| H-J Stockmann was born in 1945 in Gottingen, Germany. He started his studies in physics and mathematics in 1964 at the University of Heidelberg. He performed his diploma work in experimental physics, on Optical spectroscopy which the finished in 1969. For his doctoral work he changed to nuclear solid state physics, with experiments at the research reactor of the Kernforschungszentrum karlsruhe. |
| Preface 1 Introduction 2 Billiard experiments 2.1 Wave propagation in solids and liquids 2.1.1 Chladni figures 2.1.2 Water surface waves 2.1.3 Vibrating blocks 2.1.4 Ultrasonic fields in water-filled cavities 2.2 Microwave billiards 2.2.1 Basic principles 2.2.2 Field distributions in microwave cavities 2.2.3 Billiards with broken time-reversal symmetry 2.2.4 Josephsonjunctions 2.3 Mesoscopic structures 2.3.1 Antidot lattices 2.3.2 Quantum dot billiards 2.3.3 Quantum well billiards 2.3.4 Quantum corrals 3 Random matrices 3.1 Gaussian ensembles 3.1.1 Symmetries 3.1.2 Univeraslity classes 3.1.3 Definition of the Gaussian ensembles 3.1.4 Correlated eigenenergy distribution 3.1.5 Averaged density of states 3.2 Spectral correlations …… 3.3 Supersymmetry method 4 Floquet and tight-binding systems 4.1 Hamiltonians with periodic time depedences 4.2 Dynamical localization 4.3 Tight-binding systems 5 Eigenvalue dynamics 5.1 Pechukas-Yukawa model 5.2 Billiard level dynamics 5.3 Geometrical phases 6 Scattering systems 6.1 Billiards as scattering systems 6.2 Amplitude distribution functions 6.3 Fluctuation properties of the scattering matrix 7 Semiclassical quantum mechanics 7.1 Integrable systems 7.2 Gutzwiller trace formula 7.3 Contributions to the density of states 8 Applications of periodic orbit theory 8.1 Periodic orbit analysis of spectra and wave functions 8.2 Semiclassical theory of spectral rigidity 8.3 Periodic orbit calculation of spectra 8.4 Surfaces with constant negative curvature References Index |
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