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Revision as of 06:03, 22 January 2010 editNbarth (talk | contribs)Autopatrolled, Extended confirmed users, Pending changes reviewers, Rollbackers35,158 edits sections, Kervaire invariant, standardize notation (integer rather than real, k rather than n)← Previous edit Revision as of 06:33, 22 January 2010 edit undoNbarth (talk | contribs)Autopatrolled, Extended confirmed users, Pending changes reviewers, Rollbackers35,158 edits Definition: other dimsNext edit →
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which is a one-dimensional real vector space and can be identified with ''Z''. Therefore cup product, under these hypotheses, does give rise to a ] on ''H''<sup>2''k''</sup>(''M'',''Z''); and therefore to a quadratic form ''Q''. The form ''Q'' is ] due to Poincaré duality, as it pairs non-degenerately with itself. More generally, the signature can be defined in this way for any general compact ] with ''4n''-dimensional Poincaré duality. which is a one-dimensional real vector space and can be identified with ''Z''. Therefore cup product, under these hypotheses, does give rise to a ] on ''H''<sup>2''k''</sup>(''M'',''Z''); and therefore to a quadratic form ''Q''. The form ''Q'' is ] due to Poincaré duality, as it pairs non-degenerately with itself. More generally, the signature can be defined in this way for any general compact ] with ''4n''-dimensional Poincaré duality.


The '''signature''' of ''M'' is by definition the ] of ''Q''. If ''M'' is not connected, its signature is defined to be the sum of the signatures of its connected components. If ''M'' has dimension not divisible by 4, its signature is usually defined to be 0; however, the ] provides an alternative mod 2 generalization (for framed manifolds). The '''signature''' of ''M'' is by definition the ] of ''Q''. If ''M'' is not connected, its signature is defined to be the sum of the signatures of its connected components.

== Other dimensions ==
{{details|L-theory}}
If ''M'' has dimension not divisible by 4, its signature is usually defined to be 0. There are alternative generalization in ]: the signature can be interpreted as the 4''k''-dimensional (simply-connected) symmetric L-group <math>L^{4k},</math> or as the 4''k''-dimensional quadratic L-group <math>L_{4k},</math> and these invariants do not always vanish for other dimensions. The ] is a mod 2 (i.e., an element of <math>\mathbf{Z}/2</math>) for framed manifolds of dimension 4''k''+2 (the quadratic L-group <math>L_{4k+2}</math>), while the ] is a mod 2 invariant of manifolds of dimension 4''k''+1 (the symmetric L-group <math>L^{4k+1}</math>); the other dimensional L-groups vanish.


== Kervaire invariant == == Kervaire invariant ==

Revision as of 06:33, 22 January 2010

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In the mathematical field of topology, the signature is an integer invariant which is defined for an oriented manifold M of dimension d=4k divisible by four (doubly even-dimensional).

This invariant of a manifold has been studied in detail, starting with Rokhlin's theorem for 4-manifolds.

Definition

Given a connected and orientable manifold M of dimension 4k, the cup product gives rise to a quadratic form Q on the 'middle' real cohomology group

H(M,Z).

The basic identity for the cup product

α p β q = ( 1 ) p q ( β q α p ) {\displaystyle \alpha ^{p}\smile \beta ^{q}=(-1)^{pq}(\beta ^{q}\smile \alpha ^{p})}

shows that with p = q = 2k the product is symmetric. It takes values in

H(M,Z).

If we assume also that M is compact, Poincaré duality identifies this with

H0(M,Z),

which is a one-dimensional real vector space and can be identified with Z. Therefore cup product, under these hypotheses, does give rise to a symmetric bilinear form on H(M,Z); and therefore to a quadratic form Q. The form Q is non-degenerate due to Poincaré duality, as it pairs non-degenerately with itself. More generally, the signature can be defined in this way for any general compact polyhedron with 4n-dimensional Poincaré duality.

The signature of M is by definition the signature of Q. If M is not connected, its signature is defined to be the sum of the signatures of its connected components.

Other dimensions

Further information: L-theory

If M has dimension not divisible by 4, its signature is usually defined to be 0. There are alternative generalization in L-theory: the signature can be interpreted as the 4k-dimensional (simply-connected) symmetric L-group L 4 k , {\displaystyle L^{4k},} or as the 4k-dimensional quadratic L-group L 4 k , {\displaystyle L_{4k},} and these invariants do not always vanish for other dimensions. The Kervaire invariant is a mod 2 (i.e., an element of Z / 2 {\displaystyle \mathbf {Z} /2} ) for framed manifolds of dimension 4k+2 (the quadratic L-group L 4 k + 2 {\displaystyle L_{4k+2}} ), while the de Rham invariant is a mod 2 invariant of manifolds of dimension 4k+1 (the symmetric L-group L 4 k + 1 {\displaystyle L^{4k+1}} ); the other dimensional L-groups vanish.

Kervaire invariant

Main article: Kervaire invariant

When d = 4 k + 2 = 2 ( 2 k + 1 ) {\displaystyle d=4k+2=2(2k+1)} is twice an odd integer (singly even), the same construction gives rise to an antisymmetric bilinear form. Such forms do not have a signature invariant; if they are non-degenerate, any two such forms are equivalent. However, if one takes a quadratic refinement of the form, which occurs if one has a framed manifold, then the resulting ε-quadratic forms need not be equivalent, being distinguished by the Arf invariant. The resulting invariant of a manifold is called the Kervaire invariant.

Properties

René Thom (1954) showed that the signature of a manifold is a cobordism invariant, and in particular is given by some linear combination of its Pontryagin numbers. Friedrich Hirzebruch (1954) found an explicit expression for this linear combination as the L genus of the manifold. William Browder (1962) proved that a simply-connected compact polyhedron with 4n-dimensional Poincaré duality is homotopy equivalent to a manifold if and only if its signature satisfies the expression of the Hirzebruch signature theorem

See also

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