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3.3. Hyperplanes in the projective space [04SI]

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3.3. Hyperplanes in the projective space

This is a fundamental example for the main theorems. Let H={z1+⋯+zn+1+1=0}⊂ℂℙn+1H=\{z_{1}+\dots+z_{n+1}+1=0\}\subset{\mathbb{C}}{\mathbb{P}}^{n+1} be a hyperplane. Its toric part H∘=H∩(ℂ∗)n+1H^{\circ}=H\cap(\mathbb{C}^{*})^{n+1} is an open pair-of-pants.

Let Log\operatorname{Log} be the moment map for (ℂ∗)n+1(\mathbb{C}^{*})^{n+1} (see (3)).

Lemma 3.1.

Σn⊂Log⁡(H∘)\Sigma_{n}\subset\operatorname{Log}(H^{\circ}).

Proof.

By [12] Σn\Sigma_{n} is a spine of the amoeba Log⁡(H∘)\operatorname{Log}(H^{\circ}) and, therefore, its subset. The lemma can alternatively be verified by writing explicit inequalities defining Log⁡(H∘)\operatorname{Log}(H^{\circ}). ∎

The complement ℝn+1∖Σn\mathbb{R}^{n+1}\smallsetminus\Sigma_{n} consists of n+2n+2 components. Each component is the region where one of the functions 0,x1,…,xn+10,x_{1},\dots,x_{n+1} is maximal. In the component corresponding to xjx_{j} we consider the foliation into straight lines parallel to the gradient of xjx_{j} (the jjth basis vector). In the component corresponding to 00 we consider the foliation into straight lines parallel to (1,…,1)(1,\dots,1). These foliations glue to a singular foliation ℱ′\mathcal{F}^{\prime} which has singularities at Σn\Sigma_{n}.

Refer to caption

Figure 6. The amoeba Log⁡(H∘)\operatorname{Log}(H^{\circ}) together with the foliation ℱ′\mathcal{F}^{\prime} and its deformation ℱ\mathcal{F}.

It is easy to smooth out ℱ′\mathcal{F}^{\prime} (in a symmetric way with respect to the homogeneous coordinates permutations) at the open nn-cells of Σn\Sigma_{n} (see Figure 6). However, the singularities at the smaller-dimensional cells are essential. The leaves passing through an open (n−k)(n-k)-cell are homeomorphic to the cone over k+2k+2 points.

We denote the resulting foliation with ℱ\mathcal{F}. The foliation ℱ\mathcal{F} is a singular fibration and defines the projection πℱ:ℝn+1→Σn\pi_{\mathcal{F}}:\mathbb{R}^{n+1}\to\Sigma_{n}.

The following statement is a key lemma in the proof of the main theorems of this paper.

Lemma 3.2.

The composition

λH=πℱ∘Log:H∘→Σn\lambda_{H}=\pi_{\mathcal{F}}\circ\operatorname{Log}:H^{\circ}\to\Sigma_{n}

is a stratified TnT^{n}-fibration in the sense of Definition 7. It satisfies to all conclusions of Theorem 3 except for the third one. The fibration λH\lambda_{H} can be deformed so that the third condition will also hold.

The proof of this lemma occupies the rest of this subsection.

To figure out the fibers of λH\lambda_{H} we need to understand the critical points of Log|H∘\operatorname{Log}|_{H^{\circ}}. Following [6] and [11] for a hypersurface V∘⊂(ℂ∗)n+1V^{\circ}\subset(\mathbb{C}^{*})^{n+1} we define the logarithmic Gauss map

γ:V∘→ℂ​ℙn\gamma:V^{\circ}\to{\mathbb{C}}{\mathbb{P}}^{n}

by taking the composition of a branch of a holomorphic logarithm of each coordinate with the conventional Gauss map. This produces the following formula

γ(z1,…,zn+1)=[z1∂f∂z1:…:zn+1∂f∂zn+1],\gamma(z_{1},\dots,z_{n+1})=[z_{1}\frac{\partial f}{\partial z_{1}}:\dots:z_{n+1}\frac{\partial f}{\partial z_{n+1}}],

where ff is the polynomial defining V∘V^{\circ}.

