nLab integration over supermanifolds




Integration theory



There are different ways to define a differential volume element on a smooth manifold. Some of these definitions can be carried over to supergeometry, others cannot. The possibly most familiar way of talking about differential volume elements, in terms of top-degree differential forms, does not carry over to supermanifolds.

No top-degree forms in supergeometry

In supergeometry the notion of top-degree form does not in general make sense, since there are no top-degree wedge powers of “odd 1-forms”: if for instance θ 1\theta_1 and θ 2\theta_2 are odd functions on some super Cartesian space p|q\mathbb{R}^{p|q} and dθ 1d \theta_1 and dθ 2d \theta_2 are their differential 1-forms, then the wedge product of these is symmetric in that

dθ 1dθ 2=+dθ 2dθ 1. d\theta_1 \wedge d \theta_2 = + d\theta_2 \wedge d \theta_1 \,.

Notice the plus sign on the right, which is the product of one minus sign for interchanging θ 1\theta_1 and θ 2\theta_2, and another minus sign for interchanging the two differentials. See at signs in supergeometry for more on this.

Accordingly, the wedge product of the differential of an odd function θ\theta with itself does not in general vanish:

(dθdθ=0)(θ=0). (d \theta \wedge d\theta = 0) \Leftrightarrow (\theta = 0) \,.

On the cartesian supermanifold n|m\mathbb{R}^{n|m} with canonical even coordinate functions {x i} 1 n\{x^i\}_1^n and canonical odd coordinate functions {θ j} 1 m\{\theta^j\}_1^m the differential form which one would want to regard as the canonical volume form is

ω:=dx 1dx ndθ 1dθ m. \omega := d x^1 \wedge \cdots \wedge d x^n \wedge d\theta^1 \wedge \cdots \wedge d\theta^m \,.

Due to the above, this is not a top form, since for instance

ωdθ 10. \omega \wedge d\theta^1 \neq 0 \,.

But this example also indicates the solution: apparently for integration it is not really essential that a form is a top power, what is rather essential is that it is, locally, the wedge product of a basis of 1-forms. This perspective then does lead to a sensible definition of volume forms (and more generally “integrable forms”) on supermanifolds, described below.


Therefore the naïve identification of differential volume measures with top degree forms has to be refined. The idea is to characterize a volume form by other means, in particular as an equivalence class of choices of bases for the space of 1-forms, and then to define integrable forms to be pairs consisting of such a generalized volume form and a multivector: this pair is supposed to represent the differential form one would obtain could one contract the multivector with the volume form, as in ordinary differential geometry.

The definition of integration of integrable forms in supergeometry in terms of multivector fields leads, in the case that the supermanifold in an NQ-supermanifold to the BV formalism.



A general abstract discussion in terms of D-module theory:

Geometric discussion of picture number appearing in the context of integration over supermanifolds (and originally seen in the quantization of the NSR superstring, crucial in superstring field theory) is due to

and further amplified in

In this perspective picture number is an extra grading on differential forms on supermanifolds induced from a choice of integral top-form needed to define integration over supermanifolds:


See also:

  • Sergio L. Cacciatori, Simone Noja, Riccardo Re, The Unifying Double Complex on Supermanifolds (arXiv:2004.10906)

Last revised on March 9, 2024 at 03:21:15. See the history of this page for a list of all contributions to it.