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In
mathematics Mathematics is an area of knowledge that includes the topics of numbers, formulas and related structures, shapes and the spaces in which they are contained, and quantities and their changes. These topics are represented in modern mathematics ...
, equivariant cohomology (or ''Borel cohomology'') is a cohomology theory from
algebraic topology Algebraic topology is a branch of mathematics that uses tools from abstract algebra to study topological spaces. The basic goal is to find algebraic invariant (mathematics), invariants that classification theorem, classify topological spaces up t ...
which applies to
topological space In mathematics, a topological space is, roughly speaking, a geometrical space in which closeness is defined but cannot necessarily be measured by a numeric distance. More specifically, a topological space is a set whose elements are called points ...
s with a ''
group action In mathematics, a group action on a space is a group homomorphism of a given group into the group of transformations of the space. Similarly, a group action on a mathematical structure is a group homomorphism of a group into the automorphism ...
''. It can be viewed as a common generalization of
group cohomology In mathematics (more specifically, in homological algebra), group cohomology is a set of mathematical tools used to study groups using cohomology theory, a technique from algebraic topology. Analogous to group representations, group cohomology loo ...
and an ordinary
cohomology theory In mathematics, specifically in homology theory and algebraic topology, cohomology is a general term for a sequence of abelian groups, usually one associated with a topological space, often defined from a cochain complex. Cohomology can be viewed ...
. Specifically, the equivariant cohomology ring of a space X with action of a topological group G is defined as the ordinary
cohomology ring In mathematics, specifically algebraic topology, the cohomology ring of a topological space ''X'' is a ring formed from the cohomology groups of ''X'' together with the cup product serving as the ring multiplication. Here 'cohomology' is usually und ...
with coefficient ring \Lambda of the
homotopy quotient In mathematics, the universal bundle in the theory of fiber bundles with structure group a given topological group , is a specific bundle over a classifying space , such that every bundle with the given structure group over is a pullback by mea ...
EG \times_G X: :H_G^*(X; \Lambda) = H^*(EG \times_G X; \Lambda). If G is the
trivial group In mathematics, a trivial group or zero group is a group consisting of a single element. All such groups are isomorphic, so one often speaks of the trivial group. The single element of the trivial group is the identity element and so it is usually ...
, this is the ordinary
cohomology ring In mathematics, specifically algebraic topology, the cohomology ring of a topological space ''X'' is a ring formed from the cohomology groups of ''X'' together with the cup product serving as the ring multiplication. Here 'cohomology' is usually und ...
of X, whereas if X is
contractible In mathematics, a topological space ''X'' is contractible if the identity map on ''X'' is null-homotopic, i.e. if it is homotopic to some constant map. Intuitively, a contractible space is one that can be continuously shrunk to a point within that ...
, it reduces to the cohomology ring of the
classifying space In mathematics, specifically in homotopy theory, a classifying space ''BG'' of a topological group ''G'' is the quotient of a weakly contractible space ''EG'' (i.e. a topological space all of whose homotopy groups are trivial) by a proper free acti ...
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).


Definitions

It is also possible to define the equivariant cohomology H_G^*(X;A) of X with coefficients in a G-module ''A''; these are
abelian group In mathematics, an abelian group, also called a commutative group, is a group in which the result of applying the group operation to two group elements does not depend on the order in which they are written. That is, the group operation is commut ...
s. This construction is the analogue of cohomology with local coefficients. 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 the so-called Cartan model (see
equivariant differential form In differential geometry, an equivariant differential form on a manifold ''M'' acted upon by a Lie group ''G'' is a polynomial map :\alpha: \mathfrak \to \Omega^*(M) from the Lie algebra \mathfrak = \operatorname(G) to the space of differential fo ...
s.) The construction should not be confused with other cohomology theories, such as Bredon cohomology or the 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.
Koszul duality In mathematics, Koszul duality, named after the French mathematician Jean-Louis Koszul, is any of various kinds of dualities found in representation theory of Lie algebras, abstract algebras (semisimple algebra) and topology (e.g., equivariant cohom ...
is known to hold between equivariant cohomology and ordinary cohomology.


