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Donaldson's theorem

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On when a definite intersection form of a smooth 4-manifold is diagonalizable

Inmathematics, and especiallydifferential topology andgauge theory,Donaldson's theorem states that adefiniteintersection form of aclosed,oriented,smooth manifold ofdimension 4 isdiagonalizable. If the intersection form is positive (negative) definite, it can be diagonalized to theidentity matrix (negative identity matrix) over theintegers. The original version[1] of the theorem required the manifold to besimply connected, but it was later improved to apply to 4-manifolds with anyfundamental group.[2]

History

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The theorem was proved bySimon Donaldson. This was a contribution cited for hisFields Medal in 1986.

Idea of proof

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Donaldson's proof utilizes theYang–Mills moduli spaceMP{\displaystyle {\mathcal {M}}_{P}} of solutions to theanti-self-duality equations on aprincipalSU(2){\displaystyle \operatorname {SU} (2)}-bundleP{\displaystyle P} over the four-manifoldX{\displaystyle X}. By theAtiyah–Singer index theorem, the dimension of the moduli space is given by

dimM=8k3(1b1(X)+b+(X)),{\displaystyle \dim {\mathcal {M}}=8k-3(1-b_{1}(X)+b_{+}(X)),}

wherek=c2(P){\displaystyle k=c_{2}(P)} is aChern class,b1(X){\displaystyle b_{1}(X)} is the firstBetti number ofX{\displaystyle X}, andb+(X){\displaystyle b_{+}(X)} is the dimension of the positive-definite subspace ofH2(X,R){\displaystyle H_{2}(X,\mathbb {R} )} with respect to the intersection form. WhenX{\displaystyle X} is simply-connected with definite intersection form, possibly after changing orientation, one always hasb1(X)=0{\displaystyle b_{1}(X)=0} andb+(X)=0{\displaystyle b_{+}(X)=0}. Thus taking any principalSU(2){\displaystyle \operatorname {SU} (2)}-bundle withk=1{\displaystyle k=1}, one obtains a moduli spaceM{\displaystyle {\mathcal {M}}} of dimension five.

Cobordism given by theYang–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 exactlyb2(X){\displaystyle b_{2}(X)} many.[3] Results ofClifford Taubes andKaren Uhlenbeck show that whilstM{\displaystyle {\mathcal {M}}} is non-compact, its structure at infinity can be readily described.[4][5][6] Namely, there is an open subset ofM{\displaystyle {\mathcal {M}}}, sayMε{\displaystyle {\mathcal {M}}_{\varepsilon }}, such that for sufficiently small choices of parameterε{\displaystyle \varepsilon }, there is a diffeomorphism

MεX×(0,ε){\displaystyle {\mathcal {M}}_{\varepsilon }{\xrightarrow {\quad \cong \quad }}X\times (0,\varepsilon )}.

The work of Taubes and Uhlenbeck essentially concerns constructing sequences of ASD connections on the four-manifoldX{\displaystyle X} with curvature becoming infinitely concentrated at any given single pointxX{\displaystyle x\in 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 usingUhlenbeck's singularity theorem.[6][3]

Donaldson observed that the singular points in the interior ofM{\displaystyle {\mathcal {M}}} corresponding to reducible connections could also be described: they looked likecones over thecomplex projective planeCP2{\displaystyle \mathbb {CP} ^{2}}. Furthermore, we can count the number of such singular points. LetE{\displaystyle E} be theC2{\displaystyle \mathbb {C} ^{2}}-bundle overX{\displaystyle X} associated toP{\displaystyle P} by the standard representation ofSU(2){\displaystyle SU(2)}. Then, reducible connections modulo gauge are in a 1-1 correspondence with splittingsE=LL1{\displaystyle E=L\oplus L^{-1}} whereL{\displaystyle L} is a complex line bundle overX{\displaystyle X}.[3] WheneverE=LL1{\displaystyle E=L\oplus L^{-1}} we may compute:

1=k=c2(E)=c2(LL1)=Q(c1(L),c1(L)){\displaystyle 1=k=c_{2}(E)=c_{2}(L\oplus L^{-1})=-Q(c_{1}(L),c_{1}(L))},

whereQ{\displaystyle Q} is the intersection form on the second cohomology ofX{\displaystyle X}. Since line bundles overX{\displaystyle X} are classified by their first Chern classc1(L)H2(X;Z){\displaystyle c_{1}(L)\in H^{2}(X;\mathbb {Z} )}, we get that reducible connections modulo gauge are in a 1-1 correspondence with pairs±αH2(X;Z){\displaystyle \pm \alpha \in H^{2}(X;\mathbb {Z} )} such thatQ(α,α)=1{\displaystyle Q(\alpha ,\alpha )=-1}. Let the number of pairs ben(Q){\displaystyle n(Q)}. An elementary argument that applies to any negative definite quadratic form over the integers tells us thatn(Q)rank(Q){\displaystyle n(Q)\leq {\text{rank}}(Q)}, with equality if and only ifQ{\displaystyle 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 ofCP2{\displaystyle \mathbb {CP} ^{2}}. Secondly, glue in a copy ofX{\displaystyle X} itself at infinity. The resulting space is acobordism betweenX{\displaystyle X} and a disjoint union ofn(Q){\displaystyle n(Q)} copies ofCP2{\displaystyle \mathbb {CP} ^{2}} (of unknown orientations). The signatureσ{\displaystyle \sigma } of a four-manifold is a cobordism invariant. Thus, becauseX{\displaystyle X} is definite:

rank(Q)=b2(X)=σ(X)=σ(n(Q)CP2)n(Q){\displaystyle {\text{rank}}(Q)=b_{2}(X)=\sigma (X)=\sigma (\bigsqcup n(Q)\mathbb {CP} ^{2})\leq n(Q)},

from which one concludes the intersection form ofX{\displaystyle X} is diagonalizable.

Extensions

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

1) Any indefinite non-diagonalizable intersection form gives rise to a four-dimensionaltopological manifold with nodifferentiable structure (so cannot be smoothed).

2) Two smooth simply-connected 4-manifolds arehomeomorphic, if and only if, their intersection forms have the samerank,signature, and parity.

See also

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Notes

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  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. ^abcdDonaldson, 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. ^abUhlenbeck, K. K. (1982). Removable singularities in Yang–Mills fields. Communications in Mathematical Physics, 83(1), 11-29.

References

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