Keith B.Sc Physics, University of Toronto (Nov, 1986) Submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Doctor of Philosophy at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY May, 1991 © Massachusetts Institute of Technology, 1991 Signature of the Author ______________________________________________ Department of Physics May , 1991 Certified by ________________________________________________________ David E. Pritchard Professor of Physics Thesis Supervisor Accepted by _______________________________________________________ George F. Koster, Chairman, Department Committee on Graduate Studies 2 An Interferometer for Atoms by David William Keith Submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Doctor of Philosophy Abstract We have demonstrated an interferometer for atoms. A three grating geometry is used, resulting in an interferometer of the "amplitude division " type. We used a highly collimated beam of sodium atoms with a de Broglie wavelength of 16 pm and high-quality 0.4 mm-period free-standing gratings. The interference signal is 70 Hz, which allows us to determine the phase to 0.1 rad in 1 min. This is the first atom interferometer in the sense that it simultaneously and distinctly separates the atoms in position and momentum. In order to make the gratings for our interferometer, we have developed a novel method for fabricating free-standing micro-structures. Using this method we have made high-quality 0.2 and 0.4-mm period gratings, as well as the first zone plate lenses to be used for atoms. We have previously reported the first observation of the diffraction of atoms from a fabricated periodic structure.
    [Show full text]
  • MATTER WAVE INTERFEROMETRY in the Light of Schridinger's Wave Mechanics
    INIS-mf—11327 ATOMINSTITUT WIEN INTERNATIONAL WORKSHOP ON "SchrBdingtr'i cat* M m qrmbol for the wftrt-putieU dualiim MATTER WAVE INTERFEROMETRY in the Light of Schridinger's Wave Mechanics 14.-16. September 1987, Technical University Vienna Atominstitut der Osterreichischen Universitaten Satellite Workshop to the SCHRODINGER SYMPOSIUM which will be held in Vienna 16.-18. September 1987 on the occasion of the 100th ANNIVERSARY OF E. SCHROWNGER'S BIRTH organized by ATOMINSTmjT DER OSTERREICHISCHEN UNIVERSITATEN iad EftWIN SCHRODINGER SOCIETY urr Tentative Program Abstract Booklet INTERNATIONAL WORKSHOP ON "SchrSdinger'j cat" as a symbol for the wave-particle dualism MATTER WAVE INTERFEROMETRY in the Light of SchrOdinger's Wave Mechanics 14.-16. September 1987, Technical University Vienna Atominstitut der Osterreichischen Universitaten Satellite Workshop to the SCHRODINGER SYMPOSIUM which will be held in Vienna 16.-18. September 1987 on the occasion of the 100th ANNIVERSARY OF E. SCHRODINGER'S BIRTH organized by ATOMINSTITUT DER OSTERREICHISCHEN UNIVERSITATEN and ERWIN SCHRODINGER SOCIETY International Advisory Committee: U.Bonse (Dortmund), I.M.Frank (Dubna), A.G.Klein (Melbourne), D.M.Greenberger (New York), H.Maier-Leibnitz (Munchen), G.MOllenstedt (Tubingen), M.Namiki (Tokyo), CCShull (Cambridge), A.Tonomura (Tokyo), J.-P.Vigier (Paris), S.A.Weraer (Columbia). Organizing Committee: G.Badurek, F.Paschke, H.Rauch (chairman), J.Summhammer, A.Zeilinger Topics: Electron Interferometry Quantum Devices Neutron Interferometry Interpretational
    [Show full text]
  • Arxiv:1806.09958V3 [Physics.Ed-Ph] 1 Aug 2018 1
    Understanding quantum physics through simple experiments: from wave-particle duality to Bell's theorem Ish Dhand,1 Adam D'Souza,2 Varun Narasimhachar,3 Neil Sinclair,4, 5 Stephen Wein,4 Parisa Zarkeshian,4 Alireza Poostindouz,4, 6 and Christoph Simon4, ∗ 1Institut f¨urTheoretische Physik and Center for Integrated Quantum Science and Technology (IQST), Albert-Einstein-Allee 11, Universit¨atUlm, 89069 Ulm, Germany 2Department of Community Health Sciences, Cumming School of Medicine, University of Calgary, Calgary T2N4N1, Alberta, Canada 3School of Physical & Mathematical Sciences, Nanyang Technological University, 21 Nanyang Link Singapore 637371 4Department of Physics and Astronomy and Institute for Quantum Science and Technology (IQST), University of Calgary, Calgary T2N1N4, Alberta, Canada 5Department of Physics, Mathematics, and Astronomy and Alliance for Quantum Technologies (AQT), California Institute of Technology, 1200 East California Blvd., Pasadena, California 91125, USA 6Department of Computer Science, University of Calgary, Calgary T2N1N4, Alberta, Canada (Dated: August 3, 2018) Quantum physics, which describes the strange behavior of light and matter at the smallest scales, is one of the most successful descriptions of reality, yet it is notoriously inaccessible. Here we provide an approachable explanation of quantum physics using simple thought experiments. We derive all relevant quantum predictions using minimal mathematics, without introducing the advanced calculations that are typically used to describe quantum physics. We focus on the two key surprises of quantum physics, namely wave{particle duality, a term that was introduced to capture the fact that single quantum particles in some respects behave like waves and in other respects like particles, and entanglement, which applies to two or more quantum particles and brings out the inherent contradiction between quantum physics and seemingly obvious assumptions regarding the nature of reality.
