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日本物理学会講演概要集

24aRG-8 Upper bound on our knowledge about noncommuting observables for a qubit system

雄司 黒谷, 貴大 沙川, 正仁 上田

Published Aug 21, 2007• 0 citations
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We formulate the accuracy of quantum measurement for a qubit system in terms of a 3 by 3 matrix.This matrix, which we refer to as the accuracy matrix, can be calculated from a POVM corresponding to the quantum measurement.Based on the accuracy matrix, we derive new $trad\triangleright 0ff$ relations between the measurement accuracy of two or three noncommuting observables of a qubit system.These trade-off relations offer a quantitative information-theoretic representation of Bohr's principle of complementarity.We also show that the accuracy matrix is closely related to the maximum-likelihood estimation and the Fisher information matrix for a finite number of samples; the accuracy matrix tells us how accurately we can estimate the probability distributions of observables of an unknown state by quantum measurement.

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We formulate the accuracy of quantum measurement for a qubit system in terms of a 3 by 3 matrix.This matrix, which we refer to as the accuracy matrix, can be calculated from a POVM corresponding to the quantum measurement.Based on the accuracy matrix, we derive new trad▹0fftrad\triangleright 0fftrad▹0ff relations between the measurement accuracy of two or three noncommuting observables of a qubit system.These trade-off relations offer a quantitative information-theoretic representation of Bohr's principle of complementarity.We also show that the accuracy matrix is closely related to the maximum-likelihood estimation and the Fisher information matrix for a finite number of samples; the accuracy matrix tells us how accurately we can estimate the probability distributions of observables of an unknown state by quantum measurement.