Relation with groupoid cohomology

For a
Lie groupoid In mathematics, a Lie groupoid is a groupoid where the set \operatorname of objects and the set \operatorname of morphisms are both manifolds, all the category operations (source and target, composition, identity-assigning map and inversion) are smo ...
\mathfrak = _1 \rightrightarrows X_0/math> equivariant cohomology of a smooth manifold is a special example of the groupoid cohomology of a Lie groupoid. This is because given a G-space X for a compact Lie group G, there is an associated groupoid
\mathfrak_G = \times X \rightrightarrows X
whose equivariant cohomology groups can be computed using the Cartan complex \Omega_G^\bullet(X) which is the totalization of the de-Rham double complex of the groupoid. The terms in the Cartan complex are
\Omega^n_G(X) = \bigoplus_(\text^k(\mathfrak^\vee)\otimes \Omega^i(X))^G
where \text^\bullet(\mathfrak^\vee) is the symmetric algebra of the dual Lie algebra from the Lie group G, and (-)^G corresponds to the G-invariant forms. This is a particularly useful tool for computing the cohomology of BG for a compact Lie group G since this can be computed as the cohomology of
\rightrightarrows */math>
where the action is trivial on a point. Then,
H^*_(BG) = \bigoplus_\text^(\mathfrak^\vee)^G
For example,
\begin H^*_(BU(1)) &= \bigoplus_\text^(\mathbb^\vee) \\ &\cong \mathbb \\ &\text \deg(t) = 2 \end
since the U(1)-action on the dual Lie algebra is trivial.


Homotopy quotient

The homotopy quotient, also called homotopy orbit space or Borel construction, is a “homotopically correct” version of the
orbit space In celestial mechanics, an orbit is the curved trajectory of an object such as the trajectory of a planet around a star, or of a natural satellite around a planet, or of an artificial satellite around an object or position in space such as a p ...
(the quotient of X by its G-action) in which X is first replaced by a larger but
homotopy equivalent In topology, a branch of mathematics, two continuous functions from one topological space to another are called homotopic (from grc, ὁμός "same, similar" and "place") if one can be "continuously deformed" into the other, such a deforma ...
space so that the action is guaranteed to be free. To this end, construct the
universal bundle In mathematics, the universal bundle in the theory of fiber bundles with structure group a given topological group , is a specific bundle over a classifying space In mathematics, specifically in homotopy theory, a classifying space ''BG'' of a topo ...
''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 ''EG''. 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.


An example of a homotopy quotient

The following example is Proposition 1 o

Let ''X'' be a complex projective
algebraic curve In mathematics, an affine algebraic plane curve is the zero set of a polynomial in two variables. A projective algebraic plane curve is the zero set in a projective plane of a homogeneous polynomial in three variables. An affine algebraic plane c ...
. We identify ''X'' as a topological space with the set of the complex points X(\mathbb), which is a compact
Riemann surface In mathematics, particularly in complex analysis, a Riemann surface is a connected one-dimensional complex manifold. These surfaces were first studied by and are named after Bernhard Riemann. Riemann surfaces can be thought of as deformed vers ...
. Let ''G'' be a complex simply connected semisimple Lie group. Then any principal ''G''-bundle on ''X'' is isomorphic to a trivial bundle, since the
classifying space In mathematics, specifically in homotopy theory, a classifying space ''BG'' of a topological group ''G'' is the quotient of a weakly contractible space ''EG'' (i.e. a topological space all of whose homotopy groups are trivial) by a proper free acti ...
BG is 2-connected and ''X'' has real dimension 2. Fix some smooth ''G''-bundle P_\text on ''X''. Then any principal ''G''-bundle on X is isomorphic to P_\text. In other words, the set \Omega of all isomorphism classes of pairs consisting of a principal ''G''-bundle on ''X'' and a complex-analytic structure on it can be identified with the set of complex-analytic structures on P_\text or equivalently the set of holomorphic connections on ''X'' (since connections are integrable for dimension reason). \Omega is an infinite-dimensional complex affine space and is therefore contractible. Let \mathcal be the group of all automorphisms of P_\text (i.e.,
gauge group In physics, a gauge theory is a type of field theory in which the Lagrangian (and hence the dynamics of the system itself) does not change (is invariant) under local transformations according to certain smooth families of operations ( Lie group ...
.) Then the homotopy quotient of \Omega by \mathcal classifies complex-analytic (or equivalently algebraic) principal ''G''-bundles on ''X''; i.e., it is precisely the classifying space B\mathcal of the discrete group \mathcal. One can define the
moduli stack of principal bundles In algebraic geometry, given a smooth projective curve ''X'' over a finite field \mathbf_q and a smooth affine group scheme ''G'' over it, the moduli stack of principal bundles over ''X'', denoted by \operatorname_G(X), is an algebraic stack given b ...
\operatorname_G(X) as the
quotient stack In algebraic geometry, a quotient stack is a stack that parametrizes equivariant objects. Geometrically, it generalizes a quotient of a scheme or a variety by a group: a quotient variety, say, would be a coarse approximation of a quotient stack. T ...
Omega/\mathcal/math> and then the homotopy quotient B\mathcal is, by definition, the
homotopy type In topology, a branch of mathematics, two continuous functions from one topological space to another are called homotopic (from grc, ὁμός "same, similar" and "place") if one can be "continuously deformed" into the other, such a deforma ...
of \operatorname_G(X).


