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Kervaire invariant

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An invariant of an almost-parallelizable smooth manifold of dimension k + 2 , defined as the Arf-invariant of the quadratic form modulo 2 on the lattice of the ( 2 k + 1 ) -dimensional homology space of M .

Let M be a simply-connected almost-parallelizable closed smooth manifold of dimension 4 k + 2 whose homology groups H _ {i} ( M ; \mathbf Z ) vanish for 0 < i < 4 k + 2 , except for V = H _ {2k+ 1} ( M ; \mathbf Z ) .

On the free Abelian group V there is a skew-symmetric intersection form of cycles \Phi ( x , y ) , \Phi : V \times V \rightarrow \mathbf Z , and the dimension of the integral lattice in V is equal to 2 m . There exists on V a function \Phi _ {0} : V \rightarrow \mathbf Z _ {2} defined as follows: If x \in V , then there exists a smooth imbedding of the sphere S ^ {2k+ 1} into M that realizes the given element x , k \geq 1 . A tubular neighbourhood of this sphere S ^ {2k+ 1} in M is parallelizable, and it can be either trivial or isomorphic to a tubular neighbourhood of the diagonal in the product S ^ {2k+ 1} \times S ^ {2k+ 1} . Here, the tubular neighbourhood of the diagonal in S ^ {2k+ 1} \times S ^ {2k+ 1} is non-trivial if and only if 2 k + 1 \neq 1 , 3 , 7 (see Hopf invariant). The value of \Phi _ {0} is zero or one depending on whether or not the tubular neighbourhood of S ^ {2k+ 1} realizing x in M is trivial, 2 k + 1 \neq 1 , 3 , 7 . The function \Phi _ {0} : V \rightarrow \mathbf Z _ {2} satisfies the condition

\Phi _ {0} ( x + y ) \equiv \Phi _ {0} ( x) + \Phi _ {0} ( y) + \Phi ( x , y ) \mathop{\rm mod} 2 .

The Arf-invariant of \Phi _ {0} is also called the Kervaire invariant of the manifold M ^ {4k+ 2} , 2 k + 1 \neq 1 , 3 , 7 .

If the Kervaire invariant of M ^ {4k+ 2} is equal to zero, then there exists a symplectic basis ( e _ {i} , f _ {i} ) for V such that \Phi _ {0} ( e _ {i} ) = \Phi _ {0} ( f _ {i} ) = 0 . In this case M ^ {4k+ 2} is a connected sum of a product of spheres

M ^ {4k+ 2} = \ ( S ^ {2k+ 1} \times S ^ {2k+ 1} ) _ {1} \# \dots \# ( S ^ {2k+ 1} \times S ^ {2k+ 1} ) _ {m} .

If, on the other hand, the Kervaire invariant of M ^ {4k+ 2} is non-zero, then there is a symplectic basis ( e _ {i} , f _ {i} ) for V such that \Phi _ {0} ( e _ {i} ) = \Phi _ {0} ( f _ {i} ) = 0 for i \neq 1 and \Phi _ {0} ( e _ {1} ) = \Phi _ {0} ( f _ {1} ) = 1 . In this case the union of the tubular neighbourhoods of the two ( 2 k + 1 ) - dimensional spheres, imbedded in M ^ {4k+ 2} with transversal intersection at a point and realizing the elements e _ {1} , f _ {1} , gives a manifold K ^ {4k+ 2} . It is called the Kervaire manifold (see Dendritic manifold); its boundary \partial K ^ {4k+ 2} is diffeomorphic to the standard sphere, while the manifold M ^ {4k+ 2} itself can be expressed as the connected sum

M ^ {4k+ 2} = \ \widehat{K} {} ^ {4k+ 2} \# ( S ^ {2k+ 1} \times S ^ {2k+ 1} ) _ {1} \# \dots

{} \dots \# ( S ^ {2k+ 1} \times S ^ {2k+ 1} ) _ {m- 1} ,

where the smooth closed manifold \widehat{K} {} ^ {4k+ 2} is obtained from K ^ {4k+ 2} by attaching a cell.

If M ^ {4k+ 2} , k \neq 0 , 1 , 3 , is a smooth parallelizable ( 2 k ) -connected manifold with a boundary that is homotopic to a sphere, then the Kervaire invariant of M ^ {4k+ 2} is defined exactly as above and will have the same properties with the difference that, in the decomposition of M ^ {4k+ 2} into a connected sum of simple manifolds, the component K _ {0} ^ {4k+ 2} that is the Kervaire manifold has boundary \partial K ^ {4k+ 2} = \partial M ^ {4k+ 2} (which generally is not diffeomorphic to the standard sphere).

