Photonic Materials in Circuit Quantum Electrodynamics
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Time Quasilattices in Dissipative Dynamical Systems Abstract Contents
SciPost Phys. 5, 001 (2018) Time quasilattices in dissipative dynamical systems Felix Flicker1,2 1 Rudolph Peierls Centre for Theoretical Physics, University of Oxford, Department of Physics, Clarendon Laboratory, Parks Road, Oxford, OX1 3PU, UK 2 Department of Physics, University of California, Berkeley, California 94720 USA fl[email protected] Abstract We establish the existence of ‘time quasilattices’ as stable trajectories in dissipative dy- namical systems. These tilings of the time axis, with two unit cells of different durations, can be generated as cuts through a periodic lattice spanned by two orthogonal directions of time. We show that there are precisely two admissible time quasilattices, which we term the infinite Pell and Clapeyron words, reached by a generalization of the period- doubling cascade. Finite Pell and Clapeyron words of increasing length provide system- atic periodic approximations to time quasilattices which can be verified experimentally. The results apply to all systems featuring the universal sequence of periodic windows. We provide examples of discrete-time maps, and periodically-driven continuous-time dy- namical systems. We identify quantum many-body systems in which time quasilattices develop rigidity via the interaction of many degrees of freedom, thus constituting dissi- pative discrete ‘time quasicrystals’. Copyright F. Flicker. Received 30-10-2017 This work is licensed under the Creative Commons Accepted 15-06-2018 Check for Attribution 4.0 International License. Published 03-07-2018 updates Published -
Dynamical Control of Matter Waves in Optical Lattices Sune Schøtt
Aarhus University Faculty of Science Department of Physics and Astronomy PhD Thesis Dynamical Control of Matter Waves in Optical Lattices by Sune Schøtt Mai November 2010 This thesis has been submitted to the Faculty of Science at Aarhus Uni- versity in order to fulfill the requirements for obtaining a PhD degree in physics. The work has been carried out under the supervision of profes- sor Klaus Mølmer and associate professor Jan Arlt at the Department of Physics and Astronomy. Contents Contents i 1 Introduction 3 1.1 Thesis Outline .......................... 3 1.2 Bose-Einstein Condensation .................. 4 2 Experimental Setup and Methods 9 2.1 Overview ............................. 9 2.2 Magneto-Optic Trap and Optical Pumping .......... 9 2.3 Transport with Movable Quadrupole Traps . 13 2.4 Evaporative Cooling ...................... 14 2.5 Absorption Imaging ....................... 15 3 Optical Lattices 17 3.1 Introduction ........................... 17 3.2 AC Stark-shift Induced Potentials . 18 3.2.1 Classical and Semi-Classical Approaches . 18 3.2.2 Dressed State Picture . 20 3.3 Lattice Band Structure ..................... 22 3.3.1 Reciprocal Space Bloch Theorem . 23 3.3.2 The 1D Lattice Band-Structure . 23 4 Lattice Calibration Techniques 27 4.1 Introduction ........................... 27 4.2 Kapitza-Dirac Scattering .................... 28 4.3 Bloch Oscillation and LZ-Tunneling . 30 4.3.1 Bloch Oscillation .................... 31 4.3.2 Landau-Zener Theory . 31 i ii CONTENTS 4.3.3 Experimental Verification of the Landau-Zener Model 32 4.4 Lattice Modulation ....................... 35 4.5 Summary ............................ 35 5 Dynamically Controlled Lattices 39 5.1 Introduction ........................... 39 5.2 Overview ............................. 39 5.3 Controlled Matter Wave Beam Splitter . -
Arxiv:2005.03138V2 [Cond-Mat.Quant-Gas] 23 May 2020 Contents
Condensed Matter Physics in Time Crystals Lingzhen Guo1 and Pengfei Liang2;3 1Max Planck Institute for the Science of Light (MPL), Staudtstrasse 2, 91058 Erlangen, Germany 2Beijing Computational Science Research Center, 100193 Beijing, China 3Abdus Salam ICTP, Strada Costiera 11, I-34151 Trieste, Italy E-mail: [email protected] Abstract. Time crystals are physical systems whose time translation symmetry is spontaneously broken. Although the spontaneous breaking of continuous time- translation symmetry in static systems is proved impossible for the equilibrium state, the discrete time-translation symmetry in periodically driven (Floquet) systems is allowed to be spontaneously broken, resulting in the so-called Floquet or discrete time crystals. While most works so far searching for time crystals focus on the symmetry breaking process and the possible stabilising mechanisms, the many-body physics from the interplay of symmetry-broken states, which we call the condensed matter physics in time crystals, is not fully explored yet. This review aims to summarise the very preliminary results in this new research field with an analogous structure of condensed matter theory in solids. The whole theory is built on a hidden symmetry in time crystals, i.e., the phase space lattice symmetry, which allows us to develop the band theory, topology and strongly correlated models in phase space lattice. In the end, we outline the possible topics and directions for the future research. arXiv:2005.03138v2 [cond-mat.quant-gas] 23 May 2020 Contents 1 Brief introduction to time crystals3 1.1 Wilczek's time crystal . .3 1.2 No-go theorem . .3 1.3 Discrete time-translation symmetry breaking . -
