and
orientation, spin structure, string structure, fivebrane structure
smooth manifold, Riemannian manifold, complex manifold?
Contents
FQFT and cohomology
-Dimensional manifolds (possibly and usually equipped with certain structure, notably for instance with orientation) should naturally form an (∞,n)-category of extended cobordisms whose
objects are 0-dimensional (oriented) manifolds (disjoint unions of (oriented) points);
1-morphisms are (oriented) cobordisms between disjoint unions of (oriented) points;
2-morphisms are cobordisms between 1-dimensional cobordisms
etc.
(n+1)-morphims are diffeomorphisms between -dimensional cobordisms;
(n+2)-morphisms are smooth homotopies of these;
etc.
The -category of cobordisms is the subject of the cobordism hypothesis.
Here is an outline of the idea of the definition of as given in
where the main point, apart from the (∞,n)-category machinery in the background, is definition 2.2.9.
The idea is to start with thinking of -dimensional cobordisms as forming something like an n-fold category by simply saying that the collection of composites of cobordisms is given by big cobordisms with markings on them, indicating where we think of them as being composed.
Let’s first do this for composition in one direction, as in an ordinary 1-category of -dimensional cobordisms.
consider a manifold embedded in a vector space of the form . We can think of this as a manifold canonically equipped with a coordinate function that measures the “height” or maybe better the “length” of the embedded manifold.
We can pick a bunch of numbers and think of these as marking a bunch of slices of , the preimages . We can think of these slices as being the -dimensional boundary manifolds at which a sequence of manifolds have been glued together to produce .
(there is an obvious picture to be drawn and uploaded here, maybe somebody finds the time and energy)
In this way an embedded manifold and a set of -numbers may represent an element in the space of sequences of composable cobordisms. To make this work as expected, the markings on may not be too irregular, so we should impose some conditions on what qualifies as a marked manifold. The precise statement is given further below.
The collection of these tuples, consisting of an embedded manifold and a collection of numbers naturally form a simplicial set, which is like the nerve of the 1-category of -dimensional cobordisms under composition in one direction.
To generalize this from just a 1-categorical structure to an -categorical structure, we simply take a manifold as before, but now draw markings on it in transversal directions, thereby putting a kind of grid on it that subdivides the manifold into cubical slices. A manifold with such subdivision on it may then be regarded as giving an element in the space of -dimensional pasting diagrams in an -fold category.
To formalize this more general case, we embed not just into a , but a . This then provides us with different coordinate functions on , each running along one of the directions in which we may think of as having been glued from smaller manifolds.
A collection of markings indicating such gluing is now a collection of numbers , one for each of these directions.
For each direction this yields a simplicial set of such structures, to be thought of as the nerve of the category of cobordisms under composition in one of these directions. Taken together this is an -fold simplicial set
which is like the nerve of an -fold category of cobordisms.
When suitable regularity conditions are imposed on this data, there is naturally a topology on each of these sets of embedded marked cobordisms, that makes this into an -fold simplicial topological space
To get rid of the dependence of this construction on , we can let “grow arbitrarily large” by taking the colimit of the above -fold cosimplicial spaces as ranges over the finite dimensional subspaces of .
The resulting -fold simplicial topological space obtained by this colimit then is essentially the (∞,n)-category that we are after. It turns out that it actually is an -fold Segal soace. We just formally complete it to an n-fold complete Segal space
This, then, is a model for the (∞,n)-category of extended -dimensional cobordisms.
For we have that is the symmetric monoidal ∞-groupoid ( infinite loop space) that underlies the Thom spectrum.
Its homotopy groups are the cobordism rings
Therefore a symmetric monoidal -functor
to some symmetric monoidal -groupoid is a genus.
A specific realization of this idea in terms of (∞,n)-category modeled as n-fold complete Segal space is in (definition 2.2.9, page 36)
In that article a proof of the cobordism hypothesis is indicated.
A detailed construction of the (2,2)-category of cobordisms is
For a discussion of the relation of to the Thom spectrum and the cobordism ring see also
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Other discussions of higher categories of cobordisms are
Eugenia Cheng and Nick Gurski, Toward an -category of cobordisms , Theory and Applications of Categories 18 (2007), 274-302. (tac)