Abstract

In this work we study various notions of uncertainty for angular momentum in the spin-s representation of SU(2). We characterize the ‘uncertainty regions’ given by all vectors, whose components are specified by the variances of the three angular momentum components. A basic feature of this set is a lower bound for the sum of the three variances. We give a method for obtaining optimal lower bounds for uncertainty regions for general operator triples, and evaluate these for small s. Further lower bounds are derived by generalizing the technique by which Robertson obtained his state-dependent lower bound. These are optimal for large s, since they are saturated by states taken from the Holstein–Primakoff approximation. We show that, for all s, all variances are consistent with the so-called vector model, i.e., they can also be realized by a classical probability measure on a sphere of radius Entropic uncertainty relations can be discussed similarly, but are minimized by different states than those minimizing the variances for small s. For large s the Maassen–Uffink bound becomes sharp and we explicitly describe the extremalizing states. Measurement uncertainty, as recently discussed by Busch, Lahti and Werner for position and momentum, is introduced and a generalized observable (POVM) which minimizes the worst case measurement uncertainty of all angular momentum components is explicitly determined, along with the minimal uncertainty. The output vectors for the optimal measurement all have the same length where as

Highlights

  • The textbook literature on quantum mechanics seems to agree that the uncertainty relations for angular momentum, and for any pair of quantum observables A, B should be given by Robertson’s [25] inequality D2r (A)D2r (B)12, (1)valid for any density operator ρ, with D2r (A) denoting the variance of the outcomes of a measurement of A on the state ρ

  • In this paper we will provide some sharp measurement uncertainty relations for angular momentum, establishing along the way some methods which may be of interest in more general cases

  • In contrast to the variance, the entropy of a probability distribution does not change by permuting or rescaling the measurement outcomes and so only depends on the choice of the Pi and not on the eigenvalues ai. This implies that an entropic uncertainty relation, which constrains the output entropies of two observables A, B, only depends on the unitary operator U connecting the respective eigenbases

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Summary

25 September 2015

In this work we study various notions of uncertainty for angular momentum in the spin-s. We give a method for obtaining attribution to the author(s) and the title of optimal lower bounds for uncertainty regions for general operator triples, and evaluate these for small the work, journal citation and DOI. S. Further lower bounds are derived by generalizing the technique by which Robertson obtained his state-dependent lower bound. Further lower bounds are derived by generalizing the technique by which Robertson obtained his state-dependent lower bound These are optimal for large s, since they are saturated by states taken from the Holstein–Primakoff approximation. Entropic uncertainty relations can be discussed but are minimized by different states than those minimizing the variances for small s. The output vectors for the optimal measurement all have the same length r (s), where r (s) s 1 as s ¥

Introduction
Setting and notation
Summary of main results
Preparation uncertainty
The linear two-component bound
Robertson’s technique: a generalization
Entropic uncertainty
Measurement uncertainty
Metric error
Conclusions and outlook
Full Text
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