Resonances and localization of classical waves in random systems with correlated disorder

Physical Review E - Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics

Volumn 60, Issue 5, 1999, Pages 6081-6090

  Samelsohn, Gregory ^a   Gredeskul, Sergey A ^a   Mazar, Reuven ^a  

^a BEN GURION UNIVERSITY OF THE NEGEV   (Israel)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 85035253207     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.60.6081     Document Type: Article

References (41)

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39. The same technique, applied in Ref. 21 to the mean (coherent) field, leads to the result coinciding exactly with that given by the Bourret approximation for the Dyson equation. This can be understood as an indirect confirmation of the fact that, unlike coherence function, the behavior of the mean field is less dependent on the backscattering effects even in the localization regime.
40. The complete form of the path integral, along with a description of the integration procedure, is presented in Refs. 21 and 22. Note that in these papers, the factor (Formula presented) in the exponential is erroneously missed, and the corresponding final result, representing the second (linear, with respect to the correlation function) term in a perturbative expansion, has to be taken with appropriate correction.
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