Supersymmetric self-dual Yang–Mills theories from local nilpotent fermionic symmetry

We present a system of a self-dual vector-spinor and a self-dual Yang–Mills (YM) field with local nilpotent fermionic symmetry (but not supersymmetry) in D=2+2 dimensions that embeds self-dual supersymmetric YM theory as a special set of exact solutions. Our system has local nilpotent fermionic symm...

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Main Authors: Hitoshi Nishino, Subhash Rajpoot
Format: Article
Language:English
Published: Elsevier 2017-09-01
Series:Physics Letters B
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269317306020
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spelling doaj-4534855d49c940b6a96cd2856ef5d4742020-11-24T23:39:41ZengElsevierPhysics Letters B0370-26931873-24452017-09-01772C73173610.1016/j.physletb.2017.07.046Supersymmetric self-dual Yang–Mills theories from local nilpotent fermionic symmetryHitoshi NishinoSubhash RajpootWe present a system of a self-dual vector-spinor and a self-dual Yang–Mills (YM) field with local nilpotent fermionic symmetry (but not supersymmetry) in D=2+2 dimensions that embeds self-dual supersymmetric YM theory as a special set of exact solutions. Our system has local nilpotent fermionic symmetry generator NαI satisfying the algebra {NαI,NβJ}=0 with the adjoint index I of an arbitrary gauge group. Our original field content in D=2+2 is (AμI,ψμI,χI), where AμI is the usual YM gauge field, ψμI is a Majorana–Weyl vector-spinor gauging NαI, while χI is a Majorana–Weyl spinor compensator field needed for consistency. This system embeds self-dual supersymmetric YM system with the field content (AμI,λ−I) in D=2+2. As other examples, we consider similar systems in D=7+0 and D=8+0 embedding respectively N=1/8+7/8 and N=(1/8,1) supersymmetric YM theories with generalized self-dualities, such as FμνI=(1/2)fμνρσFρσI with a generalized octonionic structure constant fμνρσ. This result strongly suggests that our local nilpotent fermionic symmetry is more fundamental than the supersymmetric self-dual Yang–Mills systems that are supposed to generate all supersymmetric integrable models in D<4.http://www.sciencedirect.com/science/article/pii/S0370269317306020SupersymmetryNilpotent fermionic symmetryNon-Abelian interactionsVector spinorFour, seven and eight dimensionsIntegrable systems
collection DOAJ
language English
format Article
sources DOAJ
author Hitoshi Nishino
Subhash Rajpoot
spellingShingle Hitoshi Nishino
Subhash Rajpoot
Supersymmetric self-dual Yang–Mills theories from local nilpotent fermionic symmetry
Physics Letters B
Supersymmetry
Nilpotent fermionic symmetry
Non-Abelian interactions
Vector spinor
Four, seven and eight dimensions
Integrable systems
author_facet Hitoshi Nishino
Subhash Rajpoot
author_sort Hitoshi Nishino
title Supersymmetric self-dual Yang–Mills theories from local nilpotent fermionic symmetry
title_short Supersymmetric self-dual Yang–Mills theories from local nilpotent fermionic symmetry
title_full Supersymmetric self-dual Yang–Mills theories from local nilpotent fermionic symmetry
title_fullStr Supersymmetric self-dual Yang–Mills theories from local nilpotent fermionic symmetry
title_full_unstemmed Supersymmetric self-dual Yang–Mills theories from local nilpotent fermionic symmetry
title_sort supersymmetric self-dual yang–mills theories from local nilpotent fermionic symmetry
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2017-09-01
description We present a system of a self-dual vector-spinor and a self-dual Yang–Mills (YM) field with local nilpotent fermionic symmetry (but not supersymmetry) in D=2+2 dimensions that embeds self-dual supersymmetric YM theory as a special set of exact solutions. Our system has local nilpotent fermionic symmetry generator NαI satisfying the algebra {NαI,NβJ}=0 with the adjoint index I of an arbitrary gauge group. Our original field content in D=2+2 is (AμI,ψμI,χI), where AμI is the usual YM gauge field, ψμI is a Majorana–Weyl vector-spinor gauging NαI, while χI is a Majorana–Weyl spinor compensator field needed for consistency. This system embeds self-dual supersymmetric YM system with the field content (AμI,λ−I) in D=2+2. As other examples, we consider similar systems in D=7+0 and D=8+0 embedding respectively N=1/8+7/8 and N=(1/8,1) supersymmetric YM theories with generalized self-dualities, such as FμνI=(1/2)fμνρσFρσI with a generalized octonionic structure constant fμνρσ. This result strongly suggests that our local nilpotent fermionic symmetry is more fundamental than the supersymmetric self-dual Yang–Mills systems that are supposed to generate all supersymmetric integrable models in D<4.
topic Supersymmetry
Nilpotent fermionic symmetry
Non-Abelian interactions
Vector spinor
Four, seven and eight dimensions
Integrable systems
url http://www.sciencedirect.com/science/article/pii/S0370269317306020
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