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  • Letter

First passage times for continuous quantum measurement currents

Michael J. Kewming1,*, Anthony Kiely2,3, Steve Campbell2,3,4, and Gabriel T. Landi5

  • 1School of Physics, Trinity College Dublin, College Green, Dublin 2, Ireland
  • 2School of Physics, University College Dublin, Belfield, Dublin 4, Ireland
  • 3Centre for Quantum Engineering, Science, and Technology, University College Dublin, Belfield, Dublin 4, Ireland
  • 4Dahlem Center for Complex Quantum Systems, Freie Universität Berlin, Arnimallee 14, 14195 Berlin, Germany
  • 5Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA

  • *kewmingm@tcd.ie

Phys. Rev. A 109, L050202 – Published 20 May, 2024

DOI: https://doi.org/10.1103/PhysRevA.109.L050202

Abstract

The first passage time (FPT) is the time taken for a stochastic process to reach a desired threshold. In this Letter we address the FPT of the stochastic measurement current in the case of continuously measured quantum systems. We find that our approach, based on a charge-resolved master equation related to full-counting statistics of charge detection, enables efficient and analytical computation of the FPT. We develop a versatile framework applicable to quantum jump unraveling and quantum diffusion scenarios, demonstrating that the FPT can be obtained by introducing absorbing boundary conditions. Our framework is demonstrated with two relevant examples: First, we examine the tightness of recently proposed kinetic uncertainty relations for quantum jumps, which place bounds on the signal-to-noise ratio of the FPT. Second, we investigate the usage of qubits as threshold detectors for Rabi pulses, showing how our method can optimize detection probability while minimizing false positives. This Letter offers insights into the applications of the FPT for continuous measurements including the signal-to-noise ratio bounds and false positive minimization strategies, advancing quantum information processing applications.

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