Equivariant cohomology
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Borel Model
Suppose that a Lie group G acts on a manifold M. We would like to form a good notion of a quotient M / G. The problem is that if G has fixed points, the quotient space M / G will likely no longer be a manifold. However, if we could find a contractible space EG on which G acted freely, then
would have the same homotopy type as M, and the induced G action on the product would be free.
It is an interesting fact that such an EG always exists. For example,
acts freely via translations on the contractible space
, so
. In general, however, the EGs are infinite-dimensional spaces. For example, for
,
, and similarly for G = S1.
Thus
is usually an infinite-dimensional manifold. There is a natural projection map from MG onto BG = EG / G which realizes MG as a fiber bundle over BG with fiber M.
We define the equivariant cohomology
. Note first that if the action is free, then
, so the equivariant cohomology coincides with H * (M / G). On the other side of the spectrum, if the G-action is trivial, then
, and therefore
. For example, if G = S1,
, which is just
. Hence, the equivariant cohomology (with complex coefficients) is
. Thus, in some sense, the presence of large stabilizers of the group action get measured by the size of the equivariant cohomology group.
Localization Theorem
Let us now restrict ourselves to the case where G = S1. Now the natural projection map onto a point:
gives rise to a morphism
, and in this way makes
a
-module. Clearly if F is a fixed component of M, the
-module
is simply
.
The interesting fact is that if we make
into a
-module via localization, then this localized cohomology group is isomorphic to
, where the sum runs over the fixed components of M. This means that, modulo torsion, we can understand the equivariant cohomology completely from the fixed point data.
