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3.4. A localization Q n ⊂ ( ℂ ∗ ) n + 1 of the standard hyperplane [04ST]

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3.4. A localization Qn⊂(ℂ∗)n+1Q^{n}\subset(\mathbb{C}^{*})^{n+1} of the standard hyperplane

The toric part H∘⊂(ℂ∗)n+1H^{\circ}\subset(\mathbb{C}^{*})^{n+1} of a hyperplane from 3.3 is a nice embedding of 𝒫n\mathcal{P}_{n} to (ℂ∗)n+1(\mathbb{C}^{*})^{n+1}. However for our purposes it is convenient to modify it in a neighborhood of infinity to get a different submanifold QnQ^{n} which is better suited for gluing.

Note that the symmetric group Sn+2S_{n+2} acts on (ℂ∗)n+1(\mathbb{C}^{*})^{n+1} by interchanging the functions z1,…,zn+1,1z1​…​zn+1z_{1},\dots,z_{n+1},\frac{1}{z_{1}\dots z_{n+1}}. This action is inherited from the action of Sn+2S_{n+2} on ℂ​ℙn+1{\mathbb{C}}{\mathbb{P}}^{n+1} interchanging the homogeneous coordinates since (ℂ∗)n+1⊂ℂ​ℙn+1(\mathbb{C}^{*})^{n+1}\subset{\mathbb{C}}{\mathbb{P}}^{n+1} is invariant. The hyperplane H∘H^{\circ} is invariant with respect to this action.

Proposition 3.6.

There exists a proper submanifold Qn⊂(ℂ∗)n+1Q^{n}\subset(\mathbb{C}^{*})^{n+1} such that

  • •

    QnQ^{n} is embedded to (ℂ∗)n+1(\mathbb{C}^{*})^{n+1} symplectically, i.e. so that the restriction of the form (2) to QnQ^{n} is a symplectic form.

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    QnQ^{n} is isotopic to H∘H^{\circ} in (ℂ∗)n+1(\mathbb{C}^{*})^{n+1}.

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    The composition πℱ∘Logt|Qn\pi_{\mathcal{F}}\circ\operatorname{Log}_{t}|_{Q^{n}} is a stratified TnT^{n}-fibration that satisfies to all hypotheses of Theorem 3.

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    the closure Qn¯\bar{Q^{n}} of QnQ^{n} in ℂ​ℙn+1⊃(ℂ∗)n+1{\mathbb{C}}{\mathbb{P}}^{n+1}\supset(\mathbb{C}^{*})^{n+1} is a smooth manifold isotopic to HH.

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    QnQ^{n} is invariant with respect to the action of the symmetric group Sn+2S_{n+2} on (ℂ∗)n+1(\mathbb{C}^{*})^{n+1} (see above).

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    For a sufficiently large M>0M>0

    Qn∩(ℂ∗)−Mn+1=Qn−1×C−M∗,Q^{n}\cap(\mathbb{C}^{*})^{n+1}_{-M}=Q^{n-1}\times\\ C^{*}_{-M},

    where (ℂ∗)−Mn+1={(z1,…,zn+1)∈(ℂ∗)n+1​|log|​zn+1|<−M}(\mathbb{C}^{*})^{n+1}_{-M}=\{(z_{1},\dots,z_{n+1})\in(\mathbb{C}^{*})^{n+1}\ |\ \log|z_{n+1}|<-M\} and ℂ−M∗={z∈ℂ∗​|log|​z|<−M}\mathbb{C}^{*}_{-M}=\{z\in\mathbb{C}^{*}\ |\ \log|z|<-M\}. In particular, the intersection Qn∩(ℂ∗)−Mn+1Q^{n}\cap(\mathbb{C}^{*})^{n+1}_{-M} is invariant under a translation zn+1↦c​zn+1z_{n+1}\mapsto cz_{n+1}, 0<c<10<c<1.

Refer to caption

Figure 7. The amoeba of the localization QnQ^{n} of a hyperplane.
Proof.

We construct QnQ^{n} inductively by dimension nn. If n=0n=0 then H∘H^{\circ} is a point and Q0=H∘Q^{0}=H^{\circ}. Assume that QkQ^{k}, k<nk<n is already constructed. Consider the simplex

Δn(R)={x∈ℝn+1|−xj≤R,∑jxj≤R}.\Delta_{n}(R)=\{x\in\mathbb{R}^{n+1}\ |\ -x_{j}\leq R,\sum\limits_{j}x_{j}\leq R\}.

Each its kk-dimensional face is dual to a (n+1−k)(n+1-k)-cell of Σn\Sigma_{n}. Fix a sufficiently large number Rn>0R_{n}>0.