Creating Big Time Crystals with Ultracold Atoms
New J. Phys. 22 (2020) 085004 https://doi.org/10.1088/1367-2630/aba3e6 PAPER Creating big time crystals with ultracold atoms OPEN ACCESS Krzysztof Giergiel1,TienTran2, Ali Zaheer2,ArpanaSingh2,AndreiSidorov2,Krzysztof RECEIVED 1 2 1 April 2020 Sacha and Peter Hannaford 1 Instytut Fizyki Teoretycznej, Universytet Jagiellonski, ulica Profesora Stanislawa Lojasiewicza 11, PL-30-348 Krakow, Poland REVISED 2 23 June 2020 Optical Sciences Centre, Swinburne University of Technology, Hawthorn, Victoria 3122, Australia ACCEPTED FOR PUBLICATION E-mail: [email protected] and [email protected] 8 July 2020 PUBLISHED Keywords: time crystals, Bose–Einstein condensate, ultracold atoms 17 August 2020 Original content from Abstract this work may be used under the terms of the We investigate the size of discrete time crystals s (ratio of response period to driving period) that Creative Commons Attribution 4.0 licence. can be created for a Bose–Einstein condensate (BEC) bouncing resonantly on an oscillating Any further distribution mirror. We find that time crystals can be created with sizes in the range s ≈ 20–100 and that such of this work must maintain attribution to big time crystals are easier to realize experimentally than a period-doubling (s=2) time crystal the author(s) and the because they require either a larger drop height or a smaller number of bounces on the mirror. We title of the work, journal citation and DOI. also investigate the effects of having a realistic soft Gaussian potential mirror for the bouncing BEC, such as that produced by a repulsive light-sheet, which is found to make the experiment easier to implement than a hard-wall potential mirror. -
Scalability and High-Efficiency of an $(N+ 1) $-Qubit Toffoli Gate Sphere
Scalability and high-efficiency of an (n + 1)-qubit Toffoli gate sphere via blockaded Rydberg atoms Dongmin Yu1, Yichun Gao1, Weiping Zhang2,3, Jinming Liu1 and Jing Qian1,3,† 1State Key Laboratory of Precision Spectroscopy, Department of Physics, School of Physics and Electronic Science, East China Normal University, Shanghai 200062, China 2Department of Physics and Astronomy, Shanghai Jiaotong University and Tsung-Dao Lee Institute, Shanghai 200240, China and 3Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, Shanxi 030006, China∗ The Toffoli gate serving as a basic building block for reversible quantum computation, has man- ifested its great potentials in improving the error-tolerant rate in quantum communication. While current route to the creation of Toffoli gate requires implementing sequential single- and two-qubit gates, limited by longer operation time and lower average fidelity. We develop a new theoretical protocol to construct a universal (n + 1)-qubit Toffoli gate sphere based on the Rydberg blockade mechanism, by constraining the behavior of one central target atom with n surrounding control atoms. Its merit lies in the use of only five π pulses independent of the control atom number n which leads to the overall gate time as fast as 125ns and the average fidelity closing to 0.999. The maximal filling number of control atoms can be∼ up to n = 46, determined by the spherical diame- ter which is equal to the blockade radius, as well as by the nearest neighbor spacing between two trapped-atom lattices. Taking n = 2, 3, 4 as examples we comparably show the gate performance with experimentally accessible parameters, and confirm that the gate errors mainly attribute to the imperfect blockade strength, the spontaneous atomic loss and the imperfect ground-state prepa- ration. -
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Arxiv:2007.08348V3
Dynamical transitions and critical behavior between discrete time crystal phases 1 1,2, Xiaoqin Yang and Zi Cai ∗ 1Wilczek Quantum Center and Key Laboratory of Artificial Structures and Quantum Control, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China 2Shanghai Research Center for Quantum Sciences, Shanghai 201315, China In equilibrium physics, spontaneous symmetry breaking and elementary excitation are two con- cepts closely related with each other: the symmetry and its spontaneous breaking not only control the dynamics and spectrum of elementary excitations, but also determine their underlying struc- tures. In this paper, based on an exactly solvable model, we propose a phase ramping protocol to study an excitation-like behavior of a non-equilibrium quantum