|analytic integration||cohomological integration|
|measurable space||Poincaré duality|
|measure||orientation in generalized cohomology|
|volume form||(virtual) fundamental class|
|Riemann/Lebesgue integration of differential forms||push-forward in generalized cohomology/in differential cohomology|
Here we discuss the integration of a differential form (possibly twisted in some way) on a topological manifold (possibly with additional structure) over an appropriately structured submanifold (or formal linear combination thereof).
See at differential form for basic definitions.
Let be an -dimensional topological manifold, and let be a continuous -pseudoform on . Suppose that is paracompact and Hausdorff, so that we may find a locally finite cover of with a subordinate partition of unity and a continuous coordinate chart on each patch. (When is differentiable, or even smooth, then these may also be chosen to be differentiable or smooth, which may be convenient but is not necessary.) Then defines a measure on as follows:
On each coordinate patch , fix the orientation given by the coordinates to turn into an untwisted -form ; then write in coordinates as
In this situation, it is convenient also to write
in other words, we interpret as the absolute value of .
The coordinates on define a diffeomorphism between and an open subset of that we'll also call ; so use the latter formula to interpret
where the right-hand side is now interpreted in the usual way as as integral with respect to Lebesgue measure.
Using the partition of unity, write
where is a weight function defined on and is the restriction of to . Then we have
or more generally,
for a measurable subset of and the characteristic function of .
A priori, this definition depends not only on the particular coordinate patches chosen but also on the partition of unity chosen to go with them. Furthermore, the defintion could be done just as easily (perhaps even more easily) for something other than an -pseudoform. But the (perhaps surprising) fact that justifies it all is this:
When is an -pseudoform, the definition of is independent of the coordinates and partition chosen. Furthermore, the map from -pseudoforms to measures is linear.
Note that, if were an -form instead of a pseudoform, then the definition would depend on the orientation of the coordinates chosen. We could fix that by using the absolute value in place of in (1) and the following equations, but then the map from forms to measures would not be linear.
It may also be enlightening to consider how to go back from a measure to an -pseudoform. If is an absolutely continuous Radon measure on , then it defines an -pseudoform (which we may also call ) as follows:
Again, this definition is independent of the coordinate system chosen (as long as it extends the given vectors); or if that's not true, then we messed up and need to add further restrictions to the absolutely continuous Radon measure . The definition is not independent of the orientation chosen, of course; thus we get a pseudoform rather than an untwisted form. You might try to ignore the orientation and take to be always, but that does not define an exterior form, as is most easily seen if two vectors are switched (which does not change ). Instead, this would define an absolute differential form (which is equivalent to a pseudoform when, as here, the degree equals the dimension).
One can integrate forms other than -pseudoforms, of course, but only over certain structures within the manifold . Specifically, if is a -dimensional submanifold of (that is a -dimensional manifold equipped with a map ), then we would like to integrate -forms or -pseudoforms (defined on ) over . Here is how we do this:
We may integrate a -form over if is oriented, that is if is oriented. We pull back from to , then use the orientation on to turn into a -pseudoform, which we can then integrate on the -dimensional manifold .
We may integrate a -pseudoform over if is pseudooriented, that is if it is equipped with a map that, for each point on , takes a local orientation of at to a local orientation of at , continuously in and taking opposite orientations to opposite orientations. Then locally, we turn into a -form on using a local orientation on , pull that back to , and use the corresponding local orientation on to turn that back into a -pseudoform, which we can then integrate on .
Thus, while integration of -pseudoforms is the most basic, integration of general -forms is actually a bit simpler than integration of general -pseudoforms. Integration of other twisted or vector-valued forms can also be done, again given appropriate structure on .
Note that, if is thought of a submanifold of itself, then it has a natural pseudoorientation that takes each local orientation to itself, and so we recover the original definition of integration of -pseudoforms on . Also, if is an oriented manifold, then it may be viewed as an oriented submanifold of itself, giving a definition of integration of -forms on .
One often sees the definition of integration given for parametrised submanifolds, that is submanifolds where is an open subset of . This amounts to a combination of the concepts above, with the two uses of (as a coordinate patch in or as the source of a submanifold of ) identified. The theorem that the integral of an -pseudoform on is independent of the coordinates chosen now becomes a theorem that the integral of a parametrised submanifold is independent of the parametrisation (up to some details about orientation), which in the end returns the result that one can integrate forms over arbitrary submanifolds (given an orientation or pseudoorientation as above).
We discuss here a general abstract formulation of differential forms, their integration and the Stokes theorem in cohesive (∞,1)-toposes, hence the axiomatics of cohesive homotopy type theory (following Bunke-Nikolaus-Völkl 13, theorem 3.2).
As usual (see at structures in a cohesive ∞-topos – de Rham cohomology) we deduce from this the secondary cohesive modalities and : for a pointed object with loop space object (for instance the delooping ) is defined by the long homotopy fiber sequence
(Beware that elsewhere we write for what here we write .)
Dually is defined.
We assume that there is an interval object
“exhibiting the cohesion” (see at continuum) in that there is a (chosen) equivalence between the shape modality and the localization at the the projection maps out of Cartesian products with this line
It follows in particular that there is a chosen equivalence of (∞,1)-categories
Throughout in the following we leave the “inclusion” of “differential forms regarded as -connections on trivial -bundles” implicit.
Integration of differential forms is the morphism
The Stokes theorem holds:
An exposition with an eye towards applications in physics is in section 3 of