Driving Forbidden Transitions in the Fluxonium Artificial Atom

Atomic systems display a rich variety of quantum dynamics due to the different possible symmetries obeyed by the atoms. These symmetries result in selection rules that have been essential for the quantum control of atomic systems. Superconducting artificial atoms are mainly governed by parity symmetry. Its corresponding selection rule limits the types of quantum systems that can be built using electromagnetic circuits at their optimal coherence operation points ("sweet spots"). Here, we use third-order nonlinear coupling between the artificial atom and its readout resonator to drive transitions forbidden by the parity selection rule for linear coupling to microwave radiation. A Lambda-type system emerges from these newly accessible transitions, implemented here in the fluxonium artificial atom coupled to its "antenna" resonator. We demonstrate coherent manipulation of the fluxonium artificial atom at its sweet spot by stimulated Raman transitions. This type of transition enables the creation of new quantum operations, such as the control and readout of physically protected artificial atoms.

[1]  A. Niskanen,et al.  Engineered selection rules for tunable coupling in a superconducting quantum circuit , 2009 .

[2]  Probing decoherence with electromagnetically induced transparency in superconductive quantum circuits. , 2003, Physical review letters.

[3]  Thomas de Quincey [C] , 2000, The Works of Thomas De Quincey, Vol. 1: Writings, 1799–1820.

[4]  Andreas Wallraff,et al.  Deterministic Quantum State Transfer and Generation of Remote Entanglement using Microwave Photons , 2018 .

[5]  P. Joyez,et al.  Decoherence in a superconducting quantum bit circuit , 2005 .

[6]  F. Wellstood,et al.  Raman coherence in a circuit quantum electrodynamics lambda system , 2015, Nature Physics.

[7]  V. Manucharyan,et al.  Protecting a superconducting qubit from energy decay by selection rule engineering , 2017 .

[8]  Hideaki Takayanagi,et al.  Two-photon probe of the Jaynes-Cummings model and controlled symmetry breaking in circuit QED , 2009 .

[9]  R. T. Brierley,et al.  Fluxonium-Based Artificial Molecule with a Tunable Magnetic Moment , 2016, 1610.01094.

[10]  Franco Nori,et al.  Controllable coupling between flux qubits. , 2006, Physical review letters.

[11]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[12]  Uri Vool,et al.  Introduction to quantum electromagnetic circuits , 2016, Int. J. Circuit Theory Appl..

[13]  E. Solano,et al.  Two-photon probe of the Jaynes-Cummings model and symmetry breaking in circuit QED , 2008, 0805.3294.

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

[15]  Jens Koch,et al.  Fluxonium: Single Cooper-Pair Circuit Free of Charge Offsets , 2009, Science.

[16]  E. Solano,et al.  Broken selection rule in the quantum Rabi model , 2015, Scientific Reports.

[17]  L. Frunzio,et al.  Simultaneous Monitoring of Fluxonium Qubits in a Waveguide , 2016, Physical Review Applied.

[18]  R. Schoelkopf,et al.  Superconducting Circuits for Quantum Information: An Outlook , 2013, Science.

[19]  F K Wilhelm,et al.  Quantum superposition of macroscopic persistent-current states. , 2000, Science.

[20]  Jens Koch,et al.  Realization of a Λ System with Metastable States of a Capacitively Shunted Fluxonium. , 2017, Physical review letters.

[21]  I. Pop,et al.  Fabrication of stable and reproducible submicron tunnel junctions , 2011, 1105.6204.

[22]  R. Stephenson A and V , 1962, The British journal of ophthalmology.

[23]  Orlando,et al.  Josephson Persistent-Current Qubit , 2022 .

[24]  Yvonne Y Gao,et al.  Non-Poissonian quantum jumps of a fluxonium qubit due to quasiparticle excitations. , 2014, Physical review letters.

[25]  L. Frunzio,et al.  Quantization of inductively shunted superconducting circuits , 2016, 1602.01793.

[26]  H.-G. Meyer,et al.  Sisyphus cooling and amplification by a superconducting qubit , 2007, 0708.0665.

[27]  Luke D. Burkhart,et al.  Deterministic Remote Entanglement of Superconducting Circuits through Microwave Two-Photon Transitions. , 2017, Physical review letters.

[28]  L. Ioffe,et al.  Protected Josephson Rhombus chains. , 2013, Physical review letters.

[29]  John Preskill,et al.  Protected gates for superconducting qubits , 2013, 1302.4122.

[30]  L. Ioffe,et al.  Physical implementation of protected qubits , 2012, Reports on progress in physics. Physical Society.

[31]  Franco Nori,et al.  Optical selection rules and phase-dependent adiabatic state control in a superconducting quantum circuit. , 2005, Physical review letters.

[32]  K. Berggren,et al.  Microwave-Induced Cooling of a Superconducting Qubit , 2006, Science.

[33]  M. Khabipov,et al.  Traveling-Wave Parametric Amplifier Based on Three-Wave Mixing in a Josephson Metamaterial , 2017, 2017 16th International Superconductive Electronics Conference (ISEC).

[34]  I. Pop,et al.  Novel E-beam lithography technique for in-situ junction fabrication: the controlled undercut , 2011, 1101.4576.

[35]  Dmitri S. Pavlichin,et al.  Designing quantum memories with embedded control: photonic circuits for autonomous quantum error correction. , 2009, Physical review letters.

[36]  John Schlafer,et al.  Direct observation of coherent population trapping in a superconducting artificial atom. , 2009, Physical review letters.

[37]  A. Narla,et al.  3-Wave Mixing Josephson Dipole Element , 2017, 1702.00869.

[38]  Vivien Marx,et al.  Lin Tian , 2020, Nature Methods.

[39]  R. Schoelkopf,et al.  Coherent suppression of electromagnetic dissipation due to superconducting quasiparticles , 2014, Nature.

[40]  Alexandre Blais,et al.  Quantum information processing with circuit quantum electrodynamics , 2007 .

[41]  S. Girvin,et al.  Sideband transitions and two-tone spectroscopy of a superconducting qubit strongly coupled to an on-chip cavity. , 2007, Physical review letters.

[42]  Chui-Ping Yang,et al.  Quantum information transfer and entanglement with SQUID qubits in cavity QED: a dark-state scheme with tolerance for nonuniform device parameter. , 2004, Physical review letters.

[43]  V. Manucharyan,et al.  Demonstration of Protection of a Superconducting Qubit from Energy Decay. , 2018, Physical review letters.

[44]  Yasunobu Nakamura,et al.  Single microwave-photon detector using an artificial Λ-type three-level system , 2016, Nature Communications.

[45]  K. Koshino,et al.  Microwave down-conversion with an impedance-matched Λ system in driven circuit QED. , 2014, Physical review letters.

[46]  A. Zorin,et al.  Josephson traveling-wave parametric amplifier with three-wave mixing , 2016, 1602.02650.

[47]  Olivier Buisson,et al.  Junction fabrication by shadow evaporation without a suspended bridge , 2011, Nanotechnology.

[48]  Liang Jiang,et al.  On-demand quantum state transfer and entanglement between remote microwave cavity memories , 2017, 1712.05832.