    [Show full text]
  • Electron Interferometry: Interferences Between Two Electrons and a Precision Method of Measuring Decoherence
    Annales de la Fondation Louis de Broglie, Volume 29, Hors s´erie1, 2004 857 Electron interferometry: Interferences between two electrons and a precision method of measuring decoherence Franz Hasselbach, Harald Kiesel, and Peter Sonnentag Institut f¨urAngewandte Physik, Universit¨atT¨ubingen, Auf der Morgenstelle 10, D-72076 T¨ubingen,Germany ABSTRACT. Louis de Broglie’s discovery of the wave nature of matter 80 years ago and the subsequent development of quantum mechanics by Erwin Schr¨odinger, Werner Heisenberg and Paul Dirac solved many riddles of those days and determined physics of the whole 20th century. Yet, after this long time, matter wave interferometry is as up to date as it was in 1927 when Louis de Broglie’s hypothesis was verified, e.g., by Davisson and Germer. Atom interferometry, ion interferometry and Bose-Einstein condensates are today’s fascinating applications based on de Broglie’s discovery. The focus of the present contribution are Hanbury Brown-Twiss anti-correlations (i.e. interferences between two fermions (electrons)) and the quantitative observation of decoherence by electron biprism interferometry. P.A.C.S.: 03.75.-b; 05.30.Fk; 03.65.Yz 1 Observation of Hanbury Brown-Twiss anticorrelations in a beam of free electrons The astronomers R. Hanbury Brown and R.Q. Twiss (HBT) were the first to observe in 1956 that the fluctuations in the counting rate of photons originating from uncorrelated point sources become, within the coherently illuminated area, slightly enhanced compared to a random sequence of classical particles [1, 2, 3]. This at a first glance mysterious formation of correlations in the process of propagation turns out to be a consequence of quantum interference between two indistinguishable pho- tons and Bose-Einstein statistics.
    [Show full text]
  • The Double-Slit Experiment - Physicsworld.Com
    The double-slit experiment - physicsworld.com http://physicsworld.com/cws/article/print/9745 A website from the Institute of Physics Signed in as ianappelbaum My profile Sign out Contact us The double-slit experiment Share this Sep 1, 2002 E-mail to a friend This article is an extended version of the article “The Connotea double-slit experiment” that appeared in the September CiteUlike 2002 issue of Physics World (p15). It has been further Delicious extended to include three letters about the history of the Digg double-slit experiment with single electrons that were Facebook published in the May 2003 issue of the magazine. Twitter What is the most beautiful experiment in physics? This is the question that Robert Crease asked Physics World readers in May - and more than 200 replied with suggestions as diverse as Schrödinger's cat and the Trinity nuclear test in 1945. The top five Related stories included classic experiments by Galileo, Millikan, Newton and The most beautiful Thomas Young. But uniquely among the top 10, the most beautiful experiment (survey) experiment in physics - Young's double-slit experiment applied to the From the New York Times : interference of single electrons - does not have a name associated Science's 10 most beautiful with it. experiments (abstract only) Most discussions of double-slit experiments with particles refer to The most beautiful Feynman's quote in his lectures: "We choose to examine a experiment (results) phenomenon which is impossible, absolutely impossible, to explain in any classical way, and which has in it the heart of quantum Related links mechanics.
