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Equivariant cohomology : ウィキペディア英語版
Equivariant cohomology
In mathematics, equivariant cohomology is a cohomology theory from algebraic topology which applies to topological spaces with a ''group action''. It can be viewed as a common generalization of group cohomology and an ordinary cohomology theory. Specifically, the equivariant cohomology ring of a space ''X'' with action of a topological group ''G'' is defined as the ordinary cohomology ring with coefficient ring \Lambda of the homotopy quotient EG \times_G X:
:H_G^
*(X; \Lambda) = H^
*(EG \times_G X; \Lambda).
If G is the trivial group, this is the ordinary cohomology ring of X, whereas if X is contractible, it reduces to the cohomology ring of the classifying space BG (that is, the group cohomology of G when ''G'' is finite.) If ''G'' acts freely on ''X'', then the canonical map EG \times_G X \to X/G is a homotopy equivalence and so one gets: H_G^
*(X; \Lambda) = H^
*(X/G; \Lambda).
If ''X'' is a manifold, ''G'' a compact Lie group and \Lambda is the field of real numbers or the field of complex numbers (the most typical situation), then the above cohomology may be computed using so-called Cartan model (see equivariant differential forms.)
The construction should not be confused as a more naive cohomology of invariant differential forms: if ''G'' is a compact Lie group, then, by the averaging argument, any form may be made invariant; thus, cohomology of invariant differential forms does not yield new information.
The Koszul duality is known to hold between equivariant cohomology and ordinary cohomology.
== Homotopy quotient ==

The homotopy quotient, also called homotopy orbit space or Borel construction, is a “homotopically correct” version of the orbit space (the quotient of X by its G-action) in which X is first replaced by a larger but homotopy equivalent space so that the action is guaranteed to be free.
To this end, construct the universal bundle ''EG'' → ''BG'' for ''G'' and recall that ''EG'' admits a free ''G''-action. Then the product ''EG'' × ''X'' —which is homotopy equivalent to ''X'' since ''EG'' is contractible—admits a “diagonal” ''G''-action defined by (''e'',''x'').''g'' = (''eg'',''g−1x''): moreover, this diagonal action is free since it is free on ''G''. So we define the homotopy quotient ''X''''G'' to be the orbit space (''EG'' × ''X'')/''G'' of this free ''G''-action.
In other words, the homotopy quotient is the associated ''X''-bundle over ''BG'' obtained from the action of ''G'' on a space ''X'' and the principal bundle ''EG'' → ''BG''. This bundle ''X'' → ''X''''G'' → ''BG'' is called the Borel fibration.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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