First we define Qn∩Log−1⁡(∂Δ⁡(Rn))Q^{n}\cap\operatorname{Log}^{-1}(\partial\Delta(R_{n})). Each kk-face of Δ⁡(Rn)\Delta(R_{n}) is contained in a unique affine kk-space AA in ℝn+1\mathbb{R}^{n+1}. Furthermore, the adjoint faces cut the polyhedron Δk−1​(Rn)⊂A\Delta_{k-1}(R_{n})\subset A. Thus we may identify AA with ℝk\mathbb{R}^{k} and, therefore, Log−1⁡(A)\operatorname{Log}^{-1}(A) with (ℂ∗)k(\mathbb{C}^{*})^{k}. By the induction assumption we already have Qk−1⊂(ℂ∗)k→ℝkQ^{k-1}\subset(\mathbb{C}^{*})^{k}\to\mathbb{R}^{k}. We define Qn∩Log−1⁡(∂Δ⁡(Rn))Q^{n}\cap\operatorname{Log}^{-1}(\partial\Delta(R_{n})) to be equal to the union of these QkQ^{k} for all faces of ∂Δ⁡(Rn)\partial\Delta(R_{n}). By the induction hypothesis (and since RnR_{n} was large enough) the choices over different faces agree.

Our next step is to extend QnQ^{n} to the complement of Log−1⁡(Δ⁡(Rn))\operatorname{Log}^{-1}(\Delta(R_{n})). For each face Δ′\Delta^{\prime} of ∂Δ⁡(Rn)\partial\Delta(R_{n}) consider its outer normal cone CΔ′⊂ℝn+1C_{\Delta^{\prime}}\subset\mathbb{R}^{n+1} (e.g. if Δ′\Delta^{\prime} is a facet then CΔ′C_{\Delta^{\prime}} is a ray). We define

Qn∩Log−1(Δ′+CΔ′)=⋃v→∈CΔ′ev→Qn∩Log−1(Δ′).Q^{n}\cap\operatorname{Log}^{-1}(\Delta^{\prime}+C_{\Delta^{\prime}})=\bigcup\limits_{\stackrel{{\scriptstyle\to}}{{v}}\in C_{\Delta^{\prime}}}e^{\stackrel{{\scriptstyle\to}}{{v}}}Q^{n}\cap\operatorname{Log}^{-1}(\Delta^{\prime}).

In other words, we span the region above the normal cone of a kk-face Δ′\Delta^{\prime} by the translates of the manifold QkQ^{k}.

We set Qn∩Log−1⁡(Δ⁡(Rn−1))=H∘∩Log−1⁡(Δ⁡(Rn−1))Q^{n}\cap\operatorname{Log}^{-1}(\Delta(R_{n}-1))=H^{\circ}\cap\operatorname{Log}^{-1}(\Delta(R_{n}-1)). By now we have defined QnQ^{n} everywhere, but Log−1⁡(Δ⁡(Rn)∖Δ⁡(Rn−1))\operatorname{Log}^{-1}(\Delta(R_{n})\smallsetminus\Delta(R_{n}-1)).

Consider a facet Δ′\Delta^{\prime} of ∂Δ⁡(Rn−1)\partial\Delta(R_{n}-1), e.g. the one sitting in the hyperplane A={xn+1=Rn−1}A=\{x_{n+1}=R_{n}-1\}. Since RnR_{n} is large enough, zn+1Rn−1z_{n+1}^{R_{n}-1} is small enough and the intersection H∘∩Log−1⁡(A)H^{\circ}\cap\operatorname{Log}^{-1}(A) is close enough to the zero set of z1+⋯+zn+1=0z_{1}+\dots+z_{n}+1=0. By the induction hypothesis this zero set can be deformed to Qn−1Q^{n-1}. We define Qn∩{Log|zn+1|=t}Q^{n}\cap\{\operatorname{Log}|z_{n+1}|=t\}, −Rn≤t≤−Rn+1-R_{n}\leq t\leq-R_{n}+1 using this deformation. We repeat the same procedure for all other facets of Δ⁡(Rn−1)\Delta(R_{n}-1). ∎

Denote Q¯n=Qn∩Log−1⁡(Δ⁡(Rn+1))\bar{Q}^{n}=Q^{n}\cap\operatorname{Log}^{-1}(\Delta(R_{n}+1)). This is “the kernel” of QnQ^{n} and is diffeomorphic to a closed pair-of-pants 𝒫n¯\bar{\mathcal{P}_{n}} (as a manifold with boundary and corners).

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