Effective actions in supersymmetric gauge theories: heat kernels for non-minimal operators

TL;DR

This paper develops a novel method to compute the effective action for supersymmetric gauge theories with non-minimal operators, deriving explicit results for both ${ m N}=1$ and ${ m N}=2$ cases, and extends the heat kernel technique to these complex operators.

Contribution

It introduces a new approach to evaluate the effective action involving non-minimal operators in supersymmetric theories, including explicit formulas and generalizations to higher supersymmetry.

Findings

Derived closed-form induced action for ${ m N}=1$ supersymmetric models.

Extended the method to ${ m N}=2$ supersymmetry, relating it to Kähler potentials.

Computed DeWitt's $a_2$ coefficients for non-supersymmetric non-minimal operators.

Abstract

We study the quantum dynamics of a system of $n$ Abelian ${\cal N}=1$ vector multiplets coupled to $\frac 12 n(n+1)$ chiral multiplets which parametrise the Hermitian symmetric space $\mathsf{Sp}(2n, {\mathbb R})/ \mathsf{U}(n)$. In the presence of supergravity, this model is super-Weyl invariant and possesses the maximal non-compact duality group $\mathsf{Sp}(2n, {\mathbb R})$ at the classical level. These symmetries should be respected by the logarithmically divergent term (the ``induced action'') of the effective action obtained by integrating out the vector multiplets. In computing the effective action, one has to deal with non-minimal operators for which the known heat kernel techniques are not directly applicable, even in flat (super)space. In this paper we develop a method to compute the induced action in Minkowski superspace. The induced action is derived in closed form and has a simple structure. It is a higher-derivative superconformal sigma model on $\mathsf{Sp}(2n, {\mathbb R})/ \mathsf{U}(n)$. The obtained ${\cal N}=1$ results are generalised to the case of ${\cal N}=2$ local supersymmetry: a system of $n$ Abelian ${\cal N}=2$ vector multiplets coupled to ${\cal N}=2$ chiral multiplets $X^I$ parametrising $\mathsf{Sp}(2n, {\mathbb R})/ \mathsf{U}(n)$. The induced action is shown to be proportional to $ \int {\rm d}^4x {\rm d}^4 \theta {\rm d}^4 \bar \theta \, E \, {\mathfrak K}(X, \bar X )$, where ${\mathfrak K}(X, \bar X )$ is the K\"ahler potential for $\mathsf{Sp}(2n, {\mathbb R})/ \mathsf{U}(n)$. We also apply our method to compute DeWitt's $a_2 $ coefficients in some non-supersymmetric theories with non-minimal operators.