Superpotentials for superconformal Chern-Simons theories from representation theory

TL;DR

This paper explores the structure of superpotentials in superconformal Chern-Simons theories with matter, linking representation theory to the symmetry constraints and recovering known M2-brane effective theories.

Contribution

It provides a representation-theoretic framework for classifying superpotentials in superconformal Chern-Simons theories, including new insights into metric 3-Lie algebras and their embeddings.

Findings

Classifies matter representations compatible with superconformal symmetry.

Establishes a connection between triple systems and Lie (super)algebras.

Proves embedding of metric 3-Lie algebras into 3-graded Lie superalgebras.

Abstract

These notes provide a detailed account of the universal structure of superpotentials defining a large class of superconformal Chern-Simons theories with matter, many of which appear as the low-energy descriptions of multiple M2-brane configurations. The amount of superconformal symmetry in the Chern-Simons-matter theory determines the minimum amount of global symmetry that the associated quartic superpotential must realise, which in turn restricts the matter superfield representations. Our analysis clarifies the necessary representation-theoretic data which guarantees a particular amount of superconformal symmetry. Thereby we shall recover all the examples of M2-brane effective field theories that have appeared in the recent literature. The results are based on a refinement of the unitary representation theory of Lie algebras to the case when the Lie algebra admits an ad-invariant inner product. The types of representation singled out by the superconformal symmetry turn out to be intimately associated with triple systems admitting embedding Lie (super)algebras and we obtain a number of new results about these triple systems which might be of independent interest. In particular, we prove that any metric 3-Lie algebra embeds into a real metric 3-graded Lie superalgebra in such a way that the 3-bracket is given by a nested Lie bracket.