differential cohomology
As described at cohomology, a notion of cohomology exists for every (infinity,1)-topos : for and two objects of ,
an -valued cocycle on is an object in the ∞-groupoid ;
a coboundary between two such cocycles is a morphism in
the cohomology classes are the equivalence classes of , so that the cohomology set of -valued cohomology on is
where is the homotopy category of the (∞,1)-category .
Now, ordinary groupoid nonabelian cohomology is the cohomology obtained for ∞Grpd Top: cohomology on ∞-groupoids (or topological spaces) with coefficients in -groupoids.
The various notions of group cohomology are special cases of this:
Group cohomology with coefficients in a trivial module is the cohomology in ∞Grpd for the case that
the domain is a one-object groupoid being the deloopinga group ;
the coefficient object is , the strict ω-groupoid coming from the crossed complex that is concentrated in degree , where it is the abelian group (see Eilenberg-MacLane object for more details).
For One writes
for the degree- group cohomology of with values in .
Nonabelian group cohomology is obtained from this by allowing the coefficient object to be of the form
For instance for the automorphism 2-group of a possibly nonabelian group , nonabelian group cohomology classified -extensions of (see also gerbe (general idea)).
Details on this case are at nonabelian group cohomology
Group cohomology with coefficients in a nontrivial module is in turn twisted cohomology version of nonabelian group cohomology:
let be a strict ω-groupoid coming from a crossed complex of the form
with the abelian group in degree and for
the action of on required by the structure of a crossed complex;
The th group cohomology of with coefficients in the module is the connected components of the -groupoid of sections
This is an example of twisted cohomology, as explained there.
We spell out in detail how the above reproduces the ordinary definition of group cohomology.
For the case of ordinary abelian group cohomology, the context of strict omega-groupoids is in principle fully sufficient, since the domain object in that case is a 1-groupoid, clearly a strict infinity-groupoid, as are the abelian coefficient -groupoids , manifestly so as images of crossed complexes under the equivalence of crossed complexes with strict omega-groupoids.
So one possibility is to model in this case as the homotopy category induced by the model structure on strict omega-groupoids.
This is, more or less implicitly, the route taken in chapter 12 of
Since every -groupoid is fibrant, this model category category of strict -groupoids is in fact a category of fibrant objects and hence the hom-sets in its homotopy category may be computed as colimits over -anafunctors, namely
where the colimit is over all strict -groupoids with an acyclic fibration, which here is a k-surjective functor for all .
On the other hand, since also the full model structure is around, this colimit localizes on the cofibrant replacement of . But this is nothing but the free strict -groupoid on the nerve of , which is the usual bar resolution of (see the discusson at nerve):
This is of course nothing but the incarnation of as an object in the category of weak infinity-groupoids modeled as Kan complexes.
For instance the 2-cells in are of the form
where the diagram indicates what the face maps on are.
Accordingly, the 3-cells look like
The free strict -groupoid on has as -morphisms the free -groupoids generated from one -oriental per such -simplex in .
In chapter 12 of Brown-Higgins-Sivera group cocycles are computed as morphisms out of this cofibrant replacement of the ordinary 1-groupoid in the category of strict omega-groupoids. (Or rather, there the equivalent crossed complexes) are used.
Alternatively, we can pass along the inclusion
of strict -groupoids into all -groupoids modeled as Kan complexes and compute the homotopy classes of morphisms there. Every Kan complex is already cofibrant (while of course still also being fibrant), so once the situation is interpreted in SSet we can compute group cohomology in terms of ordinary morphisms without having to resolve further, without having to resort to anafunctors etc. Of course it is the nerve operation involved both in forming the cofibrant replacement in as well as in passing to that accomplishes the required resolutions in either case.
The upshot of all this is just that the following illustrative pictures may be interpreted either in or in :
A degree-one group cocycle , is just a functor . This is a group homomorphism .
A degree-2 group cocycle , is on 2-cells a map
i.e. a map such that it extends to a morphism on 3-cells:
Since there are no non-identity 3-morphisms in (non-degenerate 3-cells in ) the 3-cell on the right is required to be the identity. Since the composition of the 2-cells on the right is their addition (group multiplication in the abelian group ) this says that the assignment has to be such that
This expresses the commutativity of the above tetrahedra. And it is indeed the ordinary formula for a cocycle in degree-2 group cohomology.
similarly…
If the groups in question are not plain groups (group objects internal to Set) but groups with extra structure, such as topological groups or Lie groups, then their cohomology has to be understood in the corresponding natural context.
In parts of the literature cohomology of structured groups is defined in direct generalization of the formulas above as homotopy classes of morphisms from the simplicial object
to a simplicial object .
