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Interacting fermionic topological insulators/superconductors in three dimensions

4 Pith papers cite this work. Polarity classification is still indexing.

4 Pith papers citing it
abstract

Symmetry Protected Topological (SPT) phases are a minimal generalization of the concept of topological insulators to interacting systems. In this paper we describe the classification and properties of such phases for three dimensional(3D) electronic systems with a number of different symmetries. For symmetries representative of all classes in the famous 10-fold way of free fermion topological insulators/superconductors, we determine the stability to interactions. By combining with results on bosonic SPT phases we obtain a classification of electronic 3D SPT phases for these symmetries. In cases with a normal U(1) subgroup we show that this classification is complete. We describe the non-trivial surface and bulk properties of these states. In particular we discuss interesting correlated surface states that are not captured in a free fermion description. We show that in many, but not all cases, the surface can be gapped while preserving symmetry if it develops intrinsic topological order.

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2026 3 2025 1

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Symmetry Spans and Enforced Gaplessness

cond-mat.str-el · 2026-02-12 · unverdicted · novelty 8.0

Symmetry spans enforce gaplessness when a symmetry E embedded into two larger symmetries C and D has no compatible gapped phase that restricts from both.

Symmetry-Enforced Fermi Surfaces

cond-mat.str-el · 2025-12-03 · unverdicted · novelty 7.0

A noncompact Lie group symmetry generated by U(1) fermion number and Majorana translations enforces Fermi surfaces that generically have at least two noncontractible components in d-dimensional Bravais lattices.

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  • Symmetry-Enforced Fermi Surfaces cond-mat.str-el · 2025-12-03 · unverdicted · none · ref 3 · internal anchor

    A noncompact Lie group symmetry generated by U(1) fermion number and Majorana translations enforces Fermi surfaces that generically have at least two noncontractible components in d-dimensional Bravais lattices.