    [Show full text]
  • Gravitational and Aharonov-Bohm Phases in Neutron Interferometry
    Gravitational and Aharonov-Bohm Phases in Neutron Interferometry Dissertation zur Erlangung des Grades eines Doktors der Naturwissenschaften eingereicht von Gerbrand van der Zouw, M.Sc. durchgef¨uhrtam Institut f¨urExperimentalphysik der Universit¨atWien bei o. Univ. Prof. Dr. Anton Zeilinger Diese Arbeit wurde durch den Fond zur F¨orderungwissenschaftlicher Forschung (Projekt S6503) und durch die Europ¨aische Union (TMR Network No. ERB-FMRX-CT96-0057) unterst¨utzt. Copyright c 2000 by G. van der Zouw All rights reserved. No part of this publication may be reproduced, stored in a retrieval system or transmitted in any form or by any means, electronic, mechanical, photocopying, recording or otherwise, without the prior written permission of the author. v Abstract This thesis describes two experiments with the interferometer for very-cold-neutrons (VCN) at the Institut Laue-Langevin in Grenoble, France. This interferometer operates with neu- trons that are 40 m/s slow and uses micro-fabricated phase gratings as beam-splitters. The first experiment is a demonstration of the scalar neutron Aharonov-Bohm (AB) effect, which is the neutron analogue of the electrostatic AB effect for electrons. Aharonov and Bohm (1959) proposed this latter effect together with the magnetic AB effect to clar- ify the significance of electromagnetic potentials in quantum mechanics. The experiment described here focuses at for the first time simultaneously demonstrating the two essen- tial operational signatures of all AB-type effects: their nondispersivity, i.e. wavelength independence, and the fact that they are are not locally observable in a simply connected space-time. In this thesis it will be shown, as was already pointed out by Zeilinger (1984, 1986), that the neutron analogue also has both signatures and thus can be used to demon- strate them.
    [Show full text]
  • Selected Topics in Charged Particle Interferometry
    Scanning Microscopy Vol. 11, 1997 (Pages 345-366) 0891-7035/97$5.00+.25 Scanning Microscopy International, Chicago (AMFCharged O’Hare), particle IL 60666 interferometry USA SELECTED TOPICS IN CHARGED PARTICLE INTERFEROMETRY Franz Hasselbach Institut für Angewandte Physik der Universität Tübingen, Tübingen, Germany Abstract Introduction Following a short survey on the early developments Early developments in particle diffraction, in particle diffraction, interferometry and holography, the interferometry and holography constructional details and advantages of our novel Diffraction and interferometry of particles, especial- miniaturized low voltage biprism interferometer are ly of electrons, have been firmly established for the past presented. As a unique electron optical component in an seventy years. As early as 1925, Elsasser [34] realized that interferometer, a crossed field analyzer (Wien-filter) is in single crystals, nature provided us with almost perfectly included in the beam path. Inside the crossed field analyzer aligned interferometers for matter waves. Experimental the wave packets propagate on laterally separated paths of difficulties caused a two year delay between his suggestion different electric potential and in turn with different group and realization in the experiment in 1927 by Davisson and velocities provoking a relative longitudinal shift along the Germer [26]. For their diffraction experiment with electrons, beam path of the self interfering two wave packets at the periodically arranged nickel atoms of a single crystal were exit plane of the crossed field analyzer. The value of this used. It was the first experimental proof of the wave particle shift can be chosen to any extent desired by varying of its duality hypothesis established theoretically in duc de excitation.
    [Show full text]
  • Data Transmission by Quantum Matter Wave Modulation
    Lawrence Berkeley National Laboratory Recent Work Title Data transmission by quantum matter wave modulation Permalink https://escholarship.org/uc/item/9r5522zj Journal New Journal of Physics, 23(2) ISSN 1367-2630 Authors Röpke, R Kerker, N Stibor, A Publication Date 2021-02-01 DOI 10.1088/1367-2630/abe15f Peer reviewed eScholarship.org Powered by the California Digital Library University of California PAPER • OPEN ACCESS Data transmission by quantum matter wave modulation To cite this article: R Röpke et al 2021 New J. Phys. 23 023038 View the article online for updates and enhancements. This content was downloaded from IP address 73.202.150.227 on 10/03/2021 at 22:56 New J. Phys. 23 (2021) 023038 https://doi.org/10.1088/1367-2630/abe15f PAPER Data transmission by quantum matter wave modulation OPEN ACCESS RRöpke1,NKerker1 and A Stibor1,2,∗ RECEIVED 1 + 30 October 2020 Institute of Physics and LISA , University of Tübingen, Tübingen, Germany 2 Lawrence Berkeley National Lab, Molecular Foundry, Berkeley, United States of America REVISED ∗ Author to whom any correspondence should be addressed. 25 January 2021 E-mail: [email protected] ACCEPTED FOR PUBLICATION 29 January 2021 Keywords: communication, quantum modulation, interferometry, electron, Wien filter, secure data transfer, matter wave PUBLISHED 23 February 2021 Abstract Original content from this work may be used Classical communication schemes exploiting wave modulation are the basis of our information under the terms of the Creative Commons era. Quantum information techniques with photons enable future secure data transfer in the dawn Attribution 4.0 licence. of decoding quantum computers. Here we demonstrate that also matter waves can be applied for Any further distribution secure data transfer.
