ScalingStacks

Fibrations with torus symmetry. [04JP]

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Fibrations with torus symmetry.

Let (X,ω)(X,\omega) be a symplectic 2​n2n-manifold and let μ:(X,ω)→𝔱∗\mu:(X,\omega)\rightarrow\mathfrak{t}^{\ast} be the moment map of a Hamiltonian TkT^{k}-action. Let t∈μ⁡(X)t\in\mu(X) and let πt:μ−1​(t)→Xt\pi_{t}:\mu^{-1}(t)\rightarrow X_{t} be the projection modulo the TkT^{k} action. When tt is a regular value of μ\mu, XtX_{t} is a smooth manifold and the symplectic form ω\omega descends to a symplectic form ωt\omega_{t} on XtX_{t}. When tt is a critical value of μ\mu, XtX_{t} may be a singular space and ωt\omega_{t} will be only defined on the smooth part of XtX_{t}. The space (Xt,ωt)(X_{t},\omega_{t}) is the Marsden-Weinstein reduced space at tt.

Remark 5.1.

We shall denote by

ωℂm=i2​∑kd​zk∧d​z¯k\omega_{\mathbb{C}^{m}}=\frac{i}{2}\sum_{k}dz_{k}\wedge d\overline{z}_{k}

the standard symplectic structure on ℂm\mathbb{C}^{m} and ω0\omega_{0} will denote the reduced symplectic form of the reduced space (Xt,ωt)(X_{t},\omega_{t}) at time t=0t=0.

Goldstein [5] and Gross [6] used reduced spaces to construct TkT^{k}-invariant (special) Lagrangian fibrations. The following is a particular case of [6]Thm. 1.2:

Proposition 5.2.

Let TkT^{k} act effectively on XX, k≤n−1k\leq n-1. Suppose that there is a continuous map G:X→MG:X\rightarrow M to an (n−k)(n-k)-dimensional manifold MM such that G⁡(T⋅x)=G⁡(x)G(T\cdot x)=G(x) for all T∈TkT\in T^{k}. Suppose that for tt in a dense subset of μ⁡(X)\mu(X) the induced maps Gt:Xt→MG_{t}:X_{t}\rightarrow M have fibres that are Lagrangian with respect to ωt\omega_{t}. Then f:X→μ⁡(X)×Mf:X\rightarrow\mu(X)\times M given by:

f=(μ,G)f=(\mu,G) (23)

defines a TkT^{k}-invariant Lagrangian fibration.

When the TkT^{k}-action has fixed points, the construction of Proposition 5.2 will produce fibrations with interesting singular fibres. We will give some explicit examples shortly.

Remark 5.3.

In the extremal case when k=n−1k=n-1, constructing Lagrangian fibrations using Proposition 5.2 is very easy. In this situation, the reduced spaces XtX_{t} are two dimensional and every map Gt:Xt→ℝG_{t}:X_{t}\rightarrow\mathbb{R} with 11-dimensional level sets defines a Lagrangian fibration on XtX_{t}. In particular, any Tn−1T^{n-1}-invariant continuous map G:X→ℝG:X\rightarrow\mathbb{R} which, on each XtX_{t}, descends to a map GtG_{t} with 11-dimensional level sets can be used to construct Lagrangian fibrations. We will make much use of this fact later on.

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