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{{Short description|Integer invariant of certain classes of topological manifolds}}
{{Unreferenced|date=December 2009}}
In the ] field of ], the '''signature''' is an integer ] which is defined for an oriented ] ''M'' of dimension ''d''=4''k'' ] (]-dimensional). In the field of ], the '''signature''' is an integer ] which is defined for an oriented ] ''M'' of dimension ].


This invariant of a manifold has been studied in detail, starting with ] for 4-manifolds. This invariant of a manifold has been studied in detail, starting with ] for 4-manifolds, and ].


== Definition == == Definition ==
Given a ] and ] manifold ''M'' of dimension 4''k'', the ] gives rise to a ] ''Q'' on the 'middle' real ] Given a ] and ] manifold ''M'' of dimension 4''k'', the ] gives rise to a ] ''Q'' on the 'middle' real ]


:<math>H^{2k}(M,\mathbf{R})</math>.
:''H''<sup>2''k''</sup>(''M'',''Z'').


The basic identity for the cup product The basic identity for the cup product
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:<math>\alpha^p \smile \beta^q = (-1)^{pq}(\beta^q \smile \alpha^p)</math> :<math>\alpha^p \smile \beta^q = (-1)^{pq}(\beta^q \smile \alpha^p)</math>


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


:<math>H^{4k}(M,\mathbf{R})</math>.
:''H''<sup>4''k''</sup>(''M'',''Z'').


If we assume also that ''M'' is ], ] identifies this with If we assume also that ''M'' is ], ] identifies this with


:<math>H^{0}(M,\mathbf{R})</math>
:''H''<sub>0</sub>(''M'',''Z''),


which 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 can be identified with <math>\mathbf{R}</math>. Therefore the cup product, under these hypotheses, does give rise to a ] on ''H''<sup>2''k''</sup>(''M'',''R''); and therefore to a quadratic form ''Q''. The form ''Q'' is ] due to Poincaré duality, as it pairs non-degenerately with itself.<ref>{{cite book|last1=Hatcher|first1=Allen|title=Algebraic topology|date=2003|publisher=Cambridge Univ. Pr.|location=Cambridge|isbn=978-0521795401|page=250|edition=Repr.|url=https://pi.math.cornell.edu/~hatcher/AT/AT.pdf|accessdate=8 January 2017|language=en}}</ref> 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'', 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. The '''signature''' <math>\sigma(M)</math> of ''M'' is by definition the ] of ''Q'', that is, <math>\sigma(M) = n_+ - n_-</math> where any diagonal matrix defining ''Q'' has <math>n_+</math> positive entries and <math>n_-</math> negative entries.<ref>{{cite book|last1=Milnor|first1=John|last2=Stasheff|first2=James|title=Characteristic classes|date=1962|publisher=Annals of Mathematics Studies 246|page=224|isbn=978-0691081229|language=en|citeseerx=10.1.1.448.869}}</ref> If ''M'' is not connected, its signature is defined to be the sum of the signatures of its connected components.


== 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-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. 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 ] numbers. ] (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 ].
*Compact oriented manifolds ''M'' and ''N'' satisfy <math>\sigma(M \sqcup N) = \sigma(M) + \sigma(N)</math> by definition, and satisfy <math>\sigma(M\times N) = \sigma(M)\sigma(N)</math> by a ].

*If ''M'' is an oriented boundary, then <math>\sigma(M)=0</math>.

*] (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==
*] *]
*] *]
*]

==References==
{{Reflist}}


{{DEFAULTSORT:Signature (Topology)}} {{DEFAULTSORT:Signature (Topology)}}

Latest revision as of 15:02, 6 January 2025

Integer invariant of certain classes of topological manifolds

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

H 2 k ( M , R ) {\displaystyle H^{2k}(M,\mathbf {R} )} .

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 4 k ( M , R ) {\displaystyle H^{4k}(M,\mathbf {R} )} .

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

H 0 ( M , R ) {\displaystyle H^{0}(M,\mathbf {R} )}

which can be identified with R {\displaystyle \mathbf {R} } . 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 σ ( M ) {\displaystyle \sigma (M)} of M is by definition the signature of Q, that is, σ ( M ) = n + n {\displaystyle \sigma (M)=n_{+}-n_{-}} where any diagonal matrix defining Q has n + {\displaystyle n_{+}} positive entries and n {\displaystyle n_{-}} negative entries. 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

  • Compact oriented manifolds M and N satisfy σ ( M N ) = σ ( M ) + σ ( N ) {\displaystyle \sigma (M\sqcup N)=\sigma (M)+\sigma (N)} by definition, and satisfy σ ( M × N ) = σ ( M ) σ ( N ) {\displaystyle \sigma (M\times N)=\sigma (M)\sigma (N)} by a Künneth formula.
  • If M is an oriented boundary, then σ ( M ) = 0 {\displaystyle \sigma (M)=0} .
  • 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 p 1 3 {\displaystyle {\frac {p_{1}}{3}}} . Friedrich Hirzebruch (1954) found an explicit expression for this linear combination as the L genus of the manifold.

See also

References

  1. Hatcher, Allen (2003). Algebraic topology (PDF) (Repr. ed.). Cambridge: Cambridge Univ. Pr. p. 250. ISBN 978-0521795401. Retrieved 8 January 2017.
  2. Milnor, John; Stasheff, James (1962). Characteristic classes. Annals of Mathematics Studies 246. p. 224. CiteSeerX 10.1.1.448.869. ISBN 978-0691081229.
  3. Thom, René. "Quelques proprietes globales des varietes differentiables" (PDF) (in French). Comm. Math. Helvetici 28 (1954), S. 17–86. Retrieved 26 October 2019.
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