Note that the Newton polyhedron of zj​∂f∂zjz_{j}\frac{\partial f}{\partial z_{j}} coincides with the Newton polyhedron Δ\Delta of ff. Therefore, by Kouchnirenko’s formula [9], deg⁡γ=(n+1)!​Vol⁡Δ\deg\gamma=(n+1)!\operatorname{Vol}\Delta. In particular, if V∘=H∘V^{\circ}=H^{\circ} then deg⁡γ=1\deg\gamma=1.

Lemma 3.3 (cf. Lemma 3 of [11]).

The set of critical points of Log|V∘\operatorname{Log}|_{V^{\circ}} coincides with γ−1​(ℝ​Pn)\gamma^{-1}(\mathbb{R}P^{n}).

Proof.

Let z∈V∘z\in V^{\circ} and let ℒ​o​g\mathcal{L}og be a branch of a holomorphic logarithm (z1,…,zn+1)↦(log⁡(z1),…,log⁡(zn+1))(z_{1},\dots,z_{n+1})\mapsto(\log(z_{1}),\dots,\log(z_{n+1})) defined in a neighborhood of zz. The point zz is critical for Log|V∘\operatorname{Log}|_{V^{\circ}} iff V∘V^{\circ} and the orbit of the real torus TnT^{n} are not transversal at zz. But ℒ​o​g\mathcal{L}og takes the tangent space to an orbit of TnT^{n} to a translate of i​ℝn+1i\mathbb{R}^{n+1} in ℂn+1\mathbb{C}^{n+1}.

Therefore, zz is critical iff ℒ​o​g​(Tz​V∘)\mathcal{L}og(T_{z}V^{\circ}) contains at least nn purely imaginary vectors which is, in turn, equivalent to γ⁡(z)∈ℝ​Pn\gamma(z)\in\mathbb{R}P^{n}. ∎

Corollary 3.4.

The set of critical points of Log|H∘\operatorname{Log}|_{H^{\circ}} coincides with the real locus ℝ​H∘\mathbb{R}H^{\circ} of H∘H^{\circ} (i.e. with the set of real solutions of z1+⋯+zn+1+1=0z_{1}+\dots+z_{n+1}+1=0).

Proof.

Note that, since H∘H^{\circ} is defined over ℝ\mathbb{R}, we have γ⁡(ℝ​H∘)⊂ℝ​ℙn\gamma(\mathbb{R}H^{\circ})\subset{\mathbb{R}}{\mathbb{P}}^{n}. Note that γ\gamma extends to a map H→ℂ​ℙnH\to{\mathbb{C}}{\mathbb{P}}^{n} which is an isomorphism, since deg⁡γ=1\deg\gamma=1. ∎

Corollary 3.5.

The locus 𝒟⊂Log⁡(H∘)\mathcal{D}\subset\operatorname{Log}(H^{\circ}) of critical values of Log|H∘\operatorname{Log}|_{H^{\circ}} is an immersed manifold transverse to the foliation ℱ\mathcal{F}.

Proof.

The map Log|ℝ​H∘:ℝH∘→𝒟⊂ℝn+1\operatorname{Log}|_{\mathbb{R}H^{\circ}}:\mathbb{R}H^{\circ}\to\mathcal{D}\subset\mathbb{R}^{n+1} is an immersion since the map Log|(ℝ∗)n+1:(ℝ∗)n+1→ℝn+1\operatorname{Log}|_{(\mathbb{R}^{*})^{n+1}}:(\mathbb{R}^{*})^{n+1}\to\mathbb{R}^{n+1} is an immersion (it is a trivial 2n+12^{n+1}-covering of ℝn+1\mathbb{R}^{n+1}).