This is what is described above. But this does not in general give the right answer for structured groups:
namely cohomology is really about homotopy classes of maps in the suitable ambient (∞,1)-topos. For plain groups as in the above entry, we are working in the -topos ∞Grpd. That may be modeled by the standard model structure on simplicial sets. In that model structure, all objects a cofibrant and Kan complexes are fibrant. That means all objects we are dealing with here are both cofibrant and fibrant, and hence the simplicial set of maps between them is the cofrrect derived hom-space between these objects.
But this changes as we consider groups with extra structure. For a Lie group , the object
has to be considered as an Lie ∞-groupoid: an object in the model structure on simplicial presheaves over a site such as Diff or CartSp. As such it is in general not both cofibrant and fibrant. To that extent plain morphisms out of this object do not compute the correct derived hom-spaces. Instead, the right definition of structured group cohomology uses the correct fibrant and cofibrant replacements.
For a Lie group and an abelian Lie group, write
for the naive notion of cohomology on .
The correct definition of Lie group cohomology, denoted here or for emphasis was apparently introduced in
following
The Lie group cohomology used in Bry is the intrinsic cohomology of the object in the (∞,1)-topos of (∞,1)-sheaves on CartSp:
To derive the explicit formulas in the literature, model by the local projective model structure on simplicial presheaves on CartSp.
Fibrant objects are the Kan-complex valued objects that satisfy descent ob object of . By the special natur of the site CartSp, that descent condition is pretty trivial. For an abelian Lie group, satisfies descent on every : every -principal n-bundle on the contractible is equivalent to the trivial one.
So for a Lie group, it remains to find a cofibrant replacement for . With that in hand we have that the Lie group cohomology of is
To find that cofibrant replacement, recall from the discussion of cofibrant objects in the projective model structure over at model structure on simplicial presheaves that these are in particular given by good covers : simplicial objects that are degreewise coproducts of representables such that in each degree the degenerate part splits off as a direct summand.
To obtain this, write first
By the Bousfield-Kan map this is weakly equivalent to
with , as described there.
Then choose for each a good cover . Let be the Cech nerve of this cover. This is a simplicial presheaf weakly equivalent to . The representable are cofibrant as are the Cech nerves of their good covers, and the left Quillen bifunctor preserves weak equivalences between cofibrant objects (with the cofibrant fixed), so we have
Again by the Bousfield-Kan map this is
This is objectwise the realization of a bisimplicial set which, as described there, is the diagonal
Since this is now degreewise a coproduct of representables and still haas degeneracies being direct summands, this is cofibrant in .
So we find that the correct Lie group cohomology is given by
By the Eilenberg-Zilber theorem this is the cohomology of the total complex of abelian groups given by the double complex :
And this, finally, is indeed the definition of the smooth group cohomology of as given by Blanc, as for instance, in Bry 2000, page 4.
There is an evident morphism
obtained by pulling back a globally defined smooth cocycle to a cover.
For definiteness, by a Lie group we now mean (following Bry, page3) a paracompact Frechet manifold equipped with a group structure such that the product and the inverse maps are smooth, and there is an everywhere defined exponential map where is the Lie algebra of .
If the coefficient Lie group is a topological vector space, then the naive group cohomology coincides with the correct Lie group cohomology
If the coefficient Lie group is discrete, then Lie group cohomology coindices with the topological cohomology of the classifying space
This is Bry, prop. 1.3 and Bry, lemma 1.5.
Remark The second statement can also be seen using that is a locally contractible (∞,1)-topos, which implies by adjuncton that .
classifies central extensions of Lie groups
such that is a locally trivial smooth principal -fibration.
The image of consists of those central extensions for which is bundle is trivial.
This is Bry, prop. 1.6 and Bry, lemma 1.5.
A discussion of the relation between local Lie group cohomology and Lie algebra cohomology is in
In
-cocycles on a topological group with valzues in a topological abelian group are considered as continuous maps (p. 3 ).
A definition in terms of Ext-functors and comparison with the naive definition is in
A classical reference that considers the cohomology of Lie groups as topological spaces is
If the coefficient group is nonabelian, its higher deloopings to not exist. But n-groupoids approximating this non-existant delooping do exists. Cohomology of with coefficients in these is called nonabelian group cohomology or Schreier theory. See there for more details.
Aspects of this general point of view on group cohomology is described for instance in chaper 12 of
Much of what is called “nonabelian cohomology” in the existing literature concerns the case of nonabelian group cohomology with coefficients in the automorphism 2-group of some possibly nonabelian group .
This is the topic of Schreier theory.
A random example for this use of terminology would be
For a conceptual discussion of nonabelian group cohomology see