Interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrents

Abstract We consider a four dimensional generalized Wess-Zumino model formulated in terms of an arbitrary Kähler potential KΦΦ¯ $$ \mathcal{K}\left(\varPhi, \overline{\varPhi}\right) $$ and an arbitrary chiral superpotential WΦ $$ \mathcal{W}\left(\varPhi \right) $$. A general analysis is given to d...

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Main Authors: I. L. Buchbinder, S. James Gates, Konstantinos Koutrolikos
Format: Article
Language:English
Published: SpringerOpen 2018-05-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP05(2018)204
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spelling doaj-d1d42e48957a4934b3aaa1ba1c1524a32020-11-25T01:10:29ZengSpringerOpenJournal of High Energy Physics1029-84792018-05-012018512710.1007/JHEP05(2018)204Interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrentsI. L. Buchbinder0S. James Gates1Konstantinos Koutrolikos2Department of Theoretical Physics, Tomsk State Pedagogical UniversityDepartment of Physics, Brown UniversityInstitute for Theoretical Physics and Astrophysics, Masaryk UniversityAbstract We consider a four dimensional generalized Wess-Zumino model formulated in terms of an arbitrary Kähler potential KΦΦ¯ $$ \mathcal{K}\left(\varPhi, \overline{\varPhi}\right) $$ and an arbitrary chiral superpotential WΦ $$ \mathcal{W}\left(\varPhi \right) $$. A general analysis is given to describe the possible interactions of this theory with external higher spin gauge superfields of the (s + 1, s + 1/2) supermultiplet via higher spin supercurrents. It is shown that such interactions do not exist beyond supergravity (s ≥ 2) for any K $$ \mathcal{K} $$ and W $$ \mathcal{W} $$. However, we find three exceptions, the theory of a free massless chiral, the theory of a free massive chiral and the theory of a free chiral with linear superpotential. For the first two, the higher spin supercurrents are known and for the third one we provide the explicit expressions. We also discuss the lower spin supercurrents. As expected, a coupling to (non-minimal) supergravity (s = 1) can always be found and we give the generating supercurrent and supertrace for arbitrary K $$ \mathcal{K} $$ and W $$ \mathcal{W} $$. On the other hand, coupling to the vector supermultiplet (s = 0) is possible only if K=KΦ¯Φ $$ \mathcal{K} = \mathcal{K}\left(\overline{\varPhi}\varPhi \right) $$ and W=0 $$ \mathcal{W}=0 $$.http://link.springer.com/article/10.1007/JHEP05(2018)204SuperspacesSupersymmetric Effective Theories
collection DOAJ
language English
format Article
sources DOAJ
author I. L. Buchbinder
S. James Gates
Konstantinos Koutrolikos
spellingShingle I. L. Buchbinder
S. James Gates
Konstantinos Koutrolikos
Interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrents
Journal of High Energy Physics
Superspaces
Supersymmetric Effective Theories
author_facet I. L. Buchbinder
S. James Gates
Konstantinos Koutrolikos
author_sort I. L. Buchbinder
title Interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrents
title_short Interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrents
title_full Interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrents
title_fullStr Interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrents
title_full_unstemmed Interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrents
title_sort interaction of supersymmetric nonlinear sigma models with external higher spin superfields via higher spin supercurrents
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2018-05-01
description Abstract We consider a four dimensional generalized Wess-Zumino model formulated in terms of an arbitrary Kähler potential KΦΦ¯ $$ \mathcal{K}\left(\varPhi, \overline{\varPhi}\right) $$ and an arbitrary chiral superpotential WΦ $$ \mathcal{W}\left(\varPhi \right) $$. A general analysis is given to describe the possible interactions of this theory with external higher spin gauge superfields of the (s + 1, s + 1/2) supermultiplet via higher spin supercurrents. It is shown that such interactions do not exist beyond supergravity (s ≥ 2) for any K $$ \mathcal{K} $$ and W $$ \mathcal{W} $$. However, we find three exceptions, the theory of a free massless chiral, the theory of a free massive chiral and the theory of a free chiral with linear superpotential. For the first two, the higher spin supercurrents are known and for the third one we provide the explicit expressions. We also discuss the lower spin supercurrents. As expected, a coupling to (non-minimal) supergravity (s = 1) can always be found and we give the generating supercurrent and supertrace for arbitrary K $$ \mathcal{K} $$ and W $$ \mathcal{W} $$. On the other hand, coupling to the vector supermultiplet (s = 0) is possible only if K=KΦ¯Φ $$ \mathcal{K} = \mathcal{K}\left(\overline{\varPhi}\varPhi \right) $$ and W=0 $$ \mathcal{W}=0 $$.
topic Superspaces
Supersymmetric Effective Theories
url http://link.springer.com/article/10.1007/JHEP05(2018)204
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