2017
DOI: 10.1142/s0219749917500411
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Quantum correlation based on weak measurements

Abstract: A quantum correlation [Formula: see text] based on weak measurements for bipartite systems is introduced. It is shown that the product states do not contain this quantum correlation. Also, the necessary and sufficient condition for any two-qubit state becoming a product state is obtained. The quantum correlation [Formula: see text] and other quantum correlation for two-qubit entangled pure state, Werner states and isotropic states are compared.

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Cited by 6 publications
(3 citation statements)
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“…where the postselection on the subsystem C is given by the orthornormal basis of subsystem C. Let us mention that completely different approaches to characterize general quantum correlation based on weak measurement but without postselection, and thus independent of the concept of weak value, were reported in Refs. [47,48].…”
Section: General Nonclassical Correlation From Local Weak Value Measu...mentioning
confidence: 99%
“…where the postselection on the subsystem C is given by the orthornormal basis of subsystem C. Let us mention that completely different approaches to characterize general quantum correlation based on weak measurement but without postselection, and thus independent of the concept of weak value, were reported in Refs. [47,48].…”
Section: General Nonclassical Correlation From Local Weak Value Measu...mentioning
confidence: 99%
“…Consider the economical phase-covariant QC quantum cloning, which is developed to use in the Quantum Key Distribution BB84 Protocol [4]. Here, we propose an alternative method to realize a high fidelity asymmetric QC machine using weak measurement, which has been widely employed in quantum information processing [40][41][42][43][44]. Compared with the previous scheme [18,22], the difference of the fidelity between two copies is reduced while the sum of the fidelity between two copies is enhanced.…”
Section: Introductionmentioning
confidence: 99%
“…WMs can give rise to anomalous (imaginary and/or unbounded) values, whose real part is regarded as a conditional average of the observable in the zero-disturbance limit [9], while the imaginary one is related to the disturbance of the measuring pointer during the measurement [10]. Beyond having inspired a significant analysis of the meaning of quantum measurement [11][12][13][14][15][16][17][18], they have been used both to address foundational problems [19], like macrorealism [20,21] and contextuality [22][23][24], and as a novel, impressive tool for quantum metrology and related quantum technologies, allowing high-precision measurements (at least in presence of specific noises [25,26]), as the tiny spin Hall effect [6] or small beam deflections [27][28][29][30], and characterization of quantum states [31,32]. Furthermore, the absence of wave function collapse in WMs allows performing sequential measurements of even non-commuting observables on the same particle [33][34][35][36], a task forbidden within the strong measurement framework in quantum mechanics.…”
mentioning
confidence: 99%