    [Show full text]
  • Arxiv:2001.06154V1 [Quant-Ph] 17 Jan 2020 Tion
    Quantum decoherence by Coulomb interaction N. Kerker1, R. R¨opke1, L.M. Steinert1, A. Pooch1 and A. Stibor1;2∗ 1Institute of Physics and Center for Collective Quantum Phenomena in LISA+, University of T¨ubingen,T¨ubingen,Germany 2Lawrence Berkeley National Lab, Molecular Foundry, Berkeley, USA, *email: [email protected] The performance of modern quantum devices in communication, metrology or microscopy relies on the quantum-classical interaction which is generally described by the theory of decoherence. Despite the high relevance for long coherence times in quantum electronics, decoherence mechanisms mediated by the Coulomb force are not well understood yet and several competing theoretical models exist. Here, we present an experimental study of the Coulomb-induced decoherence of free electrons in a superposition state in a biprism electron interferometer close to a semiconducting and metallic surface. The decoherence was determined through a contrast loss at different beam path separations, surface distances and conductibilities. To clarify the current literature discussion, four theoretical models were compared to our data. We could rule out three of them and got good agreement with a theory based on macroscopic quantum electrodynamics. The results will enable the determination and minimization of specific decoherence channels in the design of novel quantum instruments. Introduction.{ A deep understanding of the transition C70 fullerene molecules, were laser excitation [14] or col- region between a quantum and a classical system is nec- lisions with gas atoms [13] led to decoherence. essary for various fields of physics and technical applica- In all these cases the quantum object was neutral. To tions. Decoherence, being the loss of quantum behaviour determine the role of decoherence by Coulomb interac- is described by a variety of theoretical approaches [1{ tion, an experiment was proposed by Anglin et al.
    [Show full text]
  • High Contrast Measurements with a Bose-Einstein Condensate Atom Interferometer
    High Contrast Measurements with a Bose-Einstein Condensate Atom Interferometer Billy Ian Robertson Experimental Quantum Optics and Photonics Group Department of Physics and SUPA University of Strathclyde A thesis presented in the fulfilment of the requirements for the degree of Doctor of Philosophy 2016 This thesis is the result of the authors original research. It has been composed by the author and has not been previously submitted for examination which has led to the award of a degree. The copyright of this thesis belongs to the author under the terms of the United Kingdom Copyright Acts as qualified by University of Strathclyde Regulation 3.50. Due acknowledgement must always be made of the use of any material contained in, or derived from, this thesis. Signed: Date: i Abstract Atom interferometry is a next-generation technique of precision measurement that can vastly outperform its optical analogue. These devices utilise the wave nature of atoms to make interferometric measurements of, for example, gravitational and magnetic fields, inertial effects, and the fine-structure constant. The main focus of this thesis is the creation of a general purpose atom interferometer in free space. We create a Bose-Einstein condensate of ∼105 87Rb atoms in a crossed-optical dipole trap. The atomic wavefunction is coherently manipulated using highly tuned pulses comprising off-resonant light that form our atom-optical elements. These atom optics are analogous to the beam splitters and mirrors in an optical interferometer. By controlling the timing and amplitude of the pulses we demonstrate the ability to excite specific momentum states with high efficiency.
    [Show full text]
  • Optics and Interferometry with Atoms and Molecules
    Optics and interferometry with atoms and molecules The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Cronin, Alexander D., Jörg Schmiedmayer, and David E. Pritchard. “Optics and interferometry with atoms and molecules.” Reviews of Modern Physics 81.3 (2009): 1051. © 2009 The American Physical Society As Published http://dx.doi.org/10.1103/RevModPhys.81.1051 Publisher American Physical Society Version Final published version Citable link http://hdl.handle.net/1721.1/52372 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. REVIEWS OF MODERN PHYSICS, VOLUME 81, JULY–SEPTEMBER 2009 Optics and interferometry with atoms and molecules Alexander D. Cronin* Department of Physics, University of Arizona, Tucson, Arizona 85721, USA Jörg Schmiedmayer† Atominstitut Österreichischen Universitäten, TU-Wien, Austria David E. Pritchard‡ Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA ͑Published 28 July 2009͒ Interference with atomic and molecular matter waves is a rich branch of atomic physics and quantum optics. It started with atom diffraction from crystal surfaces and the separated oscillatory fields technique used in atomic clocks. Atom interferometry is now reaching maturity as a powerful art with many applications in modern science. In this review the basic tools for coherent atom optics are described including diffraction by nanostructures and laser light, three-grating interferometers, and double wells on atom chips. Scientific advances in a broad range of fields that have resulted from the application of atom interferometers are reviewed.
    [Show full text]