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Emil Prodan - Bulk and Boundary Invariants for Complex Topological Insulators

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Emil Prodan Bulk and Boundary Invariants for Complex Topological Insulators
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This monograph offers an overview of rigorous results on fermionic topological insulators from the complex classes, namely, those without symmetries or with just a chiral symmetry. Particular focus is on the stability of the topological invariants in the presence of strong disorder, on the interplay between the bulk and boundary invariants and on their dependence on magnetic fields.

The first part presents motivating examples and the conjectures put forward by the physics community, together with a brief review of the experimental achievements. The second part develops an operator algebraic approach for the study of disordered topological insulators. This leads naturally to the use of analytical tools from K-theory and non-commutative geometry, such as cyclic cohomology, quantized calculus with Fredholm modules and index pairings. New results include a generalized Streda formula and a proof of the delocalized nature of surface states in topological insulators with non-trivial invariants. The concluding chapter connects the invariants to measurable quantities and thus presents a refined physical characterization of the complex topological insulators.

This book is intended for advanced students in mathematical physics and researchers alike.

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Springer International Publishing Switzerland 2016
Emil Prodan and Hermann Schulz-Baldes Bulk and Boundary Invariants for Complex Topological Insulators Mathematical Physics Studies 10.1007/978-3-319-29351-6_1
1. Illustration of Key Concepts in Dimension Picture 1
Emil Prodan 1
(1)
Physics Department, Yeshiva University, New York, NY, USA
(2)
Department Mathematik, Friedrich-Alexander-Universitt Erlangen-Nrnberg, Erlangen, Bayern, Germany
Emil Prodan (Corresponding author)
Email:
Hermann Schulz-Baldes
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Abstract
This introductory chapter presents and illustrates many of the key concepts developed in this work on a simple example, namely the Su-Schriefer-Heeger model [205] of a conducting polymer. This model has a chiral symmetry and non-trivial topology, given by a non-commutative winding number which is remarkably stable against perturbations like a random potential [139]. Hence this is a relatively simple example of a topological insulator. Here the focus is on the bulk-boundary correspondence in this model, which connects the winding number to the number of edge states weighted by their chirality. This connection will be explained in a K -theoretic manner. These arguments constitute a rather mathematical introduction to the bulk-edge correspondence and the physical motivations and insights will be given in the following chapters.
1.1 Periodic Hamiltonian and Its Topological Invariant
As a general rule, the topology in topological insulators is always inherited from periodic models and this topology can be shown in many instances to be stable under perturbations which also break the periodicity. It is therefore instructive to start out with a detailed analysis of the periodic models and to identify their topological invariants. The one-dimensional periodic Hamiltonian H considered here acts on the Hilbert space Bulk and Boundary Invariants for Complex Topological Insulators - image 2 and is given by
11 where and are the identity operators on - photo 3
(1.1)
where Picture 4 and Picture 5 are the identity operators on and and the Pauli matrices are and S is - photo 6 and and the Pauli matrices are and S is the right shift on - photo 7 and the Pauli matrices are and S is the right shift on while - photo 8 Pauli matrices are
and S is the right shift on while is the mass term The component - photo 9
and S is the right shift on Picture 10 while Picture 11 is the mass term. The component Bulk and Boundary Invariants for Complex Topological Insulators - image 12 of the Hilbert space will be referred to as the fiber. This Hamiltonian goes back to Su et al. [205] and its physical origin will be discussed in Sect.. It has a chiral symmetry w.r.t. the real unitary Bulk and Boundary Invariants for Complex Topological Insulators - image 13 squaring to the identity
Bulk and Boundary Invariants for Complex Topological Insulators - image 14
(1.2)
The Fermi level Picture 15 is always assumed positioned at 0 for chiral symmetric systems, see Chap.. Note that a model with chiral symmetry can display a spectral gap at Bulk and Boundary Invariants for Complex Topological Insulators - image 16 only if the fiber has even dimension, which is obviously the case here.
The discrete Fourier transform Bulk and Boundary Invariants for Complex Topological Insulators - image 17 defined by
Bulk and Boundary Invariants for Complex Topological Insulators - image 18
partially diagonalizes the Hamiltonian to Bulk and Boundary Invariants for Complex Topological Insulators - image 19 with
Bulk and Boundary Invariants for Complex Topological Insulators - image 20
or
Bulk and Boundary Invariants for Complex Topological Insulators - image 21
Also the chiral symmetry operator diagonalizes Bulk and Boundary Invariants for Complex Topological Insulators - image 22 , even with constant fibers Bulk and Boundary Invariants for Complex Topological Insulators - image 23 . The two eigenvalues of Bulk and Boundary Invariants for Complex Topological Insulators - image 24 are
Bulk and Boundary Invariants for Complex Topological Insulators - image 25
and both are N -fold degenerate. Their symmetry around 0 reflects the chiral symmetry Bulk and Boundary Invariants for Complex Topological Insulators - image 26 which, as for any Hamiltonian with chiral symmetry, implies Bulk and Boundary Invariants for Complex Topological Insulators - image 27 . The central gap around 0 is Bulk and Boundary Invariants for Complex Topological Insulators - image 28 with Bulk and Boundary Invariants for Complex Topological Insulators - image 29 . Hence it is open as long as Bulk and Boundary Invariants for Complex Topological Insulators - image 30 . Let us also note that for Bulk and Boundary Invariants for Complex Topological Insulators - image 31 , one has Bulk and Boundary Invariants for Complex Topological Insulators - image 32
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