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Jarzynski equality for quantum stochastic maps

Quantum Physics · Submitted 20 Jul 2013

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We analyze here a more general case of arbitrary quantum operations on finite systems and derive the corresponding form of the Jarzynski equality.

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arXiv ID1307.5370 (version 4)
Pith ID3QHORVG5, Pith's permanent record of this paper and its review
CitationAlexey E. Rastegin, Karol \.Zyczkowski. "Jarzynski equality for quantum stochastic maps." arXiv:1307.5370 (2013). https://pith.science/paper/3QHORVG5
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What the abstract itself states, as probabilities: claims first 0.08 · states limitation 0.30 · human participants 0.01 · controlled comparison 0.07 · randomized assignment 0.01 · states quantitative result 0.52 · compares with prior results 0.85 · mentions code or data availability 0.02.

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arXiv listing abstract v4. Results and the main claim are underlined; .

Jarzynski equality and related fluctuation theorems can be formulated for various setups. Such an equality was recently derived for nonunitary quantum evolutions described by unital quantum operations, i.e., for completely positive, trace-preserving maps, which preserve the maximally mixed state. We analyze here a more general case of arbitrary quantum operations on finite systems and derive the corresponding form of the Jarzynski equality. It contains a correction term due to nonunitality of the quantum map. Bounds for the relative size of this correction term are established and they are applied for exemplary systems subjected to quantum channels acting on a finite-dimensional Hilbert space.

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 Jarzynski equality and related fluctuation theorems can be formulated for various setups. background 1.00 0.05 0.02 asserted 0.82
s1 Such an equality was recently derived for nonunitary quantum evolutions described by unital quantum operations, i.e., for completely positive, trace-preserving maps, which preserve the maximally mixed state. background 1.00 0.05 0.05 asserted 1.00
s2 We analyze here a more general case of arbitrary quantum operations on finite systems and derive the corresponding form of the Jarzynski equality. contribution 1.00 0.95 0.30 asserted 1.00
s3 It contains a correction term due to nonunitality of the quantum map. result 0.98 0.84 0.41 asserted 1.00
s4 Bounds for the relative size of this correction term are established and they are applied for exemplary systems subjected to quantum channels acting on a finite-dimensional Hilbert space. result 0.53 0.91 0.15 asserted 1.00

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Original abstract

Jarzynski equality and related fluctuation theorems can be formulated for various setups. Such an equality was recently derived for nonunitary quantum evolutions described by unital quantum operations, i.e., for completely positive, trace-preserving maps, which preserve the maximally mixed state. We analyze here a more general case of arbitrary quantum operations on finite systems and derive the corresponding form of the Jarzynski equality. It contains a correction term due to nonunitality of the quantum map. Bounds for the relative size of this correction term are established and they are applied for exemplary systems subjected to quantum channels acting on a finite-dimensional Hilbert space.

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Uses the method or tool of 1 paper
  • Following Ref. [ref] , we define the corresponding average [equation] Double angular brackets in the left-hand side denote the averaging over the ensemble of possible pairs of measurement outcomes.

    Jarzynski Relations for Quantum Systems and Some Applications · Jarzynski equality for bistochastic maps · 0.91

Compares with 1 paper
  • Using notation ([ref]) for a function of two eigenvalues, we then obtain [equation] This result was recently derived in Ref. [ref] and earlier by Tasaki [ref] under a weaker assumption of a unitary evolution.

    Jarzynski Relations for Quantum Systems and Some Applications · Jarzynski equality for bistochastic maps · 0.84

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