| 18. July 2011 | 19. July 2011 | 20. July 2011 | 21. July 2011 | 22. July 2011 | 23. July 2011 |
| Monday | Tuesday | Wednesday | Thursday | Friday | Saturday |
| 09.30-10.00 registration | 09.30-10.15 Voigt | 09.30-12.30 PhD-Symposium | 09.30-10.15 Voigt | 09.30-10.15 Smilansky | 09.30-12.30 PhD-Symposium |
| 10.00-10.15 opening | 10.30-11.15 Berkolaiko | 10.30-11.15 Berkolaiko | 10.30-11.15 Smilansky | ||
| 10.15-11.00 Voigt | 11.30-12.15 Kurasov | 11.30-12.15 Kurasov | 11.30-12.15 Luger | ||
| 11.15-12.00 Berkolaiko | 12.15-13.15 break | 12.15-13.15 break | 12.15-13.15 break | ||
| 12.00-13.00 break | |||||
| 13.15-14.00 Voigt | 13.30-14.15 Luger | 14.00-18.00 excursion | 13.30-14.15 Kurasov | 13.30-14.15 Luger | 14.00-18.00 discussion |
| 14.15-15.00 Berkolaiko | 14.30-15.15 Berkolaiko | 14.30-15.15 Smilansky | 14.30-15.15 Kurasov | ||
| 15.15-16.00 Kurasov | 15.30-16.15 Schanz | 15.30-16.15 Streda | |||
| 16.00-18.00 PhD-Symposium | 16.15-18.00 PhD-Symposium | 16.15-18.00 PhD-Symposium | 15.15-18.00 PhD-Symposium |
| Gregory Berkolaiko: Nodal domains and critical nodal partitions |
| Intoduction to quantum graphs, hearing the shape of the graph, isospectral graphs and nodal domains |
| Rank-one perturbations and interlacing inequalities, variation of graph parameters |
| Bounds and exact formulas for nodal count |
| Critical partitions on graphs |
| Pavel Kurasov: Inverse problems for quantum graphs |
| Quantum graphs: definition and elementary spectral properties |
| Titchmarsh-Weyl M-function for quantum graphs and spectra of compact graphs |
| Boundary control and inverse problems for standard operators on trees |
| Inverse problems for graphs with cycles |
| Isoscattering and matching conditions |
| Annemarie Luger: Analytic matrix functions as a tool for quantum graphs |
| On the different (but equivalent) ways how to write s.a. boundary/matching conditions: a comparison and overview |
| Kreins formula and its application to quantum graphs |
| On the number of negative eigenvalues of Laplacians on graphs |
| Uzy Smilansky: Topics from the spectral theory of the discrete Laplacian on d-regular graphs |
| Introduction to d-regular graphs |
| The Bartholdi identity and spectral trace formulae. Applications for metric (quantum) graphs |
| Spectral statistics |
| Eigenvectors, nodal domains and percolation |
| Scattering on discrete graphs |
| Jügen Voigt: Differential operators on metric graphs and selfadjointness |
| Forms and self-adjoint operators on Hilbert space |
| Dirichlet forms and Beurling-Deny criteria |
| Boundary (or glueing) conditions for second order differential operators on metric graphs (quantum graphs) |
| On positivity of the associated `Schrödinger semigroup' |
| Pavel Streda: Anomalous Hall conductivity: local orbitals approach |
| A review of general features of the anomalous Hall conductivity observed on ferromagnetic systems followed by a theory based on the space distribution of the current densities will be presented. It is argued that intrinsic anomalous conductivity is determined by the Berry phase correction to the magnetic moment which is closely related to the charge polarizability. Effect of the finite electron life time is modeled by energy fluctuations of atomic-like orbitals. Presented tight-binding model gives by the unified way experimentally observed qualitative features of the anomalous Hall conductivity in the so called good metal regime and that called as bad metal or hopping regime. Posibility to describe this effect in the high conductivity regime by using Landauer- Buttiker type transport theory will be discussed. |
| Holger Schanz: Semiclassical expansion of correlation functions on quantum graphs: Applications to mesoscopic electron transport |
| The physical mechanism of electronic transport changes qualitatively when a device such as a transistor is downsized to the nanometer scale. Then the transport is mesoscopic and both, classical and quantum aspects are relevant simultaneously. In this regime, one approach to a quantitative theory is based one a semiclassical summation over classical trajectories. Quantum graphs are useful models in this context because they allow to test the summation techniques in a simplified situation, where the enumeration of trajectories and the calculation of their phases is exact. In the talk I will demonstrate this point with two examples of physical interest, Anderson localization in 1D disordered systems and electronic shot noise for a chaotic quantum dot. |