Broken (super) conformal Ward identities at finite temperature

Abstract When a (super) conformal field theory is placed on a non-trivial manifold, the (super) conformal symmetry is broken. However, it is still possible to derive broken Ward identities for these broken symmetries, which provide additional constraints on the theory. We derive and apply the broken...

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Main Authors: Enrico Marchetto, Alessio Miscioscia, Elli Pomoni
Format: Article
Language:English
Published: SpringerOpen 2023-12-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP12(2023)186
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author Enrico Marchetto
Alessio Miscioscia
Elli Pomoni
author_facet Enrico Marchetto
Alessio Miscioscia
Elli Pomoni
author_sort Enrico Marchetto
collection DOAJ
description Abstract When a (super) conformal field theory is placed on a non-trivial manifold, the (super) conformal symmetry is broken. However, it is still possible to derive broken Ward identities for these broken symmetries, which provide additional constraints on the theory. We derive and apply the broken Ward identities associated with the (super) conformal group on the thermal manifold M β = S β 1 × ℝ d − 1 $$ {\mathcal{M}}_{\beta }={S}_{\beta}^1\times {\mathbb{R}}^{d-1} $$ and M = T 2 × ℝ d − 2 $$ \mathcal{M}={T}^2\times {\mathbb{R}}^{d-2} $$ . The novel constraints not only systematically reproduce known results, including an implicit formulation of the generalized Cardy formula, but also elegantly relate the thermal energy spectrum with the conformal spectrum.
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spelling doaj.art-d692c2e11da040f0bc6e41564b66ab612024-03-31T11:08:21ZengSpringerOpenJournal of High Energy Physics1029-84792023-12-0120231214810.1007/JHEP12(2023)186Broken (super) conformal Ward identities at finite temperatureEnrico Marchetto0Alessio Miscioscia1Elli Pomoni2Mathematical Institute, University of OxfordDeutsches Elektronen-Synchrotron DESYDeutsches Elektronen-Synchrotron DESYAbstract When a (super) conformal field theory is placed on a non-trivial manifold, the (super) conformal symmetry is broken. However, it is still possible to derive broken Ward identities for these broken symmetries, which provide additional constraints on the theory. We derive and apply the broken Ward identities associated with the (super) conformal group on the thermal manifold M β = S β 1 × ℝ d − 1 $$ {\mathcal{M}}_{\beta }={S}_{\beta}^1\times {\mathbb{R}}^{d-1} $$ and M = T 2 × ℝ d − 2 $$ \mathcal{M}={T}^2\times {\mathbb{R}}^{d-2} $$ . The novel constraints not only systematically reproduce known results, including an implicit formulation of the generalized Cardy formula, but also elegantly relate the thermal energy spectrum with the conformal spectrum.https://doi.org/10.1007/JHEP12(2023)186Scale and Conformal SymmetriesSupersymmetry BreakingThermal Field Theory
spellingShingle Enrico Marchetto
Alessio Miscioscia
Elli Pomoni
Broken (super) conformal Ward identities at finite temperature
Journal of High Energy Physics
Scale and Conformal Symmetries
Supersymmetry Breaking
Thermal Field Theory
title Broken (super) conformal Ward identities at finite temperature
title_full Broken (super) conformal Ward identities at finite temperature
title_fullStr Broken (super) conformal Ward identities at finite temperature
title_full_unstemmed Broken (super) conformal Ward identities at finite temperature
title_short Broken (super) conformal Ward identities at finite temperature
title_sort broken super conformal ward identities at finite temperature
topic Scale and Conformal Symmetries
Supersymmetry Breaking
Thermal Field Theory
url https://doi.org/10.1007/JHEP12(2023)186
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AT alessiomiscioscia brokensuperconformalwardidentitiesatfinitetemperature
AT ellipomoni brokensuperconformalwardidentitiesatfinitetemperature