2019•Journal of High Energy PhysicsOpen access

The $$ \mathcal{N} $$ = 3 Weyl multiplet in four dimensions

Jesse van Muiden, Antoine Van Proeyen

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Abstract

Abstract The main ingredient for local superconformal methods is the multiplet of gauge fields: the Weyl multiplet. We construct the transformations of this multiplet for $$ \mathcal{N} $$ N = 3, D = 4. The construction is based on a supersymmetry truncation from the $$ \mathcal{N} $$ N = 4 Weyl multiplet, on coupling with a current multiplet, and on the implementation of a soft algebra at the nonlinear level, extending $$ \mathfrak{s}\mathfrak{u} $$ s u (2, 2|3). This is the first step towards a superconformal calculus for $$ \mathcal{N} $$ N = 3, D = 4.

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Abstract The main ingredient for local superconformal methods is the multiplet of gauge fields: the Weyl multiplet. We construct the transformations of this multiplet for $$ \mathcal{N} $$ N = 3, D = 4. The construction is based on a supersymmetry truncation from the $$ \mathcal{N} $$ N = 4 Weyl multiplet, on coupling with a current multiplet, and on the implementation of a soft algebra at the nonlinear level, extending $$ \mathfrak{s}\mathfrak{u} $$ s u (2, 2|3). This is the first step towards a superconformal calculus for $$ \mathcal{N} $$ N = 3, D = 4.

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Available abstract

Abstract The main ingredient for local superconformal methods is the multiplet of gauge fields: the Weyl multiplet. We construct the transformations of this multiplet for $$ \mathcal{N} $$ N = 3, D = 4. The construction is based on a supersymmetry truncation from the $$ \mathcal{N} $$ N = 4 Weyl multiplet, on coupling with a current multiplet, and on the implementation of a soft algebra at the nonlinear level, extending $$ \mathfrak{s}\mathfrak{u} $$ s u (2, 2|3). This is the first step towards a superconformal calculus for $$ \mathcal{N} $$ N = 3, D = 4.

Key concepts: Multiplet, Physics, Coupling (piping), Truncation (statistics), Supersymmetry, Gauge (firearms), Mathematical physics, Theoretical physics

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