Signature (topology)




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.




Contents






  • 1 Definition


  • 2 Other dimensions


    • 2.1 Kervaire invariant




  • 3 Properties


  • 4 See also


  • 5 References





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



H2k(M,R){displaystyle H^{2k}(M,mathbf {R} )}{displaystyle H^{2k}(M,mathbf {R} )}.

The basic identity for the cup product


αp⌣βq=(−1)pq(βq⌣αp){displaystyle alpha ^{p}smile beta ^{q}=(-1)^{pq}(beta ^{q}smile alpha ^{p})}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



H4k(M,R){displaystyle H^{4k}(M,mathbf {R} )}{displaystyle H^{4k}(M,mathbf {R} )}.

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


H0(M,R){displaystyle H^{0}(M,mathbf {R} )}{displaystyle H^{0}(M,mathbf {R} )}

which can be identified with R{displaystyle mathbf {R} }mathbf {R} . Therefore cup product, under these hypotheses, does give rise to a symmetric bilinear form on H2k(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.[1] 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



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 L4k,{displaystyle L^{4k},}{displaystyle L^{4k},} or as the 4k-dimensional quadratic L-group L4k,{displaystyle L_{4k},}{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}mathbf{Z}/2) for framed manifolds of dimension 4k+2 (the quadratic L-group L4k+2{displaystyle L_{4k+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 L4k+1{displaystyle L^{4k+1}}{displaystyle L^{4k+1}}); the other dimensional L-groups vanish.



Kervaire invariant



When d=4k+2=2(2k+1){displaystyle d=4k+2=2(2k+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. For example, in four dimensions, it is given by p13{displaystyle {frac {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. 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



  • Hirzebruch signature theorem

  • Genus of a multiplicative sequence



References





  1. ^ Hatcher, Allen (2003). Algebraic topology (PDF) (Repr. ed.). Cambridge: Cambridge Univ. Pr. p. 250. ISBN 978-0521795401. Retrieved 8 January 2017..mw-parser-output cite.citation{font-style:inherit}.mw-parser-output q{quotes:"""""""'""'"}.mw-parser-output code.cs1-code{color:inherit;background:inherit;border:inherit;padding:inherit}.mw-parser-output .cs1-lock-free a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/6/65/Lock-green.svg/9px-Lock-green.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-lock-limited a,.mw-parser-output .cs1-lock-registration a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/d/d6/Lock-gray-alt-2.svg/9px-Lock-gray-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-lock-subscription a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/a/aa/Lock-red-alt-2.svg/9px-Lock-red-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration{color:#555}.mw-parser-output .cs1-subscription span,.mw-parser-output .cs1-registration span{border-bottom:1px dotted;cursor:help}.mw-parser-output .cs1-hidden-error{display:none;font-size:100%}.mw-parser-output .cs1-visible-error{font-size:100%}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration,.mw-parser-output .cs1-format{font-size:95%}.mw-parser-output .cs1-kern-left,.mw-parser-output .cs1-kern-wl-left{padding-left:0.2em}.mw-parser-output .cs1-kern-right,.mw-parser-output .cs1-kern-wl-right{padding-right:0.2em}









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