PT -symmetric circuit QED

A parity-time (PT)-symmetric system emerging from a quantum dynamics is highly desirable in order to understand the possible implications of PT symmetry in the next generation of quantum technologies. In this work, we address this need by proposing and studying a circuit-QED architecture that consists of two coupled resonators and two qubits (each coupled to one resonator). By means of external driving fields on the qubits, we are able to tune gains and losses in the resonators. Starting with the quantum dynamics of this system, we show the emergence of the PT symmetry via the selection of both driving amplitudes and frequencies. We engineer the system such that a non-number-conserving dipole-dipole interaction emerges, introducing an instability at large coupling strengths. The PT symmetry and its breaking, as well as the predicted instability in this circuit-QED system, can be observed in a transmission experiment.

[1]  Natalia M. Litchinitser,et al.  Orbital angular momentum microlaser , 2016, Science.

[2]  F. Nori,et al.  Simultaneous cooling of an artificial atom and its neighboring quantum system. , 2007, Physical review letters.

[3]  H. Yilmaz,et al.  Loss-induced suppression and revival of lasing , 2014, Science.

[4]  장윤희,et al.  Y. , 2003, Industrial and Labor Relations Terms.

[5]  Collett,et al.  Input and output in damped quantum systems: Quantum stochastic differential equations and the master equation. , 1985, Physical review. A, General physics.

[6]  S. Girvin,et al.  Charge-insensitive qubit design derived from the Cooper pair box , 2007, cond-mat/0703002.

[7]  Shanhui Fan,et al.  Parity–time-symmetric whispering-gallery microcavities , 2013, Nature Physics.

[8]  F. Nori,et al.  Microwave photonics with superconducting quantum circuits , 2017, 1707.02046.

[9]  M. Devoret Quantum Fluctuations in Electrical Circuits , 1997 .

[10]  Franco Nori,et al.  What is and what is not electromagnetically induced transparency in whispering-gallery microcavities , 2014, Nature Communications.

[11]  F. Nori,et al.  Quantum information processing with superconducting qubits in a microwave field , 2003, cond-mat/0306207.

[12]  D. Christodoulides,et al.  Parity-time–symmetric microring lasers , 2014, Science.

[13]  Lan Yang,et al.  Exceptional points enhance sensing in an optical microcavity , 2017, Nature.

[14]  E. Solano,et al.  Tunable and switchable coupling between two superconducting resonators , 2014, 1405.1969.

[15]  Y. Ashida,et al.  Parity-time-symmetric quantum critical phenomena , 2016, Nature Communications.

[16]  Franco Nori,et al.  PT-symmetric phonon laser. , 2014, Physical review letters.

[17]  Lan Yang,et al.  Chiral modes and directional lasing at exceptional points , 2016, Proceedings of the National Academy of Sciences.

[18]  A. Houck,et al.  Low-Disorder Microwave Cavity Lattices for Quantum Simulation with Photons , 2012, 1203.5363.

[19]  Tsampikos Kottos,et al.  Experimental study of active LRC circuits with PT symmetries , 2011, 1109.2913.

[20]  David Zueco,et al.  Qubit-oscillator dynamics in the dispersive regime: Analytical theory beyond the rotating-wave approximation , 2009, 0907.3516.

[21]  A. Marx,et al.  Gradiometric flux qubits with a tunable gap , 2012, 1210.3982.

[22]  Davide Gatti,et al.  Robust light transport in non-Hermitian photonic lattices , 2015, Scientific Reports.

[23]  I. V. Barashenkov,et al.  Jamming anomaly in   -symmetric systems , 2016, 1606.04347.

[24]  C. Schneider,et al.  Observation of non-Hermitian degeneracies in a chaotic exciton-polariton billiard , 2015, Nature.

[25]  Franco Nori,et al.  Multiphoton quantum Rabi oscillations in ultrastrong cavity QED , 2015, 1509.06102.

[26]  J Casanova,et al.  Deep strong coupling regime of the Jaynes-Cummings model. , 2010, Physical review letters.

[27]  A. Saxena,et al.  PT -symmetric slowing down of decoherence , 2016, 1607.05778.

[28]  V. Vinokur,et al.  Stimulation of the fluctuation superconductivity by PT symmetry. , 2010, Physical review letters.

[29]  Franco Nori,et al.  Two-level systems driven by large-amplitude fields , 2007 .

