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{{Short description|Integer invariant of certain classes of topological manifolds}}
In ], the '''signature''' of an oriented ] ''M'' is defined when ''M'' has dimension ''d'' ]. In that case, when ''M'' is ] and ], ] gives rise to a ] ''Q'' on the 'middle' real ]
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, and ].
:''H''<sup>2''n''</sup>(''M'',''R''),


== Definition ==
where
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>.
:''d'' = 4''n''.


The basic identity for the cup product The basic identity for the cup product
Line 11: Line 13:
:<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''n'' 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''n''</sup>(''M'',''R'').


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'',''R''),


which is a one-dimensional real vector space and can be identified with ''R''. Therefore cup product, under these hypotheses, does give rise to a ] on ''H''<sup>2''n''</sup>(''M'',''R''); and therefore to a quadratic form ''Q''. More generally, the signature can 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.
be defined in this way for any general compact ] with ''4n''-dimensional ].


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.
The ] 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. If ''M'' has dimension not divisible by 4, its signature is usually defined to be 0. The form ''Q'' is ]. This invariant of a manifold has been studied in detail, starting with ] for 4-manifolds.


== Other dimensions ==
When ''d'' is ], the same construction gives rise to an ]. Such forms do not have a signature invariant; if they are non-degenerate, any two such forms are equivalent.
{{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 ===
] (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 ''4n''-dimensional ] is homotopy equivalent to a manifold if and only if its signature satisfies the expression of the ]
{{main|Kervaire invariant}}
When <math>d=4k+2=2(2k+1)</math> is twice an odd integer (]), the same construction gives rise to an ]. Such forms do not have a signature invariant; if they are non-degenerate, any two such forms are equivalent. However, if one takes a ] of the form, which occurs if one has a ], then the resulting ]s need not be equivalent, being distinguished by the ]. The resulting invariant of a manifold is called the ].


==See also== == Properties ==


*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==
*] *]
*] *]
*]

==References==
{{Reflist}}


{{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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