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• W1980175919 endingPage "6720" @default.
• W1980175919 startingPage "6713" @default.
• W1980175919 abstract "We extend the theory of the Hermitian optical phase operator to analyze the quantum phase properties of pairs of electromagnetic field modes. The operators representing the sum and difference of the two single-mode phases are simply the sum and difference of the two single-mode phase operators. The eigenvalue spectra of the sum and difference operators have widths of 4ensuremath{pi}, but phases differing by 2ensuremath{pi} are physically indistinguishable. This means that the phase sum and difference probability distributions must be cast into a 2ensuremath{pi} range. We obtain mod(2ensuremath{pi}) probability distributions for the phase sum and difference that unambiguously reveal the signatures of randomness, phase correlations, and phase locking. We use our approach to investigate the phase sum and difference properties for uncorrelated modes in random and partial phase states and the phase-locked properties of the two-mode squeezed vacuum states. We reveal the fundamental property of two-mode squeezed states that the phase sum is locked to the argument of the squeezing parameter. The variance of the phase sum depends dilogarithmically on 1+tanhr, where r is the magnitude of the squeezing parameter, vanishing in the large squeezing limit." @default.
• W1980175919 created "2016-06-24" @default.
• W1980175919 creator A5024625077 @default.
• W1980175919 creator A5085565215 @default.
• W1980175919 date "1990-12-01" @default.
• W1980175919 modified "2023-10-16" @default.
• W1980175919 title "Quantum theory of optical phase correlations" @default.
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• W1980175919 doi "https://doi.org/10.1103/physreva.42.6713" @default.
• W1980175919 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/9903971" @default.
• W1980175919 hasPublicationYear "1990" @default.
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