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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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 |
work_keys_str_mv |
AT hitoshinishino supersymmetricselfdualyangmillstheoriesfromlocalnilpotentfermionicsymmetry AT subhashrajpoot supersymmetricselfdualyangmillstheoriesfromlocalnilpotentfermionicsymmetry |
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1725512328606121984 |