2015
DOI: 10.1007/s10701-015-9915-4
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Supersymmetric Duality in Deformed Superloop Space

Abstract: In this paper, we will analyse the superloop space formalism for a four dimensional supersymmetric Yang-Mills theory in deformed superspace. We will deform the N = 1 superspace by imposing non-anticommutativity. This non-anticommutative deformation of the superspace will break half the supersymmetry of the original theory. So, this theory will have N = 1/2 supersymmetry. We will analyse the superloop space duality for this deformed supersymmetric Yang-Mills theory using the N = 1/2 superspace formalism. We wil… Show more

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Cited by 4 publications
(15 citation statements)
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“…The loop space formalism has been used to construct loop space duality for ordinary Yang-Mills theories [35,36,37,38]. This duality reduces to the usual electromagnetic Hodge duality for abelian gauge theories.…”
Section: Resultsmentioning
confidence: 99%
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“…The loop space formalism has been used to construct loop space duality for ordinary Yang-Mills theories [35,36,37,38]. This duality reduces to the usual electromagnetic Hodge duality for abelian gauge theories.…”
Section: Resultsmentioning
confidence: 99%
“…Thus, we will have demonstrated that a monopole contribution can generated from deformation of loop space variables. It may be noted that monopoles in general have been analyzed in loop space using a duality which reduces to electromagnetic Hodge duality for abelian theories [35,36,37,38]. However, as far as we know, all such constructions use the loop space formalism, and we are not aware of any proof of this duality using space-time variables alone.…”
Section: Monopole Chargementioning
confidence: 99%
“…The problem with this approach is that it has not been possible to construct a generalization of Hodge duality to non-abelian gauge theories in spacetime. However, it is possible to construct a such a duality in Yang-Mills theories using Polyakov variable [25,23,24,26]. It has also been demonstrated that this duality reduces to the electromagnetic Hodge duality for abelian gauge theories [25].…”
Section: Introductionmentioning
confidence: 99%
“…The connection in the Polyakov loop space is called Polyakov variable. As this Polyakov variable which has been used to construct a nonabelian generalization of Hodge duality [25,23,24,26], and gravity can be constructed as a gauge theory of Lorentz group [17,18,19,20,21,22], we can construct Polyakov variable for gravity, and use it to construct a dual for gravity beyond linearized approximation. It may be noted that this duality has been used in Yang-Mills theories to obtain several interesting results.…”
Section: Introductionmentioning
confidence: 99%
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