ProofComplete

Proof of the Duistermaat-Heckman Theorem

The Duistermaat-Heckman theorem describes the exact behavior of the push-forward of the symplectic volume form under the moment map. It shows that this measure is piecewise polynomial, a remarkable exactness result.


Statement

Theorem5.3Duistermaat-Heckman Theorem

Let (M2n,ω)(M^{2n}, \omega) be a compact symplectic manifold with a Hamiltonian S1S^1-action and moment map μ:MR\mu: M \to \mathbb{R}. Then the Duistermaat-Heckman measure μ ⁣(ωnn!)\mu_*\!\left(\frac{\omega^n}{n!}\right) is a piecewise polynomial measure on R\mathbb{R}. Equivalently, the oscillatory integral Meitμωnn!=FMS1eitμ(F)j=1nF(itwj(F))\int_M e^{i t \mu} \frac{\omega^n}{n!} = \sum_{F \subseteq M^{S^1}} \frac{e^{it\mu(F)}}{\prod_{j=1}^{n_F} (i t w_j(F))} is computed exactly by the fixed-point contributions (localization formula), where wj(F)w_j(F) are the weights of the S1S^1-action on the normal bundle of the fixed component FF.


Proof Sketch

Proof

The key tool is the equivariant cohomology localization formula (Atiyah-Bott-Berline-Vergne).

The equivariant symplectic form ω+tμ\omega + t\mu is equivariantly closed. The integral Meω+tμ\int_M e^{\omega + t\mu} can be computed by localization: Meω+tμ=FFeωF+tμ(F)eT(NF),\int_M e^{\omega + t\mu} = \sum_{F} \int_F \frac{e^{\omega_F + t\mu(F)}}{e_T(N_F)}, where the sum is over fixed components FF, ωF\omega_F is the restriction of ω\omega, and eT(NF)=j(twj)e_T(N_F) = \prod_j (tw_j) is the equivariant Euler class of the normal bundle.

For isolated fixed points pp with weights w1,,wnw_1, \ldots, w_n: Meω+tμ=petμ(p)j=1n(twj(p)).\int_M e^{\omega + t\mu} = \sum_p \frac{e^{t\mu(p)}}{\prod_{j=1}^n (tw_j(p))}.

The Duistermaat-Heckman measure is the inverse Fourier transform of this expression, which is piecewise polynomial. \square

Example$S^2$ with Rotation

For S2S^2 with the standard S1S^1-rotation and moment map μ=\mu = height function, the DH measure is μ(ω)=dt\mu_*(\omega) = dt on [1,1][-1, 1] (the uniform measure). The fixed points are the north and south poles with μ=±1\mu = \pm 1 and weights ±1\pm 1: S2eitμω=eitit+eitit=2sintt.\int_{S^2} e^{it\mu}\omega = \frac{e^{it}}{it} + \frac{e^{-it}}{-it} = \frac{2\sin t}{t}.

RemarkWall-Crossing

When μ\mu crosses a critical value, the DH polynomial changes. The change (wall-crossing formula) is determined by the fixed-point data at the critical level. This connects the DH theorem to the variation of symplectic quotients.