Abstract

The dimensionality of a thermometer is key in the design of quantum thermometry schemes. In general, the phenomenology that is typical of finite-dimensional quantum thermometry does not apply to infinite dimensional ones. We analyse the dynamical and metrological features of non-equilibrium Gaussian Quantum Thermometers: on one hand, we highlight how quantum entanglement can enhance the readiness of composite Gaussian thermometers; on the other hand, we show that non-equilibrium conditions do not guarantee the best sensitivities in temperature estimation, thus suggesting the reassessment of the working principles of quantum thermometry.

Highlights

  • The direct assessment of the properties of quantum mechanical systems is not always possible or convenient: In general, any direct interference would alter the properties of the system, possibly spoiling them

  • We analyze the dynamical and metrological features of nonequilibrium Gaussian quantum thermometers: On one hand, we highlight how quantum entanglement can enhance the readiness of composite Gaussian thermometers; on the other hand, we show that nonequilibrium conditions do not guarantee the best sensitivities in temperature estimation, suggesting the reassessment of some of the working principles underpinning quantum thermometry

  • While the formalism used to illustrate our findings is that of Gaussian quantum states and operations [34,35,36], our study addresses a wealth of physical situations of strong experimental relevance for quantum probing, from micro-/nanomechanical oscillators driven by optical or electric forces to microwave fields in superconducting waveguides and atomic spin systems collectively coupled to driving fields [37]

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Summary

INTRODUCTION

The direct assessment of the properties of quantum mechanical systems is not always possible or convenient: In general, any direct interference would alter the properties of the system, possibly spoiling them. Most of the current investigations in quantum thermometry use two-level systems as thermometers [8,9,10,11], shedding light on the link between the equilibrium heat capacity of such microscopic probes and the amount of information that can be gathered on the temperature of the environment [12,13,14], introducing bounds on the irreversible entropy production of the probe [15,16,17], and clarifying the extent of the advantages resulting from finite-time interactions for both temperature discrimination and estimation [14,18].

PHYSICAL MODEL
GEOMETRIC CONSIDERATIONS
METROLOGICAL CONSIDERATIONS
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