| P. Cvitanovi'c, B. Eckhardt, Symmetry decomposition of chaotic dynamics, Nonlinearity 6 (1993) 277-311. |
....creeping orbits 8m 0 : 1.7) The semiclassical denominator is (1 Gamma 1= and not (1 Gamma 1= 0 ) as one would naively expect, because the periodic orbit is tracing the boundary of the fundamental domain of this system. For the special properties of boundary orbits see Refs. [25, 26]. See also Eq. 7.32) of Berry s KKR paper [8] where the contribution of the bounce orbit (between two discs) to the integrated spectral density for Sinai s billiard can be found. Thus for the 2 disk system the quantum mechanical cumulant expansion of the characteristic determinant and the ....
P. Cvitanovi'c, B. Eckhardt, Symmetry decomposition of chaotic dynamics, Nonlinearity 6 (1993) 277-311.
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