Odd Laplacians: geometrical meaning of potential, and modular class

TL;DR

This paper explores the geometric interpretation of potentials in second order self-adjoint operators, especially odd Laplacians on supermanifolds, linking them to modular classes and structures like the Nijenhuis bracket.

Contribution

It provides a novel analysis of the potential U as a gauge field in odd Laplacians on supermanifolds, highlighting its primary role and connection to modular classes.

Findings

Potential U acts as a gauge field compensating coordinate transformations.

In odd supermanifolds, the potential becomes a primary geometric object.

The study links modular classes of odd Poisson manifolds with Laplacian operators.

Abstract

A second order self-adjoint operator $\Delta=S\partial^2+U$ is uniquely defined by its principal symbol $S$ and potential $U$ if it acts on half-densities. We analyse the potential $U$ as a compensating field (gauge field) in the sense that it compensates the action of coordinate transformations on the second derivatives in the same way as an affine connection compensates the action of coordinate transformations on first derivatives in the first order operator, a covariant derivative, $\nabla=\partial+\Gamma$. Usually a potential $U$ is derived from other geometrical constructions such as a volume form, an affine connection, or a Riemannian structure, etc. The story is different if $\Delta$ is an odd operator on a supermanifold. In this case the second order potential becomes a primary object. For example, in the case of an odd symplectic supermanifold, the compensating field of the canonical odd Laplacian depends only on this symplectic structure, and can be expressed by the formula obtained by K.Bering. We also study modular classes of odd Poisson manifolds via $\Delta$-operators, and consider an example of a non-trivial modular class which is related with the Nijenhuis bracket.