[30]  Fernando Quijandría,et al.  Circuit QED bright source for chiral entangled light based on dissipation. , 2012, Physical review letters.

[31]  H. Harney,et al.  PT symmetry and spontaneous symmetry breaking in a microwave billiard. , 2011, Physical review letters.

[32]  R. Morandotti,et al.  Observation of PT-symmetry breaking in complex optical potentials. , 2009, Physical review letters.

[33]  F. Nori,et al.  Atomic physics and quantum optics using superconducting circuits , 2011, Nature.

[34]  E. Solano,et al.  Ultrastrong coupling in two-resonator circuit QED , 2014, 1412.7372.

[35]  Hong-Gyu Park,et al.  Direct observation of exceptional points in coupled photonic-crystal lasers with asymmetric optical gains , 2016, Nature Communications.

[36]  Masahito Ueda,et al.  Information Retrieval and Criticality in Parity-Time-Symmetric Systems. , 2017, Physical review letters.

[37]  Blatt,et al.  Laser cooling of trapped ions in a standing wave. , 1992, Physical review. A, Atomic, molecular, and optical physics.

[38]  Persistent single-photon production by tunable on-chip micromaser with a superconducting quantum circuit , 2005, quant-ph/0512145.

[39]  Andrea Alù,et al.  An invisible acoustic sensor based on parity-time symmetry , 2015, Nature Communications.

[40]  S. Girvin,et al.  0 40 73 25 v 1 1 3 Ju l 2 00 4 Circuit Quantum Electrodynamics : Coherent Coupling of a Single Photon to a Cooper Pair Box , 2022 .

[41]  M. Segev,et al.  Observation of parity–time symmetry in optics , 2010 .

[42]  F. Nori,et al.  Superconducting Circuits and Quantum Information , 2005, quant-ph/0601121.

[43]  Bernhard H. Haak,et al.  Open Quantum Systems , 2019, Tutorials, Schools, and Workshops in the Mathematical Sciences.

[44]  Xuedong Hu,et al.  Low-decoherence flux qubit , 2007 .

[45]  U. Peschel,et al.  Parity–time synthetic photonic lattices , 2012, Nature.

[46]  C. Bender,et al.  Observation of PT phase transition in a simple mechanical system , 2012, 1206.4972.

[47]  D. Porras,et al.  The Bose–Hubbard model with squeezed dissipation , 2014, 1409.0361.

[48]  A. Szameit,et al.  Mobility transition from ballistic to diffusive transport in non-Hermitian lattices , 2013, Nature Communications.

[49]  E Solano,et al.  Dynamical Casimir effect entangles artificial atoms. , 2014, Physical review letters.

[50]  P. Rabl,et al.  Dynamically encircling exceptional points in a waveguide: asymmetric mode switching from the breakdown of adiabaticity , 2016, 1603.02325.

[51]  G. Strasser,et al.  Reversing the pump dependence of a laser at an exceptional point , 2014, Nature Communications.

[52]  Demetrios N. Christodoulides,et al.  Enhanced sensitivity at higher-order exceptional points , 2017, Nature.

[53]  Jing Zhang,et al.  Optomechanically-induced transparency in parity-time-symmetric microresonators , 2014, Scientific Reports.

[54]  Franco Nori,et al.  High-order exceptional points in optomechanics , 2016, Scientific Reports.

[55]  Luyao Jiang,et al.  Topological energy transfer in an optomechanical system with exceptional points , 2016, Nature.

[56]  Franco Nori,et al.  Exceptional Points in Random-Defect Phonon Lasers , 2017, 1701.08000.

[57]  C. Bender Introduction to 𝒫𝒯-symmetric quantum theory , 2005, quant-ph/0501052.

[58]  R. Gross,et al.  Tunable coupling engineering between superconducting resonators: From sidebands to effective gauge fields , 2012, 1207.3408.

[59]  C. Harmans,et al.  Tuning the gap of a superconducting flux qubit. , 2008, Physical review letters.

[60]  Y. Wang,et al.  Single-mode laser by parity-time symmetry breaking , 2014, Science.

[61]  C. Bender,et al.  Real Spectra in Non-Hermitian Hamiltonians Having PT Symmetry , 1997, physics/9712001.

[62]  Jianming Wen,et al.  Anti-parity–time symmetry with flying atoms , 2016 .