matter: a discrete time crystal phase with spontaneous temporal translational symmetry breaking. It is shown that slow ramp- ing could induce a dynamical transition between two Z2 symmetry breaking time crystal phases in time domain, which can be considered as a temporal analogue of the soliton excitation spacially sandwiched by two degenerate charge density wave states in polyacetylene. By tuning the ramping rate, we observe a critical value at which point the transition duration diverges, resembling the critical slowing down phenomenon in nonequilibrium statistic physics. We also discuss the effect of stochastic sequences of such phase ramping processes and its implication to the stability of the discrete time crystal phase against noisy perturbations. Usually, the ground state energy of an equilibrium sys- question is how to generalize such an idea into the non- tem does not have much to do with its observable behav- equilibirum quantum matters with intriguing SSB absent ior. -
Chapter 5. Atoms in Optical Lattices
Strongly correlated systems in atomic and condensed matter physics Lecture notes for Physics 284 by Eugene Demler Harvard University September 18, 2014 2 Chapter 5 Atoms in optical lattices Optical lattices provide a powerful tool for creating strongly correlated many- body systems of ultracold atoms. By choosing different lattice geometries one can obtain very different single particle dispersions. The ratio of the interaction and kinetic energies can be controlled by tuning the depth of the lattice. 5.1 Noninteracting particles in optical lattices The simplest possible periodic optical potential is formed by overlapping two counter-propagating beams. Electric field in the resulting standing wave is E(z) = E0 sin(kz + θ) cos !t (5.1) Here k = 2π/λ is the wavevector of the laser light. Following the general recipe for AC Stark effects, we calculate electric dipolar moments induced by this field in the atoms, calculate interaction between dipolar moments and the electric field, and average over fast optical oscillations (see chapter ??). The result is the potential 2 V (z) = −V0 sin (kz + θ) (5.2) 2 where V0 = α(!)E0 =2, with α(!) being polarizability. It is common to express 2 2 V0 in units of the recoil energy Er = ~ k =2m. In real experiments one also needs to take into account the transverse profile of the beam. Hence V (r?; z) = exp{−2r2=w2(z)g×V (z). In most experiments the main effect of the transverse profile is only to renormalize the parabolic confining potentia. Combining three perpendicular sets of standing waves we get a simple cubic lattice V (r) = −Vx 0 cosqxx − Vy 0 cosqyy − Vz 0 cosqzz (5.3) 3 4 CHAPTER 5. -
Self-Peeling of Impacting Droplets
LETTERS PUBLISHED ONLINE: 11 SEPTEMBER 2017 | DOI: 10.1038/NPHYS4252 Self-peeling of impacting droplets Jolet de Ruiter†, Dan Soto† and Kripa K. Varanasi* Whether an impacting droplet1 sticks or not to a solid formation, 10 µs, is much faster than the typical time for the droplet surface has been conventionally controlled by functionalizing to completely crash22, 2R=v ∼1ms. These observations suggest that the target surface2–8 or by using additives in the drop9,10. the number of ridges is set by a local competition between heat Here we report on an unexpected self-peeling phenomenon extraction—leading to solidification—and fluid motion—opposing that can happen even on smooth untreated surfaces by it through local shear, mixing, and convection (see first stage of taking advantage of the solidification of the impacting drop sketch in Fig. 2c). We propose that at short timescales (<1 ms, and the thermal properties of the substrate. We control top row sketch of Fig. 2c), while the contact line of molten tin this phenomenon by tuning the coupling of the short- spreads outwards, a thin liquid layer in the immediate vicinity of timescale fluid dynamics—leading to interfacial defects upon the surface cools down until it forms a solid crust. At that moment, local freezing—and the longer-timescale thermo-mechanical the contact line pins, while the liquid above keeps spreading on a stresses—leading to global deformation. We establish a regime thin air film squeezed underneath. Upon renewed touchdown of map that predicts whether a molten metal drop impacting the liquid, a small air ridge remains trapped, forming the above- onto a colder substrate11–14 will bounce, stick or self-peel. -
Veselago Lensing with Ultracold Atoms in an Optical Lattice
