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Volumn 3, Issue 1, 1986, Pages 76-85

New theory of partial coherence in the space-frequency domain. Part II: Steady-state fields and higher-order correlations

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EID: 84975571278     PISSN: 10847529     EISSN: 15208532     Source Type: Journal    
DOI: 10.1364/JOSAA.3.000076     Document Type: Article
Times cited : (132)

References (29)
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    • Inverse source problem for three-dimensional partially coherent sources and fields
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    • Young's interference fringes with narrow-band light
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    • 2, ω), is discussed in E. Wolf, "Young's interference fringes with narrow-band light," Opt. Lett. 8, 250-252 (1983).
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    • 2, τ) will not contain any negative frequency components (Ref. 12, Sec. 10.3.2), and the lower limits in the integrals in Eqs. (3.17) and (3.18) can then be replaced by zero
    • 2, τ) will not contain any negative frequency components (Ref. 12, Sec. 10.3.2), and the lower limits in the integrals in Eqs. (3.17) and (3.18) can then be replaced by zero.
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    • Some coherence properties of non-Gaussian light
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    • Field correlations of arbitrary order appear to have been discussed first in the framework of the classical theory of stationary fields by L. Mandel, "Some coherence properties of non-Gaussian light," in Quantum Electronics III, P. Grivet and N. Bloembergen, eds. (Columbia U. Press, New York, 1964), Vol. I, pp. 101-109.
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    • Some coherence properties of non-Gaussian light
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    • It is implicitly assumed here that M > 1. When M = 1 one readily finds that the first product term (with the index j) in Eq. (4.10), and in all subsequent formulas where it appears, must be replaced by unity
    • It is implicitly assumed here that M > 1. When M = 1 one readily finds that the first product term (with the index j) in Eq. (4.10), and in all subsequent formulas where it appears, must be replaced by unity.
  • 23
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    • Cross-spectral density functions of arbitrary orders in classical wave fields were first considered by L. Mandel in Ref. 18. See also Refs. 21-23
    • Cross-spectral density functions of arbitrary orders in classical wave fields were first considered by L. Mandel in Ref. 18. See also Refs. 21-23.
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    • Light fluctuations as a new spectroscopic tool
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    • Some properties of higher order coherence functions
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    • Similar remarks apply here to those made in note 19 in connection with Eq. (4.10)
    • Similar remarks apply here to those made in note 19 in connection with Eq. (4.10).
  • 28
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    • A preliminary account of this application of our theory was presented at the 1984 Annual Meeting of the Optical Society of America [J. Opt. Soc. Am. A 1, 1311 (A) (1984)]
    • A preliminary account of this application of our theory was presented at the 1984 Annual Meeting of the Optical Society of America [J. Opt. Soc. Am. A 1, 1311 (A) (1984)].
  • 29
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    • Correlation theory of wave-fields generated by fluctuating, three-dimensional, primary, scalar sources. I: General theory
    • Equation (A13) was obtained previously by a somewhat less rigorous argument by Sec. 2
    • Equation (A13) was obtained previously by a somewhat less rigorous argument by W. H. Carter and E. Wolf in "Correlation theory of wave-fields generated by fluctuating, three-dimensional, primary, scalar sources. I: General theory," Opt. Acta 28, 227-244 (1981), Sec. 2.
    • (1981) Opt. Acta , vol.28 , pp. 227-244
    • Carter, W.H.1    Wolf, E.2


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