2018
DOI: 10.1103/physreva.97.022105
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Variance uncertainty relations without covariances for three and four observables

Abstract: New sum and product uncertainty relations, containing variances of three or four observables, but not containing explicitly their covariances, are derived. One of consequences is the new inequality, giving a nonzero lower bound for the product of two variances in the case of zero mean value of the commutator between the related operators. Moreover, explicit examples show that in some cases this new bound can be better than the known Robertson-Schrödinger one.

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Cited by 24 publications
(27 citation statements)
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“…Several interesting questions and problems arise in connection with our study. For example, is it possible to obtain more precise limits for the high-order uncertainty products for several degrees of freedom, generalizing known results for the products of variances [ 2 , 29 , 76 , 77 , 78 , 79 , 80 , 81 , 82 ]? Probably, applications to the problem of intensity-difference squeezing [ 83 , 84 ] can be found.…”
Section: Discussionmentioning
confidence: 99%
“…Several interesting questions and problems arise in connection with our study. For example, is it possible to obtain more precise limits for the high-order uncertainty products for several degrees of freedom, generalizing known results for the products of variances [ 2 , 29 , 76 , 77 , 78 , 79 , 80 , 81 , 82 ]? Probably, applications to the problem of intensity-difference squeezing [ 83 , 84 ] can be found.…”
Section: Discussionmentioning
confidence: 99%
“…SUR was initially derived from the Cauchy-Schwarz inequality, and can only be used to describe the uncertainty relation for two incompatible obervables. Since then, lots of work has been done along the way of Schrödinger regime [51][52][53][54][55] , and most of them mainly focused on extending SUR to uncertainty relations for more incompatible observables 56 . We refer to these uncertainty relations as the Schrödinger's spirit, and these uncertainty relations can be uniformly derived as follows.…”
Section: Uncertainty Relation Class-c0mentioning
confidence: 99%
“…Denoting ℳ =̂1 −̂2 − 〈̂̂1〉̂/〈̂̂〉 + 〈̂̂2〉̂/〈̂̂〉, where ̂=̂ or ̂ , and taking advantage of 〈ℳℳ † 〉 ≥ 0 [30] and Eq. (1), one can obtain a lower bound for ∆(̂1 −̂2) 2 (for more details, please see the appendix):…”
Section: Deduction Of the Local Criterions For Quantum Phase Syncmentioning
confidence: 99%