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2/c.
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edited by H. Blok, H. A. Ferwerda, and H. K. Kuiken (North-Holland, Amsterdam)
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D. Lenstra, in Huygens Principle 1690-1990; Theory and Applications, edited by H. Blok, H. A. Ferwerda, and H. K. Kuiken (North-Holland, Amsterdam, 1990).
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Lenstra, D.1
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0343120947
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note
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In the presence of disorder some of the pump light will be retroreflected, but since the pumps are typically three orders of magnitude stronger than the probe, we neglect this reflection for weak disorder. Also, as long as probe and conjugate reflected and transmitted intensities are sufficiently small, pump depletion can be neglected and the pumps may be taken as constant in the medium.
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23
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0019543746
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A. A. Abrikosov, Solid State Commun. 37, 997 (1981); V. I. Mel'nikov, Fiz. Tverd. Tela (Leningrad) 23, 782 (1981) [Sov. Phys. Solid State 23, 444 (1981)].
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Abrikosov, A.A.1
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A. A. Abrikosov, Solid State Commun. 37, 997 (1981); V. I. Mel'nikov, Fiz. Tverd. Tela (Leningrad) 23, 782 (1981) [Sov. Phys. Solid State 23, 444 (1981)].
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Mel'nikov, V.I.1
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A. A. Abrikosov, Solid State Commun. 37, 997 (1981); V. I. Mel'nikov, Fiz. Tverd. Tela (Leningrad) 23, 782 (1981) [Sov. Phys. Solid State 23, 444 (1981)].
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Sov. Phys. Solid State
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26
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0343120944
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note
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p≈1, in the regime of either weak disorder or a combination of strong disorder and weak phase conjugation.
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27
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33646603273
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P. W. Anderson et al., Phys. Rev. B 22, 3519 (1980); N. Kumar, ibid. 31, 5513 (1985).
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4243150711
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p). This moments equation generalizes the one ob-tained by Freilikher et al. [Phys. Rev. Lett. 73, 810 (1994)] for a linear absorbing random medium.
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Phys. Rev. Lett.
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Freilikher1
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Joshi, S.K.1
Jayannavar, A.M.2
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35
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0343993023
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note
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The 1D invariant imbedding approach used here can straight-forwardly be extended to 2D and 3D disordered PCM's by decomposing the system into one longitudinal dimension (direction of propagation) and one or two transverse dimension(s) (transverse modes).
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