Title:
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Transport and escape in quantum dynamic systems
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Discrete spatial symmetries affect ergodic transport through two-dimensional mesoscopic
systems with chaos-inducing geometries and coherence lengths greater than
the system's size. This thesis looks at those effects in symmetries both commuting
and anticommuting with the current. Additionally the validity of the fractal Weyl
law for quantum systems with mixed phase space is examined.
Calculating the joint probability distribution of transmission eigenvalues of
systems with discrete symmetries using random matrix theory shows that in the
orthogonal universality class the transmission eigenvalues show repulsion of every
second eigenvalue. For lead-preserving symmetries this behaviour is a result of
superposition of independent sequences, while for symmetries mapping leads onto
each other different one-point weights in the probability distribution prevent such
an interpretation. This has the largest effect for narrow leads, as confirmed by
numerical calculations.
Microscopical understanding of symmetry effects is gained using a semiclassical
approach to calculate the weak localization corrections and universal conductance
fluctuations of systems where symmetry is broken by disturbing the internal symmetry
of the system or displacing the leads. Duplicating random matrix theory
results for perfect symmetry, this approach shows that symmetry effects vanish
fast for small deviations from symmetry over a large part of the system while
arbitrary deviations with a width smaller than the lead width have finite effect.
Symmetry effects will show whenever leads overlap in part with mirrored leads.
These results are confirmed with a crossover of random matrix ensembles.
We examine the statistics of resonances in open systems with a mixed phase
space. For this, we introduce a Husimi representation of decaying states based on
the Schur decomposition of the time evolution operator. Applying this method
to the open kicked rotator shows that a modified fractal Weyl law holds, which is
cormected to emerging quantum-to-classical correspondence.
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