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Quantum work in the Bohmian framework

  • University of Exeter
  • Loughborough University

Research output: Contribution to journal › Article › Scientific › peer-review

31 Citations (Scopus)
213 Downloads (Pure)

Abstract

At nonzero temperature classical systems exhibit statistical fluctuations of thermodynamic quantities arising from the variation of the system's initial conditions and its interaction with the environment. The fluctuating work, for example, is characterized by the ensemble of system trajectories in phase space and, by including the probabilities for various trajectories to occur, a work distribution can be constructed. However, without phase-space trajectories, the task of constructing a work probability distribution in the quantum regime has proven elusive. Here we use quantum trajectories in phase space and define fluctuating work as power integrated along the trajectories, in complete analogy to classical statistical physics. The resulting work probability distribution is valid for any quantum evolution, including cases with coherences in the energy basis. We demonstrate the quantum work probability distribution and its properties with an exactly solvable example of a driven quantum harmonic oscillator. An important feature of the work distribution is its dependence on the initial statistical mixture of pure states, which is reflected in higher moments of the work. The proposed approach introduces a fundamentally different perspective on quantum thermodynamics, allowing full thermodynamic characterization of the dynamics of quantum systems, including the measurement process.

Original languageEnglish
Article number012131
Pages (from-to)1-8
JournalPhysical Review A
Volume97
Issue number1
DOIs
Publication statusPublished - 30 Jan 2018
MoE publication typeA1 Journal article-refereed

Funding

We would like to thank M. Campisi, I. Starshinov, H. Miller, P. Muratore-Ginanneschi, and B. Donvil for inspiring discussions and M. Campisi, J. Garrahan, C. Jarzynski, P. Solinas, and P. Talkner for critical reading of the manuscript. This work has been in part supported by the Academy of Finland through its CoE Grants No. 284621 and No. 287750. R.S. acknowledges support from the Magnus Ehrnrooth Foundation. J.A. acknowledges support from EPSRC (Grant No. EP/M009165/1) and the Royal Society. This research was supported by the COST network No. MP1209 “Thermodynamics in the quantum regime”.

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