Equivariant characteristic classes

Let ''E'' be an
equivariant vector bundle In mathematics, given an action \sigma: G \times_S X \to X of a group scheme ''G'' on a scheme ''X'' over a base scheme ''S'', an equivariant sheaf ''F'' on ''X'' is a sheaf of \mathcal_X-modules together with the isomorphism of \mathcal_-modules ...
on a ''G''-manifold ''M''. It gives rise to a vector bundle \widetilde on the homotopy quotient EG \times_G M so that it pulls-back to the bundle \widetilde=EG \times E over EG \times M. An equivariant characteristic class of ''E'' is then an ordinary characteristic class of \widetilde, which is an element of the completion of the cohomology ring H^*(EG \times_G M) = H^*_G(M). (In order to apply Chern–Weil theory, one uses a finite-dimensional approximation of ''EG''.) Alternatively, one can first define an equivariant Chern class and then define other characteristic classes as invariant polynomials of Chern classes as in the ordinary case; for example, the equivariant Todd class of an equivariant line bundle is the
Todd function Todd or Todds may refer to: Places ;Australia: * Todd River, an ephemeral river ;United States: * Todd Valley, California, also known as Todd, an unincorporated community * Todd, Missouri, a ghost town * Todd, North Carolina, an unincorporated ...
evaluated at the equivariant first Chern class of the bundle. (An equivariant Todd class of a line bundle is a power series (not a polynomial as in the non-equivariant case) in the equivariant first Chern class; hence, it belongs to the completion of the equivariant cohomology ring.) In the non-equivariant case, the first Chern class can be viewed as a bijection between the set of all isomorphism classes of complex line bundles on a manifold ''M'' and H^2(M; \mathbb).using
Čech cohomology In mathematics, specifically algebraic topology, Čech cohomology is a cohomology theory based on the intersection properties of open covers of a topological space. It is named for the mathematician Eduard Čech. Motivation Let ''X'' be a topolo ...
and the isomorphism H^1(M; \mathbb^*) \simeq H^2(M; \mathbb) given by the exponential map.
In the equivariant case, this translates to: the equivariant first Chern gives a bijection between the set of all isomorphism classes of equivariant complex line bundles and H^2_G(M; \mathbb).


Localization theorem

The localization theorem is one of the most powerful tools in equivariant cohomology.


See also

*
Equivariant differential form In differential geometry, an equivariant differential form on a manifold ''M'' acted upon by a Lie group ''G'' is a polynomial map :\alpha: \mathfrak \to \Omega^*(M) from the Lie algebra \mathfrak = \operatorname(G) to the space of differential fo ...
* Kirwan map *
Localization formula for equivariant cohomology In differential geometry, the localization formula states: for an equivariantly closed equivariant differential form \alpha on an orbifold ''M'' with a torus action and for a sufficient small \xi in the Lie algebra of the torus ''T'', : \int_M \al ...
* GKM variety * Bredon cohomology


Notes


References

* * * * *


Relation to stacks

* PDF page 10 has the main result with examples.


Further reading

* *


External links

* — Excellent survey article describing the basics of the theory and the main important theorems * *{{cite web , author=Young-Hoon Kiem , url=http://www.math.snu.ac.kr/~kiem/mylecture-equivcoh.pdf , title=Introduction to equivariant cohomology theory , date=2008 , publisher=Seoul National University
What is the equivariant cohomology of a group acting on itself by conjugation?
Algebraic topology Homotopy theory Symplectic topology Group actions (mathematics)