In the cases k = 0 , 1 , 3 the original manifolds M ^ {2} , M ^ {6} , M ^ {14} can be expressed as the connected sum ( S ^ {2k+ 1} \times S ^ {2k+ 1} ) \# \dots \# ( S ^ {2k+ 1} \times S ^ {2k+ 1} ) ( if the boundary is empty) or ( S ^ {2k+ 1} \times S ^ {2k+ 1} ) _ {0} \# \dots \# ( S ^ {2k+ 1} \times S ^ {2k+ 1} ) _ {m- 1} ( if the boundary is non-empty), where ( S ^ {2k+ 1} \times S ^ {2k+ 1} ) _ {0} is obtained by removing an open cell from S ^ {2k+ 1} \times S ^ {2k+ 1} .

However, a Kervaire invariant can be defined for the closed manifolds M ^ {2} , M ^ {6} , M ^ {14} (see Pontryagin invariant; Kervaire–Milnor invariant) and depends in these dimensions on the choice of the framing, that is, it is an invariant of the framed surgery of the pair ( M ^ {4k+ 2} , f _ {r} ) , k = 0 , 1 , 3 . In dimensions k \neq 0 , 1 , 3 the manifold M ^ {4k+ 2} can be modified to the sphere S ^ {4k+ 2} if and only if the pair ( M ^ {4k+ 2} , f _ {r} ) has a framed surgery to the pair ( S ^ {4k+ 2} , f _ {r} ) under any choice of f _ {r} on the original manifold M ^ {4k+ 2} (see Surgery on a manifold).

The Kervaire invariant is defined for any stably-parallelizable manifold M ^ {4k+ 2} as an invariant of framed surgery, and any element in the stable homotopy groups of spheres can be represented either as a framed homotopy sphere or as a closed smooth framed Kervaire manifold (in this case m = 4 k + 2 , k \neq 0 , 1 , 3 ), or as the framed manifold S ^ {2k+ 1} \times S ^ {2k+ 1} if k = 0 , 1 , 3 .

In other words, the Kervaire invariant can be regarded as an obstruction to "carrying over" the given framing on the manifold to the sphere of the same dimension, k \neq 0 , 1 , 3 . In this sense the Kervaire invariant fulfills the same role for the values k = 0 , 1 , 3 : The given framing on S ^ {2k+ 1} \times S ^ {2k+ 1} , k = 0 , 1 , 3 , cannot, in general, be "carried over" to the sphere S ^ {4k+ 2} , k = 0 , 1 , 3 , by means of framed surgery.

L.S. Pontryagin was the first to construct such a framing on the manifold S ^ {2k+ 1} \times S ^ {2k+ 1} for the case k = 0 , that is, a framing on the 2 - dimensional torus ( ( S ^ {1} \times S ^ {1} ) , f _ {r} ) that cannot be "carried over" to S ^ {2} . There are also such examples of a framing on the manifolds S ^ {3} \times S ^ {3} and S ^ {7} \times S ^ {7} .

The fundamental problem concerning the Kervaire invariant is the following: For which odd values of n does there exist a pair ( M ^ {2n} , f _ {r} ) with non-zero Kervaire invariant? For n \neq 2 ^ {i} - 1 the answer to this question is negative and for n = 2 ^ {i} - 1 it is affirmative, where i = 1 (Pontryagin, see [2]), i = 2 , 3 (M.A. Kervaire and J.W. Milnor, [5], [6]), i = 4 (W. Browder, [3]), i = 5 , 6 (M. Barratt, M. Mahowald, A. Milgram). For other values of i the answer is unknown (1989).

References

[1] S.P. Novikov, "Homotopy-equivalent smooth manifolds I" Izv. Akad. Nauk SSSR. Ser. Mat. , 28 : 2 (1964) pp. 365–474 (In Russian)
[2] L.S. Pontryagin, "Smooth manifolds and their applications in homology theory" , Moscow (1976) (In Russian)
[3] W. Browder, "The Kervaire invariant of framed manifolds and its generalization" Ann. of Math. , 90 (1969) pp. 157–186
[4] W.B. Browder, "Surgery on simply-connected manifolds" , Springer (1972)
[5] M. Kervaire, "A manifold which does not admit any differentiable structure" Comm. Math. Helv. , 34 (1960) pp. 257–270
[6] M.A. Kervaire, J.W. Milnor, "Groups of homotopy spheres I" Ann. Mat. , 77 : 3 (1963) pp. 504–537
How to Cite This Entry:
Kervaire invariant. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Kervaire_invariant&oldid=51841
This article was adapted from an original article by M.A. Shtan'ko (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article