Anomaly constraint on chiral central charge of (2+1)d topological order

In this short paper, we argue that the chiral central charge c_{−} of a (2+1)d topological ordered state is sometimes strongly constrained by 't Hooft anomaly of antiunitary global symmetry. For example, if a (2+1)d fermionic topological quantum field theory (TQFT) has a time-reversal anomaly w...

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Main Author: Ryohei Kobayashi
Format: Article
Language:English
Published: American Physical Society 2021-05-01
Series:Physical Review Research
Online Access:http://doi.org/10.1103/PhysRevResearch.3.023107
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author Ryohei Kobayashi
author_facet Ryohei Kobayashi
author_sort Ryohei Kobayashi
collection DOAJ
description In this short paper, we argue that the chiral central charge c_{−} of a (2+1)d topological ordered state is sometimes strongly constrained by 't Hooft anomaly of antiunitary global symmetry. For example, if a (2+1)d fermionic topological quantum field theory (TQFT) has a time-reversal anomaly with T^{2}=(−1)^{F} labeled as ν∈Z_{16}, the TQFT must have c_{−}=1/4 mod 1/2 for odd ν, while c_{−}=0 mod 1/2 for even ν. This generalizes the fact that the bosonic TQFT with T anomaly in a particular class must carry c_{−}=4 mod 8 to fermionic cases. We also study such a constraint for fermionic TQFT with U(1)×CT symmetry, which is regarded as a gapped surface of the topological superconductor in class AIII.
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spelling doaj.art-e27e34a254bf49e9986b0286bbf745d92024-04-12T17:09:47ZengAmerican Physical SocietyPhysical Review Research2643-15642021-05-013202310710.1103/PhysRevResearch.3.023107Anomaly constraint on chiral central charge of (2+1)d topological orderRyohei KobayashiIn this short paper, we argue that the chiral central charge c_{−} of a (2+1)d topological ordered state is sometimes strongly constrained by 't Hooft anomaly of antiunitary global symmetry. For example, if a (2+1)d fermionic topological quantum field theory (TQFT) has a time-reversal anomaly with T^{2}=(−1)^{F} labeled as ν∈Z_{16}, the TQFT must have c_{−}=1/4 mod 1/2 for odd ν, while c_{−}=0 mod 1/2 for even ν. This generalizes the fact that the bosonic TQFT with T anomaly in a particular class must carry c_{−}=4 mod 8 to fermionic cases. We also study such a constraint for fermionic TQFT with U(1)×CT symmetry, which is regarded as a gapped surface of the topological superconductor in class AIII.http://doi.org/10.1103/PhysRevResearch.3.023107
spellingShingle Ryohei Kobayashi
Anomaly constraint on chiral central charge of (2+1)d topological order
Physical Review Research
title Anomaly constraint on chiral central charge of (2+1)d topological order
title_full Anomaly constraint on chiral central charge of (2+1)d topological order
title_fullStr Anomaly constraint on chiral central charge of (2+1)d topological order
title_full_unstemmed Anomaly constraint on chiral central charge of (2+1)d topological order
title_short Anomaly constraint on chiral central charge of (2+1)d topological order
title_sort anomaly constraint on chiral central charge of 2 1 d topological order
url http://doi.org/10.1103/PhysRevResearch.3.023107
work_keys_str_mv AT ryoheikobayashi anomalyconstraintonchiralcentralchargeof21dtopologicalorder