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A pedestrian's guide to the topological phases of free fermions

Frank Schindler

Abstract

These lecture notes explain the classification of some simple fermionic topological phases of matter in a pedestrian manner, with an aim to be maximally pedagogical = doing things in excruciating detail. We focus on a many-body perspective, even if many of the models we work with are non-interacting. We start out with symmetry protected topological (SPT) phases of free fermions that are protected by U(1) symmetry = topological insulators. We then look at fermion topological phases that don't even need a symmetry = topological superconductors, and explain how their classification changes in presence of spinless time-reversal symmetry. We close by perturbatively checking which of the 1D topological phases we had found are stable to interactions.

A pedestrian's guide to the topological phases of free fermions

Abstract

These lecture notes explain the classification of some simple fermionic topological phases of matter in a pedestrian manner, with an aim to be maximally pedagogical = doing things in excruciating detail. We focus on a many-body perspective, even if many of the models we work with are non-interacting. We start out with symmetry protected topological (SPT) phases of free fermions that are protected by U(1) symmetry = topological insulators. We then look at fermion topological phases that don't even need a symmetry = topological superconductors, and explain how their classification changes in presence of spinless time-reversal symmetry. We close by perturbatively checking which of the 1D topological phases we had found are stable to interactions.

Paper Structure

This paper contains 30 sections, 121 equations, 3 figures.

Figures (3)

  • Figure 1: The OBC Kitaev chain Hamiltonian $H_1$ from Eq. \ref{['eq: H1 OBC']}. Each circle represents a Majorana operator $\gamma_\alpha$. Each bar represents a coupling term of the form $\mathrm{i} \gamma_\alpha \gamma_\beta$ that appears in the Hamiltonian.
  • Figure 2: Two copies of $H_1$.
  • Figure 3: Two copies of $H_1$ with local edge couplings.