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Gapped Symmetry Preserving Surface-State for the Electron Topological Insulator
Strongly Correlated Electrons · Submitted 13 Jun 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Here we show that it is possible for the TI surface to be both gapped and symmetry-preserving, at the expense of having surface-topological order.
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The abstract, sentence by sentence
It is well known that the 3D electronic topological insulator (TI) with charge-conservation and time-reversal symmetry cannot have a trivial insulating surface that preserves symmetry. It is often implicitly assumed that if the TI surface preserves both symmetries then it must be gapless. Here we show that it is possible for the TI surface to be both gapped and symmetry-preserving, at the expense of having surface-topological order. In contrast to analogous bosonic topological insulators, this symmetric surface topological order is intrinsically non-Abelian. We show that the surface-topological order provides a complete non-perturbative definition of the electron TI that transcends a free-particle band-structure picture, and could provide a useful perspective for studying strongly correlated topological Mott insulators.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | It is well known that the 3D electronic topological insulator (TI) with charge-conservation and time-reversal symmetry cannot have a trivial insulating surface that preserves symmetry. | background 1.00 | 0.03 | 0.03 | asserted 1.00 |
| s1 | It is often implicitly assumed that if the TI surface preserves both symmetries then it must be gapless. | background 0.92 | 0.03 | 0.03 | asserted 0.62 |
| s2 | Here we show that it is possible for the TI surface to be both gapped and symmetry-preserving, at the expense of having surface-topological order. | result 0.80 | 0.94 | 0.91 | asserted 0.73 |
| s3 | In contrast to analogous bosonic topological insulators, this symmetric surface topological order is intrinsically non-Abelian. | result 0.97 | 0.76 | 0.09 | asserted 1.00 |
| s4 | We show that the surface-topological order provides a complete non-perturbative definition of the electron TI that transcends a free-particle band-structure picture, and could provide a useful perspective for studying strongly correlated topological Mott insulators. | interpretation 0.96 | 0.90 | 0.21 | asserted 0.65 |
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The paper
Original abstract
It is well known that the 3D electronic topological insulator (TI) with charge-conservation and time-reversal symmetry cannot have a trivial insulating surface that preserves symmetry. It is often implicitly assumed that if the TI surface preserves both symmetries then it must be gapless. Here we show that it is possible for the TI surface to be both gapped and symmetry-preserving, at the expense of having surface-topological order. In contrast to analogous bosonic topological insulators, this symmetric surface topological order is intrinsically non-Abelian. We show that the surface-topological order provides a complete non-perturbative definition of the electron TI that transcends a free-particle band-structure picture, and could provide a useful perspective for studying strongly correlated topological Mott insulators.
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References
How the literature uses it
24 arXiv papers cite this in 30 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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Here we discuss a novel possibility in the presence of interactions, a surface phase that preserves all symmetries but is nevertheless gapped and insulating.
Symmetry Enforced Non-Abelian Topological Order at the Surface of a Topological Insulator · 0.84
Papers citing it · 25 sentences without a confident label
Compares with it 1 paper
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Wang et al. [ref] constructing another time-reversal invariant and charge-conserving topological phase, described by the anyon model $.
A Time-Reversal Invariant Topological Phase at the Surface of a 3D Topological Insulator · Conclusion · 0.88
Cites it as background 4 papers
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The other quantum disordered states, which has been studied extensively recently, are so-called a Symmetry Protected Topological (SPT) phase [ref] .
Conflicting Symmetries in Topologically Ordered Surface States of Three-dimensional Bosonic Symmetry Protected Topological Phases · Introduction · 0.90
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For time-reversal-invariant class AII topological insulators (TI) and class DIII superconductors (TSC), several different approaches, including vortex condensation [ref] , coupled layer constructions [ref] and decorated Walker-Wang models [ref] have been pursued and a number of possible STOs have been identified, leading to a rather complete understanding of the classifications of interacting TIs and TSCs in 3 [ref] .
Microscopic Theory of Surface Topological Order for Topological Crystalline Superconductors · Introduction · 0.94
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[ref] A topological order is characterized by a set of anyon types and their topological properties, such as fusion and braiding.
Bulk characterization of topological crystalline insulators: stability under interactions and relations to symmetry enriched U(1) quantum spin liquids · A symmetric surface topological order · 0.93
What it cites · 8 sentences without a confident label
Compares with 3 papers
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Qi [ref] which obtains the same STO as in Ref. [ref] .
A Time-Reversal Invariant Topological Phase at the Surface of a 3D Topological Insulator · Discussion · 0.86
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Qi [ref] which obtains the same STO as in Ref. [ref] .
Symmetry Enforced Non-Abelian Topological Order at the Surface of a Topological Insulator · Discussion · 0.86
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Fisher which obtains the same STO [ref] , and a related work by P.
A symmetry-respecting topologically-ordered surface phase of 3d electron topological insulators · Discussion · 0.86
Cites as background 1 paper
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For boson TIs, the lens of STO provides a useful perspective into 3+1D strongly correlated boson TIs as well as 2+1D gauge theories [ref] .
Boson topological insulators: A window into highly entangled quantum phases · Discussion · 0.81
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