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 be a hyperplane. Its toric part is an open pair-of-pants.
Let be the moment map for (see (3)).
Lemma 3.1.
.
Proof.
By [12] is a spine of the amoeba and, therefore, its subset. The lemma can alternatively be verified by writing explicit inequalities defining . ∎
The complement consists of components. Each component is the region where one of the functions is maximal. In the component corresponding to we consider the foliation into straight lines parallel to the gradient of (the th basis vector). In the component corresponding to we consider the foliation into straight lines parallel to . These foliations glue to a singular foliation which has singularities at .

It is easy to smooth out (in a symmetric way with respect to the homogeneous coordinates permutations) at the open -cells of (see Figure 6). However, the singularities at the smaller-dimensional cells are essential. The leaves passing through an open -cell are homeomorphic to the cone over points.
We denote the resulting foliation with . The foliation is a singular fibration and defines the projection .
The following statement is a key lemma in the proof of the main theorems of this paper.
Lemma 3.2.
The proof of this lemma occupies the rest of this subsection.
To figure out the fibers of we need to understand the critical points of . Following [6] and [11] for a hypersurface we define the logarithmic Gauss map
by taking the composition of a branch of a holomorphic logarithm of each coordinate with the conventional Gauss map. This produces the following formula
where is the polynomial defining .
Note that the Newton polyhedron of coincides with the Newton polyhedron of . Therefore, by Kouchnirenko’s formula [9], . In particular, if then .
Lemma 3.3 (cf. Lemma 3 of [11]).
The set of critical points of coincides with .
Proof.
Let and let be a branch of a holomorphic logarithm defined in a neighborhood of . The point is critical for iff and the orbit of the real torus are not transversal at . But takes the tangent space to an orbit of to a translate of in .
Therefore, is critical iff contains at least purely imaginary vectors which is, in turn, equivalent to . ∎
Corollary 3.4.
The set of critical points of coincides with the real locus of (i.e. with the set of real solutions of ).
Proof.
Note that, since is defined over , we have . Note that extends to a map which is an isomorphism, since . ∎
Corollary 3.5.
The locus of critical values of is an immersed manifold transverse to the foliation .
Proof.
The map is an immersion since the map is an immersion (it is a trivial -covering of ).
To see the transversality we recall the definition of the foliation . For each component of the foliation is parallel to a vector normal to a facet of the Newton polyhedron of . Therefore, any hyperplane in the image is transverse to . Furthermore, hyperplanes close to being parallel to are close to the hyperplane in corresponding to this facet and therefore are far from the given component of . Thus the result of smoothing is also transverse to and the angle between them in is separated from 0. ∎
Note that is a stratified -fibration. Thus, the transversality of and implies that is a stratified fibration for . We need to show that the restriction of to open -cells of is a torus fibration.
Consider a point for a large . Note that is almost horizontal near . Thus the fiber of over is diffeomorphic to the fiber of a composition of and the linear projection onto the first coordinates. Note that the map obtained by taking the arguments of the first coordinates is a diffeomorphism. Recall that is given by the equation . The absolute values of the coordinates are fixed. For any value of their argument we take to get the unique point from corresponding to this choice of the arguments. Since are small .
We verify the conclusions of Theorem 3 item-by-item. The first and the last conclusions are vacuous in this case, since (and, therefore, as well) is contractible. The second one holds since is itself an open pair-of-pants.
To make the third conclusion true we have to modify a little. The fiber is not Lagrangian, but it is close to a Lagrangian torus . We can deform a little in a neighborhood of to make it intersect the fiber of along . Therefore, is Lagrangian for a nearby symplectic structure. By Moser’s trick (see e.g. [2]) there exists a self-diffeomorphism of constant outside of a neighborhood of and taking one symplectic structure to another. We redefine as . This ensures a Lagrangian fiber over one of the open -cells of . We do the same for all other -cells.