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1 Cover Page The handle holds various files of this Leiden University dissertation. Author: Dahlhaus, Jan Patrick Title: Random-matrix theory and stroboscopic models of topological insulators and superconductors Date:
2 Random-matrix theory and stroboscopic models of topological insulators and superconductors Proefschrift ter verkrijging van de graad van Doctor aan de Universiteit Leiden, op gezag van de Rector Magnificus prof. mr P. F. van der Heijden, volgens besluit van het College voor Promoties te verdedigen op woensdag 21 november 2012 klokke uur door Jan Patrick Dahlhaus geboren te Essen, Duitsland in 1982
3 Promotiecommissie Promotor: Overige leden: Prof. dr. C. W. J. Beenakker Prof. dr. E. R. Eliel Prof. dr. ir. L. P. Kouwenhoven (Technische Universiteit Delft) Prof. dr. H. Schomerus (Lancaster University) Prof. dr. J. Zaanen Casimir PhD Series, Delft-Leiden, ISBN Dit werk maakt deel uit van het onderzoekprogramma van de Stichting voor Fundamenteel Onderzoek der Materie (FOM), die deel uit maakt van de Nederlandse Organisatie voor Wetenschappelijk Onderzoek (NWO). This work is part of the research programme of the Foundation for Fundamental Research on Matter (FOM), which is part of the Netherlands Organisation for Scientific Research (NWO). Cover: Topological invariant of a nodal Rashba superconductor in contact with a metal, as a function of interface orientation and momentum. Compare with the left panel of Fig. 5.4.
4 To Nina and my parents.
5
6 Contents 1 Introduction Preface Concept of topology in insulating systems Example: winding number Boundary states Role of symmetries and dimensionality Anderson localization and topology Topological superconductors Example: Majorana wire Random-matrix theory Symmetry classes Circular ensembles Stroboscopic models The quantum kicked rotator Stroboscopic models in higher dimensions and the Anderson metal-insulator transition This thesis Chapter Chapter Chapter Chapter Chapter Chapter Chapter Random-matrix theory of thermal conduction in superconducting quantum dots Introduction
7 vi CONTENTS 2.2 Formulation of the problem Andreev quantum dot Scattering matrix ensembles Transmission eigenvalue distribution Joint probability distribution Eigenvalue density Distribution of the thermal conductance Minimal channel number Large number of channels Arbitrary number of channels How to reach the single-channel limit using topological phases Conclusion Appendix 2.A Calculation of the transmission eigenvalue distribution Random-matrix theory of Andreev reflection from a topological superconductor Introduction Andreev reflection eigenvalues Random-matrix theory Class D, ensemble CRE Class DIII, ensemble T-CRE Class C, ensemble CQE Class CI, ensemble T-CQE Dependence of conductance distributions on topological invariant Broken time-reversal symmetry Preserved time-reversal symmetry Weak localization and UCF Conclusion and comparison with a model Hamiltonian.. 64 Appendix 3.A Calculation of the invariant measure A.1 Class D (ensemble CRE) A.2 Class DIII (ensemble T-CRE) Appendix 3.B Proof of the topological-charge theorem for circular ensembles
8 CONTENTS vii 4 Quantum point contact as a probe of a topological superconductor Introduction Integer versus half-integer conductance plateaus Effect of disorder Effect of finite voltage and temperature Conclusion Appendix 4.A Model Hamiltonian Appendix 4.B Béri degeneracy Scattering theory of topological invariants in nodal superconductors Introduction Topological invariant for Andreev reflection Chiral symmetry Topological invariant Topologically protected boundary states Relation between conductance and topological invariant Effects of additional unitary symmetries Spatial symmetries Symmetries that preserve k Application: 2D Rashba superconductor Hamiltonian and edge states Reflection matrix and conductance Anisotropic spin-orbit coupling Effects of angular averaging and disorder Three-dimensional superconductors Topological invariant for arc surface states Example Conclusion Appendix 5.A Topological invariant counts number of unit Andreev reflection eigenvalues A.1 Proof for the Z invariant A.2 Proof for the Z 2 invariant Appendix 5.B Proof of Eq. (5.34) Appendix 5.C Equality of conductance and topological invariant in class BDI
9 viii CONTENTS 6 Quantum Hall effect in a one-dimensional dynamical system Introduction Formulation of the 2D stroboscopic model Quantum anomalous Hall effect Stroboscopic Hamiltonian Relation to quantum kicked rotator Floquet operator Mapping onto a 1D model Localization in the quantum Hall effect Numerical simulation Localization-delocalization transition Scaling and critical exponent Hall conductance and topological invariant Discussion Appendix 6.A Tight-binding representation Appendix 6.B Finite-time scaling Appendix 6.C Scattering matrix from Floquet operator Metal topological-insulator transition in the quantum kicked rotator with Z 2 symmetry Introduction Construction of the Z 2 quantum kicked rotator Stationary model without disorder Time-dependent model with disorder Mapping from 2D to 1D Phase diagram with disorder Scaling law and critical exponent Conclusion Geodesic scattering by surface deformations of a topological insulator Introduction Geodesic scattering Geodesic motion Scattering angle Calculation of the conductivity Linearized Boltzmann equation Isotropic dispersion relation Anisotropic dispersion relation
10 CONTENTS ix 8.4 Results Isotropic dispersion relation Anisotropic dispersion relation Comparison with potential scattering Carrier density dependence Anisotropy dependence of conductivity Appendix 8.A Calculation of scattering cross section A.1 Christoffel symbols in rotated basis A.2 Geodesic equation for shallow deformation A.3 Circularly symmetric deformation Samenvatting 181 Summary 185 List of Publications 187 Curriculum Vitæ 189
11 x CONTENTS
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