Information theory, squeezing, and quantum correlations
- 1 July 1991
- journal article
- research article
- Published by American Physical Society (APS) in Physical Review A
- Vol. 44 (1), 535-545
- https://doi.org/10.1103/physreva.44.535
Abstract
Information theory allows us to make quantitative statements about the strength and nature of the correlations between systems. Application of this theory to the quantized electromagnetic field reveals a special role for the two-mode squeezed states. The nonclassical properties of these states arise from the intermode correlations, and we apply information-theoretic methods to determine the strength of the correlation between specific pairs of observables. This analysis leads to the important general result that for any correlated pure state a given pair of single-system observables contains at most only half the information about the correlations. We discuss the implications of this result for the distinction between classical and quantum systems.Keywords
This publication has 37 references indexed in Scilit:
- Periodicity, phase, and entropy in models of two-photonresonanceJournal of the Optical Society of America B, 1990
- Entropy as a measure of quantum optical correlationPhysical Review A, 1989
- Fluctuations and entropy in models of quantum optical resonanceAnnals of Physics, 1988
- Violations of classical inequalities in quantum opticsPhysical Review A, 1986
- Experimental Test of Bell's Inequalities Using Time- Varying AnalyzersPhysical Review Letters, 1982
- Experimental Realization of Einstein-Podolsky-Rosen-BohmGedankenexperiment: A New Violation of Bell's InequalitiesPhysical Review Letters, 1982
- Squeezed States and Sub-Poissonian Photon StatisticsPhysical Review Letters, 1982
- A general argument against superluminal transmission through the quantum mechanical measurement processLettere al Nuovo Cimento (1971-1985), 1980
- Entropy, information and quantum measurementsCommunications in Mathematical Physics, 1973
- Can Quantum-Mechanical Description of Physical Reality Be Considered Complete?Physical Review B, 1935