Superspace First Order Formalism, Trivial Symmetries and Electromagnetic Interactions of Linearized Supergravity

TL;DR

This paper develops a first order superspace formalism for linearized non-minimal supergravity, constructs electromagnetic interaction vertices, and explores trivial symmetries, extending previous non-supersymmetric results to supersymmetric theories.

Contribution

It introduces a novel first order superspace description of non-minimal supergravity and constructs supersymmetric electromagnetic interaction vertices with implications for gauge symmetry deformations.

Findings

Superspace action expressed with a single superfield after integrating out auxiliary fields.

Constructed cubic interaction vertex for supergravity multiplets and vector multiplet.

Showed that the interaction depends on the vector superfield strength, generalizing non-supersymmetric results.

Abstract

We introduce a first order description of linearized non-minimal ($n=-1$) supergravity in superspace, using the unconstrained prepotential superfield instead of the conventionally constrained super one forms. In this description, after integrating out the connection-like auxiliary superfield of first-order formalism, the superspace action is expressed in terms of a single superfield which combines the prepotential and compensator superfields. We use this description to construct the supersymmetric cubic interaction vertex $3/2-3/2-1/2$ which describes the electromagnetic interaction between two non-minimal supergravity multiplets (superspin $\textsf{Y}=3/2$ which contains a spin 2 and a spin 3/2 particles) and a vector multiplet (superspin $\textsf{Y}=1/2$ contains a spin 1 and a spin 1/2 particles). Exploring the trivial symmetries emerging between the two $\textsf{Y}=3/2$ supermultiplets, we show that this cubic vertex must depend on the vector multiplet superfield strength. This result generalize previous results for non-supersymmetric electromagnetic interactions of spin 2 particles. The constructed cubic interaction generates non-trivial deformations of the gauge transformations.