Abstract

Heisenberg’s uncertainty principle has recently led to general measurement uncertainty relations for quantum systems: incompatible observables can be measured jointly or in sequence only with some unavoidable approximation, which can be quantified in various ways. The relative entropy is the natural theoretical quantifier of the information loss when a `true’ probability distribution is replaced by an approximating one. In this paper, we provide a lower bound for the amount of information that is lost by replacing the distributions of the sharp position and momentum observables, as they could be obtained with two separate experiments, by the marginals of any smeared joint measurement. The bound is obtained by introducing an entropic error function, and optimizing it over a suitable class of covariant approximate joint measurements. We fully exploit two cases of target observables: (1) n-dimensional position and momentum vectors; (2) two components of position and momentum along different directions. In (1), we connect the quantum bound to the dimension n; in (2), going from parallel to orthogonal directions, we show the transition from highly incompatible observables to compatible ones. For simplicity, we develop the theory only for Gaussian states and measurements.

Highlights

  • Uncertainty relations for position and momentum [1] have always been deeply related to the foundations of Quantum Mechanics

  • In order to deal with measurement uncertainty relations (MURs) for position and momentum observables, we have to introduce the class of approximate joint measurements of position and momentum, whose marginals we will compare with the respective sharp observables

  • The entropic MURs we found share the nice property of being scale invariant and well-behaved in the classical and macroscopic limits

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Summary

Introduction

Uncertainty relations for position and momentum [1] have always been deeply related to the foundations of Quantum Mechanics. This is a flaw due to the very definition of differential entropy, and one of the reasons that lead us to introduce relative entropy based MURs. In Section 5 we construct the covariant observables which will be used as approximate joint measurements of the position and momentum target observables.

Target Observables and States
Position and Momentum
Vector Observables
Scalar Observables
Quantum Moments
Weyl Operators and Gaussian States
Relative and Differential Entropies
Relative Entropy or Kullback-Leibler Divergence
Differential Entropy
Entropic PURs for Position and Momentum
Approximate Joint Measurements of Position and Momentum
Covariant Vector Observables
Covariant Scalar Observables
Gaussian Measurements
Covariant Gaussian Observables
Entropic MURs for Position and Momentum
Error Function
Entropic Incompatibility Degree of Qu and Pv
Entropic Incompatibility Degree of Q and P
Conclusions
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