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== Other dimensions == | == Other dimensions == | ||
{{details|L-theory}} | {{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 |
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 === | ||
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== Properties == | == Properties == | ||
] (1954) showed that the signature of a manifold is a cobordism invariant, and in particular is given by some linear combination of its ] ].<ref>{{cite news|last1=Thom|first1=René|title=Quelques proprietes globales des varietes differentiables|publisher=Comm. Math. Helvetici 28 (1954), S. 17–86|url=https://www.maths.ed.ac.uk/~v1ranick/papers/thomcob.pdf|accessdate=26 October 2019|language=fr}}</ref> For example, in four dimensions, it is given by <math>\frac{p_1}{3}</math>. ] (1954) found an explicit expression for this linear combination as the ] of the manifold. ] (1962) proved that a simply |
] (1954) showed that the signature of a manifold is a cobordism invariant, and in particular is given by some linear combination of its ] ].<ref>{{cite news|last1=Thom|first1=René|title=Quelques proprietes globales des varietes differentiables|publisher=Comm. Math. Helvetici 28 (1954), S. 17–86|url=https://www.maths.ed.ac.uk/~v1ranick/papers/thomcob.pdf|accessdate=26 October 2019|language=fr}}</ref> For example, in four dimensions, it is given by <math>\frac{p_1}{3}</math>. ] (1954) found an explicit expression for this linear combination as the ] of the manifold. ] (1962) proved that a simply connected compact ] with 4''n''-dimensional ] is homotopy equivalent to a manifold if and only if its signature satisfies the expression of the ]. ] says that the signature of a 4-dimensional simply connected manifold with a ] is divisible by 16. | ||
==See also== | ==See also== |
Revision as of 16:43, 11 September 2022
In the field of topology, the signature is an integer invariant which is defined for an oriented manifold M of dimension divisible by four.
This invariant of a manifold has been studied in detail, starting with Rokhlin's theorem for 4-manifolds, and Hirzebruch signature theorem.
Definition
Given a connected and oriented manifold M of dimension 4k, the cup product gives rise to a quadratic form Q on the 'middle' real cohomology group
- .
The basic identity for the cup product
shows that with p = q = 2k the product is symmetric. It takes values in
- .
If we assume also that M is compact, Poincaré duality identifies this with
which can be identified with . Therefore the cup product, under these hypotheses, does give rise to a symmetric bilinear form on H(M,R); 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, an ordered triple according to its definition. 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-theoryIf 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 or as the 4k-dimensional quadratic L-group and these invariants do not always vanish for other dimensions. The Kervaire invariant is a mod 2 (i.e., an element of ) for framed manifolds of dimension 4k+2 (the quadratic L-group ), while the de Rham invariant is a mod 2 invariant of manifolds of dimension 4k+1 (the symmetric L-group ); the other dimensional L-groups vanish.
Kervaire invariant
Main article: Kervaire invariantWhen 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. For example, in four dimensions, it is given by . 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. Rokhlin's theorem says that the signature of a 4-dimensional simply connected manifold with a spin structure is divisible by 16.
See also
References
- Milnor, John; Stasheff, James (1962). Characteristic classes. Annals of Mathematics Studies 246. p. 224. CiteSeerX 10.1.1.448.869. ISBN 978-0691081229.
- Hatcher, Allen (2003). Algebraic topology (PDF) (Repr. ed.). Cambridge: Cambridge Univ. Pr. p. 250. ISBN 978-0521795401. Retrieved 8 January 2017.
- Thom, René. "Quelques proprietes globales des varietes differentiables" (PDF) (in French). Comm. Math. Helvetici 28 (1954), S. 17–86. Retrieved 26 October 2019.