2008
DOI: 10.1103/physreve.78.055204
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Chaotic scattering in the regime of weakly overlapping resonances

Abstract: We measure the transmission and reflection amplitudes of microwaves in a resonator coupled to two antennas at room temperature in the regime of weakly overlapping resonances and in a frequency range of 3-16GHz . Below 10.1GHz the resonator simulates a chaotic quantum system. The distribution of the elements of the scattering matrix S is not Gaussian. The Fourier coefficients of S are used for a best fit of the autocorrelation function of S to a theoretical expression based on random-matrix theory. We find very… Show more

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Cited by 31 publications
(43 citation statements)
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“…For their experimental verification, scattering data were taken at room temperature using a microwave resonator with the shape of a chaotic tilted stadium billiard allowing tests also with unprecedented accuracy in the regions of isolated and weakly overlapping resonances. 34,[36][37][38][39] Experiments were furthermore performed with microwave billiards where a partial T violation was induced by a magnetized ferrite. 40 For the analysis of the latter, we extended predictions derived for T -invariant systems by Verbaarschot, Weidenm€ uller, and Zirnbauer 32 for the Smatrix autocorrelation functions to systems with partial T violation.…”
Section: Quantum Chaos In Closed and Open Systems: The Bunimovicmentioning
confidence: 99%
“…For their experimental verification, scattering data were taken at room temperature using a microwave resonator with the shape of a chaotic tilted stadium billiard allowing tests also with unprecedented accuracy in the regions of isolated and weakly overlapping resonances. 34,[36][37][38][39] Experiments were furthermore performed with microwave billiards where a partial T violation was induced by a magnetized ferrite. 40 For the analysis of the latter, we extended predictions derived for T -invariant systems by Verbaarschot, Weidenm€ uller, and Zirnbauer 32 for the Smatrix autocorrelation functions to systems with partial T violation.…”
Section: Quantum Chaos In Closed and Open Systems: The Bunimovicmentioning
confidence: 99%
“…It is to be noticed that for α = ∞ we retrieve the case where ports/apertures radiate in free-space. In the limit of infinitesimal losses the impedance fluctuation become very strong: this is a situation that can occur in superconducting cavities Alt et al (1998), in low-loss optical systems, e.g., lasers Türeci et al (2006), in microwave cavities operated in the non-Ericsson (weak overlapping) regime Dietz et al (2008Dietz et al ( , 2009, and in reverberation chambers/enclosures operated in the undermoded regime Arnaut (2001); Warne et al (2003); Orjubin et al (2006); Arnaut and Gradoni (2011).…”
Section: Random Coupling Model In Action: Numerical Simulationsmentioning
confidence: 99%
“…3(b). The shape of the cavity is a symmetry-reduced "cut-circle" that shows chaos for ray trajectories [24,[50][51][52][53]. The superconducting cavity is made of copper with Pb-plated walls and cooled to a temperature (6.6 [K]) below the transition temperature of Pb.…”
Section: A Three Experimental Systemsmentioning
confidence: 99%