ARTICLE Received 9 Dec 2013 | Accepted 27 Jan 2014 | Published 14 Feb 2014 DOI: 10.1038/ncomms4327 Veselago lensing with ultracold atoms in an optical lattice Martin Leder1, Christopher Grossert1 & Martin Weitz1 Veselago pointed out that electromagnetic wave theory allows for materials with a negative index of refraction, in which most known optical phenomena would be reversed. A slab of such a material can focus light by negative refraction, an imaging technique strikingly different from conventional positive refractive index optics, where curved surfaces bend the rays to form an image of an object. Here we demonstrate Veselago lensing for matter waves, using ultracold atoms in an optical lattice. A relativistic, that is, photon-like, dispersion relation for rubidium atoms is realized with a bichromatic optical lattice potential. We rely on a Raman p-pulse technique to transfer atoms between two different branches of the dispersion relation, resulting in a focusing that is completely analogous to the effect described by Veselago for light waves. Future prospects of the demonstrated effects include novel sub-de Broglie wavelength imaging applications. 1 Institut fu¨r Angewandte Physik der Universita¨t Bonn, Wegelerstrae 8, 53115 Bonn, Germany. Correspondence and requests for materials should be addressed to M.W. (email: [email protected]). NATURE COMMUNICATIONS | 5:3327 | DOI: 10.1038/ncomms4327 | www.nature.com/naturecommunications 1 & 2014 Macmillan Publishers Limited. All rights reserved. ARTICLE NATURE COMMUNICATIONS | DOI: 10.1038/ncomms4327 eselago lensing is a concept based on negative of spatial periodicity l/4, generated by the dispersion of multi- refraction1–3, where a spatially diverging pencil of rays photon Raman transitions17. -
Time-Domain Grating with a Periodically Driven Qutrit
PHYSICAL REVIEW APPLIED 11, 014053 (2019) Time-Domain Grating with a Periodically Driven Qutrit Yingying Han,1,2,3,§ Xiao-Qing Luo,2,3,§ Tie-Fu Li,4,2,* Wenxian Zhang,1,† Shuai-Peng Wang,2 J.S. Tsai,5,6 Franco Nori,5,7 and J.Q. You3,2,‡ 1 School of Physics and Technology, Wuhan University, Wuhan, Hubei 430072, China 2 Quantum Physics and Quantum Information Division, Beijing Computational Science Research Center, Beijing 100193, China 3 Interdisciplinary Center of Quantum Information and Zhejiang Province Key Laboratory of Quantum Technology and Device, Department of Physics and State Key Laboratory of Modern Optical Instrumentation, Zhejiang University, Hangzhou 310027, China 4 Institute of Microelectronics, Department of Microelectronics and Nanoelectronics, and Tsinghua National Laboratory of Information Science and Technology, Tsinghua University, Beijing 100084, China 5 Theoretical Quantum Physics Laboratory, RIKEN Cluster for Pioneering Research, Wako-shi, Saitama 351-0198, Japan 6 Department of Physic, Tokyo University of Science, Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan 7 Department of Physics, The University of Michigan, Ann Arbor, Michigan 48109-1040, USA (Received 23 October 2018; revised manuscript received 3 December 2018; published 28 January 2019) Physical systems in the time domain may exhibit analogous phenomena in real space, such as time crystals, time-domain Fresnel lenses, and modulational interference in a qubit. Here, we report the experi- mental realization of time-domain grating using a superconducting qutrit in periodically modulated probe and control fields via two schemes: simultaneous modulation and complementary modulation. Both exper- imental and numerical results exhibit modulated Autler-Townes (AT) and modulation-induced diffraction (MID) effects. -
Three-Component Fermions with Surface Fermi Arcs in Tungsten Carbide
LETTERS https://doi.org/10.1038/s41567-017-0021-8 Three-component fermions with surface Fermi arcs in tungsten carbide J.-Z. Ma 1,2, J.-B. He1,3, Y.-F. Xu1,2, B. Q. Lv1,2, D. Chen1,2, W.-L. Zhu1,2, S. Zhang1, L.-Y. Kong 1,2, X. Gao1,2, L.-Y. Rong2,4, Y.-B. Huang 4, P. Richard1,2,5, C.-Y. Xi6, E. S. Choi7, Y. Shao1,2, Y.-L. Wang 1,2,5, H.-J. Gao1,2,5, X. Dai1,2,5, C. Fang1, H.-M. Weng 1,5, G.-F. Chen 1,2,5*, T. Qian 1,5* and H. Ding 1,2,5* Topological Dirac and Weyl semimetals not only host quasi- bulk valence and conduction bands, which are protected by the two- particles analogous to the elementary fermionic particles in dimensional (2D) topological properties on time-reversal invariant high-energy physics, but also have a non-trivial band topol- planes in the Brillouin zone (BZ)24,26. ogy manifested by gapless surface states, which induce In addition to four- and two-fold degeneracy, it has been shown exotic surface Fermi arcs1,2. Recent advances suggest new that space-group symmetries in crystals may protect other types of types of topological semimetal, in which spatial symmetries degenerate point, near which the quasiparticle excitations are not protect gapless electronic excitations without high-energy the analogues of any elementary fermions described in the standard analogues3–11. Here, using angle-resolved photoemission model. Theory has proposed three-, six- and eight-fold degener- spectroscopy, we observe triply degenerate nodal points near ate points at high-symmetry momenta in the BZ in several specific the Fermi level of tungsten carbide with space group P 62m̄ non-symmorphic space groups3,4,10,11, where the combination of non- (no.