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Statistics of resonance poles, phase shifts and time delays in quantum chaotic scattering: Random matrix approach for systems with broken time-reversal invariance

J. Math. Phys. 38, 1918 (1997); doi:10.1063/1.531919

Issue Date: April 1997

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Yan V. Fyodorov and Hans-Jürgen Sommers
Fachbereich Physik, Universität-GH Essen, D-45117 Essen, Germany
Assuming the validity of random matrices for describing the statistics of a closed chaotic quantum system, we study analytically some statistical properties of the S-matrix characterizing scattering in its open counterpart. In the first part of the paper we attempt to expose systematically ideas underlying the so-called stochastic (Heidelberg) approach to chaotic quantum scattering. Then we concentrate on systems with broken time-reversal invariance coupled to continua via Mopen channels; a=1,2,...,M. A physical realization of this case corresponds to the chaotic scattering in ballistic microstructures pierced by a strong enough magnetic flux. By using the supersymmetry method we derive an explicit expression for the density of S-matrix poles (resonances) in the complex energy plane. When all scattering channels are considered to be equivalent our expression describes a crossover from the chi2 distribution of resonance widths (regime of isolated resonances) to a broad power-like distribution typical for the regime of overlapping resonances. The first moment is found to reproduce exactly the Moldauer–Simonius relation between the mean resonance width and the transmission coefficient. Under the same assumptions we derive an explicit expression for the parametric correlation function of densities of eigenphases thetaa of the S-matrix (taken modulo 2pi). We use it to find the distribution of derivatives taua=[partial-derivative]thetaa/[partial-derivative]E of these eigenphases with respect to the energy ("partial delay times") as well as with respect to an arbitrary external parameter. We also find the parametric correlations of the Wigner–Smith time delay tauw(E)=(1/M)[summation]a [partial-derivative]thetaa/[partial-derivative]E at two different energies EOmega/2 and E+Omega/2 as well as at two different values of the external parameter. The relation between our results and those following from the semiclassical approach as well as the relevance to experiments are briefly discussed. ©1997 American Institute of Physics.
History: Received 24 July 1996; accepted 11 December 1996
Permalink: http://link.aip.org/link/?JMAPAQ/38/1918/1
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KEYWORDS and PACS

Keywords
PACS
  • 03.65.Nk
    Classical and quantum physics: mechanics and fields Quantum mechanics Nonrelativistic scattering theory
  • 05.45.+b
    Statistical physics and thermodynamics Theory and models of chaotic systems
  • 03.65.Sq
    Classical and quantum physics: mechanics and fields Quantum mechanics Semiclassical theories and applications
  • 02.10.Sp
    Mathematical methods in physics Logic, set theory, and algebra Linear and multilinear algebra; matrix theory (finite and infinite)
  • 11.55.-m
    General theory of fields and particles S-matrix theory; analytic structure of amplitudes
  • YEAR: 1996-97

PUBLICATION DATA

ISSN:
0022-2488 (print)   1089-7658 (online)
Publisher:
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