Abstract

Beam splitters are important components in numerous tasks of quantum information protocols used either in simple or in an interferometric arrangement or together with other quantum systems. This report shows interesting aspects of the quantum correlations of two-mode Gaussian state (TMGS) for the photons retrieved via a linear beam splitter when they are initially employed at the input of either pure or mixed two single-mode Gaussian states (TSMGSs). The quantum correlations obey the boundaries of quantum non-locality, steering, entanglement and discord for pure input states. Though Bell inequality does not violate, quantum steering, entanglement and discord exist in the quantum state evolved by the beam splitter when input states become mixed. Specifically, the quantum steering, entanglement and discord persist to some degrees against the thermal photon number, the Bell inequality is, nonetheless, obeyed by the quantum state except in a very sharp regime.

Highlights

  • A Bell type inequality is defined to measure quantum non-locality

  • This expression can be described as an expectation value of the displaced parity operator

  • It results in J1 = (b2 + 2c2 b2/b1) (18), the optimized Bell’s combination appears as

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Summary

Introduction

A Bell type inequality is defined to measure quantum non-locality. The displaced parity operator for a two-mode field becomes Π (α′1, (creation) operator and Dai(α′. × exp[4Y( α1 2 b2cos2φ1 + α2 2 b1cos2φ2 + y)], (13) This expression can be described as an expectation value of the displaced parity operator. A Bell type inequality is defined to measure quantum non-locality.

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