Donaldson's theorem

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Short description: On when a definite intersection form of a smooth 4-manifold is diagonalisable

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

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

Idea of proof

Donaldson's proof utilizes the moduli space ℳP of solutions to the anti-self-duality equations on a principal SU⁡(2)-bundle P over the four-manifold X. By the Atiyah–Singer index theorem, the dimension of the moduli space is given by

dim⁡ℳ=8k−3(1−b1(X)+b+(X)),

where c2(P)=k, b1(X) is the first Betti number of X and b+(X) is the dimension of the positive-definite subspace of H2(X,ℝ) with respect to the intersection form. When X is simply-connected with definite intersection form, possibly after changing orientation, one always has b1(X)=0 and b+(X)=0. Thus taking any principal SU⁡(2)-bundle with k=1, one obtains a moduli space ℳ 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 b2(X) many.[3] Results of Clifford Taubes and Karen Uhlenbeck show that whilst ℳ is non-compact, its structure at infinity can be readily described.[4][5][6] Namely, there is an open subset of ℳ, say ℳε, such that for sufficiently small choices of parameter ε, there is a diffeomorphism

ℳε→≅X×(0,ε).

The work of Taubes and Uhlenbeck essentially concerns constructing sequences of ASD connections on the four-manifold X with curvature becoming infinitely concentrated at any given single point x∈X. 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 ℳ corresponding to reducible connections could also be described: they looked like cones over the complex projective plane ℂℙ2. Furthermore, we can count the number of such singular points. Let E be the ℂ2-bundle over X associated to P by the standard representation of SU(2). Then, reducible connections modulo gauge are in a 1-1 correspondence with splittings E=L⊕L−1 where L is a complex line bundle over X.[3] Whenever E=L⊕L−1 we may compute:

1=k=c2(E)=c2(L⊕L−1)=−Q(c1(L),c1(L)),

where Q is the intersection form on the second cohomology of X. Since line bundles over X are classified by their first Chern class c1(L)∈H2(X;ℤ), we get that reducible connections modulo gauge are in a 1-1 correspondence with pairs ±α∈H2(X;ℤ) such that Q(α,α)=−1. Let the number of pairs be n(Q). An elementary argument that applies to any negative definite quadratic form over the integers tells us that n(Q)≤rank(Q), with equality if and only if Q 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 ℂℙ2. Secondly, glue in a copy of X itself at infinity. The resulting space is a cobordism between X and a disjoint union of n(Q) copies of ℂℙ2 (of unknown orientations). The signature σ of a four-manifold is a cobordism invariant. Thus, because X is definite:

rank(Q)=b2(X)=σ(X)=σ(⨆n(Q)ℂℙ2)≤n(Q),

from which one concludes the intersection form of X is diagonalizable.

Extensions

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 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

Notes

  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. http://dx.doi.org/10.4310/jdg/1214437665. 
  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. http://dx.doi.org/10.4310/jdg/1214441485. 
  3. ↑ 3.0 3.1 3.2 3.3 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. ↑ 6.0 6.1 Uhlenbeck, K. K. (1982). Removable singularities in Yang–Mills fields. Communications in Mathematical Physics, 83(1), 11-29.

References

  • Donaldson, S. K. (1983), "An application of gauge theory to four-dimensional topology", Journal of Differential Geometry 18 (2): 279–315, doi:10.4310/jdg/1214437665 
  • Donaldson, S. K.; Kronheimer, P. B. (1990), The Geometry of Four-Manifolds, Oxford Mathematical Monographs, ISBN 0-19-850269-9 
  • Freed, D. S.; Uhlenbeck, K. (1984), Instantons and Four-Manifolds, Springer 
  • Freedman, M.; Quinn, F. (1990), Topology of 4-Manifolds, Princeton University Press 
  • Scorpan, A. (2005), The Wild World of 4-Manifolds, American Mathematical Society