Abstract

A cost-precision trade-off relationship, the so-called thermodynamic uncertainty relation (TUR), has been recently discovered in stochastic thermodynamics. It bounds certain thermodynamic observables in terms of the associated entropy production. In this work, we experimentally study the TUR in a two-qubit system using an NMR setup. Each qubit is prepared in an equilibrium state, but at different temperatures. The qubits are then coupled, allowing energy exchange (in the form of heat). Using the quantum state tomography technique we obtain the moments of heat exchange within a certain time interval and analyze the relative uncertainty of the energy exchange process. We find that generalized versions of the TUR, which are based on the fluctuation relation, are obeyed. However, the specialized TUR, a tighter bound that is valid under specific dynamics, is violated in certain regimes of operation, in excellent agreement with analytic results. Altogether, this experiment-theory study provides a deep understanding of heat exchange in quantum systems, revealing favorable noise-dissipation regimes of operation.

Highlights

  • Obtaining universal bounds of experimentally accessible physical observables has been a fundamental topic in physics

  • We experimentally examined the thermodynamic uncertainty relations (TURs) for heat exchange by realizing the XY model, performing quantum state tomography, and extracting the heat exchange cumulants

  • We found that the S-TUR provides a tight bound up to a certain threshold value for the qubit-qubit coupling parameter sin2(2π Jτ ), beyond which the bound is invalidated

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Summary

Introduction

Obtaining universal bounds of experimentally accessible physical observables has been a fundamental topic in physics. Recent studies have shown that for systems that are out of equilibrium, there exist trade-off relations between the relative uncertainty of integrated currents (heat, charge) and the associated entropy production [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42].

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