Donaldson's theorem

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In mathematics, and especially differential topology and gauge theory, Donaldson's theorem states that a definite intersection form of a compact, oriented, smooth manifold of dimension 4 is diagonalisable. If the intersection form is positive (negative) definite, it can be diagonalized to the identity matrix (negative identity matrix) over the integers. The original version[1] of the theorem required the manifold to be simply connected, but it was later improved to apply to 4-manifolds with any fundamental group.[2]

History edit

The theorem was proved by Simon Donaldson. This was a contribution cited for his Fields medal in 1986.

Idea of proof edit

Donaldson's proof utilizes the moduli space   of solutions to the anti-self-duality equations on a principal  -bundle   over the four-manifold  . By the Atiyah–Singer index theorem, the dimension of the moduli space is given by

 

where  ,   is the first Betti number of   and   is the dimension of the positive-definite subspace of   with respect to the intersection form. When   is simply-connected with definite intersection form, possibly after changing orientation, one always has   and  . Thus taking any principal  -bundle with  , one obtains a moduli space   of dimension five.

 
Cobordism given by Yang–Mills moduli space in Donaldson's theorem

This moduli space is non-compact and generically smooth, with singularities occurring only at the points corresponding to reducible connections, of which there are exactly   many.[3] Results of Clifford Taubes and Karen Uhlenbeck show that whilst   is non-compact, its structure at infinity can be readily described.[4][5][6] Namely, there is an open subset of  , say  , such that for sufficiently small choices of parameter  , there is a diffeomorphism

 .

The work of Taubes and Uhlenbeck essentially concerns constructing sequences of ASD connections on the four-manifold   with curvature becoming infinitely concentrated at any given single point  . For each such point, in the limit one obtains a unique singular ASD connection, which becomes a well-defined smooth ASD connection at that point using Uhlenbeck's removable singularity theorem.[6][3]

Donaldson observed that the singular points in the interior of   corresponding to reducible connections could also be described: they looked like cones over the complex projective plane  . Furthermore, we can count the number of such singular points. Let   be the  -bundle over   associated to   by the standard representation of  . Then, reducible connections modulo gauge are in a 1-1 correspondence with splittings   where   is a complex line bundle over  .[3] Whenever   we may compute:

 ,

where   is the intersection form on the second cohomology of  . Since line bundles over   are classified by their first Chern class  , we get that reducible connections modulo gauge are in a 1-1 correspondence with pairs   such that  . Let the number of pairs be  . An elementary argument that applies to any negative definite quadratic form over the integers tells us that  , with equality if and only if   is diagonalizable.[3]

It is thus possible to compactify the moduli space as follows: First, cut off each cone at a reducible singularity and glue in a copy of  . Secondly, glue in a copy of   itself at infinity. The resulting space is a cobordism between   and a disjoint union of   copies of   (of unknown orientations). The signature   of a four-manifold is a cobordism invariant. Thus, because   is definite:

 ,

from which one concludes the intersection form of   is diagonalizable.

Extensions edit

Michael Freedman had previously shown that any unimodular symmetric bilinear form is realized as the intersection form of some closed, oriented four-manifold. Combining this result with the Serre classification theorem and Donaldson's theorem, several interesting results can be seen:

1) Any indefinite non-diagonalizable intersection form gives rise to a four-dimensional topological manifold with no differentiable structure (so cannot be smoothed).

2) Two smooth simply-connected 4-manifolds are homeomorphic, if and only if, their intersection forms have the same rank, signature, and parity.

See also edit

Notes edit

  1. ^ Donaldson, S. K. (1983-01-01). "An application of gauge theory to four-dimensional topology". Journal of Differential Geometry. 18 (2). doi:10.4310/jdg/1214437665. ISSN 0022-040X.
  2. ^ Donaldson, S. K. (1987-01-01). "The orientation of Yang-Mills moduli spaces and 4-manifold topology". Journal of Differential Geometry. 26 (3). doi:10.4310/jdg/1214441485. ISSN 0022-040X. S2CID 120208733.
  3. ^ a b c d Donaldson, S. K. (1983). An application of gauge theory to four-dimensional topology. Journal of Differential Geometry, 18(2), 279-315.
  4. ^ Taubes, C. H. (1982). Self-dual Yang–Mills connections on non-self-dual 4-manifolds. Journal of Differential Geometry, 17(1), 139-170.
  5. ^ Uhlenbeck, K. K. (1982). Connections with L p bounds on curvature. Communications in Mathematical Physics, 83(1), 31-42.
  6. ^ a b Uhlenbeck, K. K. (1982). Removable singularities in Yang–Mills fields. Communications in Mathematical Physics, 83(1), 11-29.

References edit