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Record W4400081780 · doi:10.1103/physrevx.14.021053

Classification of Symmetry-Enriched Topological Quantum Spin Liquids

2024· article· en· W4400081780 on OpenAlexafffund
Weicheng Ye, Liujun Zou

Bibliographic record

VenuePhysical Review X · 2024
Typearticle
Languageen
FieldPhysics and Astronomy
TopicAdvanced Condensed Matter Physics
Canadian institutionsPerimeter Institute
FundersMinistry of Colleges and UniversitiesInstitut Périmètre de physique théoriquePeking University
KeywordsSymmetry (geometry)QuantumSpin (aerodynamics)PhysicsTheoretical physicsTopology (electrical circuits)Condensed matter physicsQuantum mechanicsMathematicsGeometryCombinatorics

Abstract

fetched live from OpenAlex

We present a systematic framework to classify symmetry-enriched topological quantum spin liquids in two spatial dimensions. This framework can deal with all topological quantum spin liquids, which may be either Abelian or non-Abelian and chiral or nonchiral. It can systematically treat a general symmetry, which may include both lattice symmetry and internal symmetry, may contain antiunitary symmetry, and may permute anyons. The framework applies to all types of lattices and can systematically distinguish different lattice systems with the same symmetry group using their quantum anomalies, which are sometimes known as Lieb-Schultz-Mattis anomalies. We apply this framework to classify <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi mathvariant="normal">U</a:mi><a:mo stretchy="false">(</a:mo><a:mn>1</a:mn><a:msub><a:mo stretchy="false">)</a:mo><a:mrow><a:mn>2</a:mn><a:mi>N</a:mi></a:mrow></a:msub></a:math> chiral states and non-Abelian <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"><f:mrow><f:msup><f:mrow><f:mi>Ising</f:mi></f:mrow><f:mrow><f:mo stretchy="false">(</f:mo><f:mi>ν</f:mi><f:mo stretchy="false">)</f:mo></f:mrow></f:msup></f:mrow></f:math> states enriched by a <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"><j:mi>p</j:mi><j:mn>6</j:mn><j:mo>×</j:mo><j:mrow><j:mi>SO</j:mi></j:mrow><j:mo stretchy="false">(</j:mo><j:mn>3</j:mn><j:mo stretchy="false">)</j:mo></j:math> or <n:math xmlns:n="http://www.w3.org/1998/Math/MathML" display="inline"><n:mi>p</n:mi><n:mn>4</n:mn><n:mo>×</n:mo><n:mrow><n:mi>SO</n:mi></n:mrow><n:mo stretchy="false">(</n:mo><n:mn>3</n:mn><n:mo stretchy="false">)</n:mo></n:math> symmetry and <r:math xmlns:r="http://www.w3.org/1998/Math/MathML" display="inline"><r:msub><r:mi mathvariant="double-struck">Z</r:mi><r:mi>N</r:mi></r:msub></r:math> topological orders and <u:math xmlns:u="http://www.w3.org/1998/Math/MathML" display="inline"><u:mi mathvariant="normal">U</u:mi><u:mo stretchy="false">(</u:mo><u:mn>1</u:mn><u:msub><u:mo stretchy="false">)</u:mo><u:mrow><u:mn>2</u:mn><u:mi>N</u:mi></u:mrow></u:msub><u:mo>×</u:mo><u:mi mathvariant="normal">U</u:mi><u:mo stretchy="false">(</u:mo><u:mn>1</u:mn><u:msub><u:mo stretchy="false">)</u:mo><u:mrow><u:mo>−</u:mo><u:mn>2</u:mn><u:mi>N</u:mi></u:mrow></u:msub></u:math> topological orders enriched by a <cb:math xmlns:cb="http://www.w3.org/1998/Math/MathML" display="inline"><cb:mi>p</cb:mi><cb:mn>6</cb:mn><cb:mi>m</cb:mi><cb:mo>×</cb:mo><cb:mrow><cb:mi>SO</cb:mi></cb:mrow><cb:mo stretchy="false">(</cb:mo><cb:mn>3</cb:mn><cb:mo stretchy="false">)</cb:mo><cb:mo>×</cb:mo><cb:msubsup><cb:mi mathvariant="double-struck">Z</cb:mi><cb:mn>2</cb:mn><cb:mi>T</cb:mi></cb:msubsup></cb:math>, <hb:math xmlns:hb="http://www.w3.org/1998/Math/MathML" display="inline"><hb:mi>p</hb:mi><hb:mn>4</hb:mn><hb:mi>m</hb:mi><hb:mo>×</hb:mo><hb:mrow><hb:mi>SO</hb:mi></hb:mrow><hb:mo stretchy="false">(</hb:mo><hb:mn>3</hb:mn><hb:mo stretchy="false">)</hb:mo><hb:mo>×</hb:mo><hb:msubsup><hb:mi mathvariant="double-struck">Z</hb:mi><hb:mn>2</hb:mn><hb:mi>T</hb:mi></hb:msubsup></hb:math>, <mb:math xmlns:mb="http://www.w3.org/1998/Math/MathML" display="inline"><mb:mi>p</mb:mi><mb:mn>6</mb:mn><mb:mi>m</mb:mi><mb:mo>×</mb:mo><mb:msubsup><mb:mi mathvariant="double-struck">Z</mb:mi><mb:mn>2</mb:mn><mb:mi>T</mb:mi></mb:msubsup></mb:math>, or <pb:math xmlns:pb="http://www.w3.org/1998/Math/MathML" display="inline"><pb:mi>p</pb:mi><pb:mn>4</pb:mn><pb:mi>m</pb:mi><pb:mo>×</pb:mo><pb:msubsup><pb:mi mathvariant="double-struck">Z</pb:mi><pb:mn>2</pb:mn><pb:mi>T</pb:mi></pb:msubsup></pb:math> symmetry, where <sb:math xmlns:sb="http://www.w3.org/1998/Math/MathML" display="inline"><sb:mi>p</sb:mi><sb:mn>6</sb:mn></sb:math>, <ub:math xmlns:ub="http://www.w3.org/1998/Math/MathML" display="inline"><ub:mi>p</ub:mi><ub:mn>4</ub:mn></ub:math>, <wb:math xmlns:wb="http://www.w3.org/1998/Math/MathML" display="inline"><wb:mi>p</wb:mi><wb:mn>6</wb:mn><wb:mi>m</wb:mi></wb:math>, and <yb:math xmlns:yb="http://www.w3.org/1998/Math/MathML" display="inline"><yb:mi>p</yb:mi><yb:mn>4</yb:mn><yb:mi>m</yb:mi></yb:math> are lattice symmetries while SO(3) and <ac:math xmlns:ac="http://www.w3.org/1998/Math/MathML" display="inline"><ac:msubsup><ac:mi mathvariant="double-struck">Z</ac:mi><ac:mn>2</ac:mn><ac:mi>T</ac:mi></ac:msubsup></ac:math> are spin rotation and time-reversal symmetries, respectively. In particular, we identify symmetry-enriched topological quantum spin liquids that are not easily captured by the usual parton-mean-field approach, including examples with the familiar <dc:math xmlns:dc="http://www.w3.org/1998/Math/MathML" display="inline"><dc:msub><dc:mi mathvariant="double-struck">Z</dc:mi><dc:mn>2</dc:mn></dc:msub></dc:math> topological order. Published by the American Physical Society 2024

