From quantum jumps to quasiparticle population

ORAL

Abstract

Superconducting quasiparticles (QP) play a dominant role in the relaxation of the fluxonium qubit in the vicinity of the half-flux-quantum bias point. Recent experiments integrating the fluxonium with a quantum-limited amplifier have measured quantum jump trajectories between the ground state and the first excited state. These trajectories show a change in the characteristic lifetime of the fluxonium qubit as a function of time, arising from a change in the number of QP's in the sample [1]. Using a simple model of QP dynamics and their effect on the fluxonium qubit, we can access the QP population with temporal resolution better than a 100 microsecond. Such rapid monitoring of QP dynamics is essential for understanding the sources of QP's and ultimately suppressing them.\\[4pt] [1] ``Non-Poissonian quantum jumps of a fluxonium qubit due to quasiparticle excitations,'' U. Vool, I.M. Pop et al. to be published in PRL 2014.

*Work supported by: IARPA, ARO, and ONR.

Authors

  • U. Vool

    • Department of Applied Physics, Yale University
    • Yale University
    • Yale Univ
  • I.M. Pop

    • Department of Applied Physics, Yale University
  • K. Sliwa

    • Department of Applied Physics, Yale University
  • B. Abdo

    • Department of Applied Physics, Yale University
  • C. Wang

    • Department of Applied Physics, Yale University
  • Y.Y. Gao

    • Department of Applied Physics, Yale University
  • A. Kou

    • Department of Applied Physics, Yale University
  • W.C. Smith

    • Department of Applied Physics, Yale University
  • T. Brecht

    • Department of Applied Physics, Yale University
  • S. Shankar

    • Department of Applied Physics, Yale University
  • M. Hatridge

    • Department of Applied Physics, Yale University
  • G. Catelani

    • Peter Gr\"unberg Institut (PGI-2), Forschungszentrum J\"ulich
  • L. Frunzio

    • Department of Applied Physics, Yale University
  • R.J. Schoelkopf

    • Department of Applied Physics, Yale University
  • L. Glazman

    • Department of Applied Physics, Yale University
  • M. Mirrahimi

    • Department of Applied Physics, Yale University and INRIA Paris Rocquencourt
  • M.H. Devoret

    • Department of Applied Physics, Yale University