To see the transversality we recall the definition of the foliation ℱ′\mathcal{F}^{\prime}. For each component of ℝn+1∖Σn\mathbb{R}^{n+1}\smallsetminus\Sigma_{n} the foliation ℱ′\mathcal{F}^{\prime} is parallel to a vector v→\stackrel{{\scriptstyle\to}}{{v}} normal to a facet of the Newton polyhedron of H∘H^{\circ}. Therefore, any hyperplane in the image γ⁡(ℝ​H∘)\gamma(\mathbb{R}H^{\circ}) is transverse to v→\stackrel{{\scriptstyle\to}}{{v}}. Furthermore, hyperplanes close to being parallel to v→\stackrel{{\scriptstyle\to}}{{v}} are close to the hyperplane in ℂ​ℙn+1{\mathbb{C}}{\mathbb{P}}^{n+1} corresponding to this facet and therefore are far from the given component of ℝn+1∖Σn\mathbb{R}^{n+1}\smallsetminus\Sigma_{n}. Thus the result ℱ\mathcal{F} of smoothing is also transverse to 𝒟\mathcal{D} and the angle between them in ℝn+1\mathbb{R}^{n+1} is separated from 0. ∎

Note that πℱ\pi_{\mathcal{F}} is a stratified [−1,1][-1,1]-fibration. Thus, the transversality of 𝒟\mathcal{D} and ℱ\mathcal{F} implies that λH\lambda_{H} is a stratified fibration for Σn\Sigma_{n}. We need to show that the restriction of πF\pi_{F} to open nn-cells of Σ\Sigma is a torus fibration.

Consider a point x=(−t,…,−t,0)x=(-t,\dots,-t,0) for a large t>0t>0. Note that 𝒟\mathcal{D} is almost horizontal near xx. Thus the fiber of λH\lambda_{H} over xx is diffeomorphic to the fiber FF of a composition of Log|H∘\operatorname{Log}|_{H^{\circ}} and the linear projection onto the first nn coordinates. Note that the map F→TnF\to T^{n} obtained by taking the arguments of the first nn coordinates is a diffeomorphism. Recall that H∘H^{\circ} is given by the equation z1+⋯+zn+1+1=0z_{1}+\dots+z_{n+1}+1=0. The absolute values of the coordinates z1,…,znz_{1},\dots,z_{n} are fixed. For any value of their argument we take zn+1=1−z1−⋯−znz_{n+1}=1-z_{1}-\dots-z_{n} to get the unique point from FF corresponding to this choice of the arguments. Since |z1|,…,|zn||z_{1}|,\dots,|z_{n}| are small zn+1≠0z_{n+1}\neq 0.

We verify the conclusions of Theorem 3 item-by-item. The first and the last conclusions are vacuous in this case, since Σn\Sigma_{n} (and, therefore, Σ¯n\bar{\Sigma}_{n} as well) is contractible. The second one holds since H∘H^{\circ} is itself an open pair-of-pants.

To make the third conclusion true we have to modify λH\lambda_{H} a little. The fiber FF is not Lagrangian, but it is close to a Lagrangian torus Λ={|zj|=const,j=1,…,n,zn+1=−1}\Lambda=\{|z_{j}|=\operatorname{const},\ j=1,\dots,n,\ z_{n+1}=-1\}. We can deform H∘H^{\circ} a little in a neighborhood of Log−1⁡(x)\operatorname{Log}^{-1}(x) to make it intersect the fiber of πℱ∘Log\pi_{\mathcal{F}}\circ\operatorname{Log} along Λ\Lambda. Therefore, FF is Lagrangian for a nearby symplectic structure. By Moser’s trick (see e.g. [2]) there exists a self-diffeomorphism hh of H∘H^{\circ} constant outside of a neighborhood of Log−1⁡(x)\operatorname{Log}^{-1}(x) and taking one symplectic structure to another. We redefine λ\lambda as λ∘h\lambda\circ h. This ensures a Lagrangian fiber over one of the (n+22)\begin{pmatrix}n+2\\ 2\end{pmatrix} open nn-cells of Σn\Sigma_{n}. We do the same for all other nn-cells.

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