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How this classification was reachedexpand

Full frame distilled prediction

Teacher imitation

Not calibrated prevalence, not ground truth. Human validation pending. Learned from the 10,348 direct Codex labels and 10,348 direct Gemma labels. Candidate is the union of thresholded teacher heads; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels or direct frontier model labels.

metaresearch head score (Codex)0.000
metaresearch head score (Gemma)0.000
Version: codex-gemma-dda1882f352aValidation status: machine_predicted_unvalidated
Candidate categoriesnone
Consensus categoriesnone
DomainCandidate signal: none · Consensus signal: none
Study designCandidate signal: Theoretical or conceptual · Consensus signal: Theoretical or conceptual
GenreCandidate signal: Empirical · Consensus signal: Empirical
Teacher disagreement score0.208
Threshold uncertainty score0.552

Codex and Gemma teacher scores by category

CategoryCodexGemma
Metaresearch0.0000.000
Meta-epidemiology (narrow)0.0000.000
Meta-epidemiology (broad)0.0000.000
Bibliometrics0.0000.000
Science and technology studies0.0000.000
Scholarly communication0.0000.000
Open science0.0000.000
Research integrity0.0000.000
Insufficient payload (model declined to judge)0.0000.000

Machine scores (provisional)

The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.

Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.

Opus teacher head0.028
GPT teacher head0.363
Teacher spread0.334 · how far apart the two teachers sit on this one work
Validation statusscore_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from it

Classification

machine, unvalidated

Machine predicted; a candidate call from one teacher head, not a consensus.

The models applied no category: nothing in the taxonomy fit this work.
Study designTheoretical or conceptual
Domainnot available
GenreEmpirical

How this classification was reached, model by model and score by score, is at the end of the page under "How this classification was reached".

Quick stats

Citations7
Published2024
Admission routes2
Has abstractyes

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