Bootstrapping the minimal 3D SCFT

Abstract We study the conformal bootstrap constraints for 3D conformal field theories with a ℤ 2 or parity symmetry, assuming a single relevant scalar operator ϵ that is invariant under the symmetry. When there is additionally a single relevant odd scalar σ, we map out the allowed space of dimension...

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Main Authors: Alexander Atanasov, Aaron Hillman, David Poland
Format: Article
Language:English
Published: SpringerOpen 2018-11-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP11(2018)140
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spelling doaj-62346854d449470ba3d4b416c6f88ab62020-11-25T01:58:53ZengSpringerOpenJournal of High Energy Physics1029-84792018-11-0120181111510.1007/JHEP11(2018)140Bootstrapping the minimal 3D SCFTAlexander Atanasov0Aaron Hillman1David Poland2Department of Physics, Yale UniversityDepartment of Physics, Yale UniversityDepartment of Physics, Yale UniversityAbstract We study the conformal bootstrap constraints for 3D conformal field theories with a ℤ 2 or parity symmetry, assuming a single relevant scalar operator ϵ that is invariant under the symmetry. When there is additionally a single relevant odd scalar σ, we map out the allowed space of dimensions and three-point couplings of such “Ising-like” CFTs. If we allow a second relevant odd scalar σ′, we identify a feature in the allowed space compatible with 3D N $$ \mathcal{N} $$ = 1 superconformal symmetry and conjecture that it corresponds to the minimal N $$ \mathcal{N} $$ = 1 supersymmetric extension of the Ising CFT. This model has appeared in previous numerical bootstrap studies, as well as in proposals for emergent supersymmetry on the boundaries of topological phases of matter. Adding further constraints from 3D N $$ \mathcal{N} $$ =1 superconformal symmetry, we isolate this theory and use the numerical bootstrap to compute the leading scaling dimensions Δ σ = Δ ϵ − 1 = .58444(22) and three-point couplings λ σσϵ = 1.0721(2) and λ ϵϵϵ = 1.67(1). We additionally place bounds on the central charge and use the extremal functional method to estimate the dimensions of the next several operators in the spectrum. Based on our results we observe the possible exact relation λ ϵϵϵ /λ σσϵ = tan(1).http://link.springer.com/article/10.1007/JHEP11(2018)140Conformal and W SymmetryConformal Field TheoryNonperturbative EffectsSupersymmetry and Duality
collection DOAJ
language English
format Article
sources DOAJ
author Alexander Atanasov
Aaron Hillman
David Poland
spellingShingle Alexander Atanasov
Aaron Hillman
David Poland
Bootstrapping the minimal 3D SCFT
Journal of High Energy Physics
Conformal and W Symmetry
Conformal Field Theory
Nonperturbative Effects
Supersymmetry and Duality
author_facet Alexander Atanasov
Aaron Hillman
David Poland
author_sort Alexander Atanasov
title Bootstrapping the minimal 3D SCFT
title_short Bootstrapping the minimal 3D SCFT
title_full Bootstrapping the minimal 3D SCFT
title_fullStr Bootstrapping the minimal 3D SCFT
title_full_unstemmed Bootstrapping the minimal 3D SCFT
title_sort bootstrapping the minimal 3d scft
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2018-11-01
description Abstract We study the conformal bootstrap constraints for 3D conformal field theories with a ℤ 2 or parity symmetry, assuming a single relevant scalar operator ϵ that is invariant under the symmetry. When there is additionally a single relevant odd scalar σ, we map out the allowed space of dimensions and three-point couplings of such “Ising-like” CFTs. If we allow a second relevant odd scalar σ′, we identify a feature in the allowed space compatible with 3D N $$ \mathcal{N} $$ = 1 superconformal symmetry and conjecture that it corresponds to the minimal N $$ \mathcal{N} $$ = 1 supersymmetric extension of the Ising CFT. This model has appeared in previous numerical bootstrap studies, as well as in proposals for emergent supersymmetry on the boundaries of topological phases of matter. Adding further constraints from 3D N $$ \mathcal{N} $$ =1 superconformal symmetry, we isolate this theory and use the numerical bootstrap to compute the leading scaling dimensions Δ σ = Δ ϵ − 1 = .58444(22) and three-point couplings λ σσϵ = 1.0721(2) and λ ϵϵϵ = 1.67(1). We additionally place bounds on the central charge and use the extremal functional method to estimate the dimensions of the next several operators in the spectrum. Based on our results we observe the possible exact relation λ ϵϵϵ /λ σσϵ = tan(1).
topic Conformal and W Symmetry
Conformal Field Theory
Nonperturbative Effects
Supersymmetry and Duality
url http://link.springer.com/article/10.1007/JHEP11(2018)140
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