2.1 Notation and strategy [04NG]
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2.1 Notation and strategy
We set such that . Since for every irreducible component of , the intersection is connected by assumption, this allows us to denote by with the components of intersecting transversally along , so that the toric boundary of is given by .
Remark 2.1.1.
The dlt assumption on and the toricness of ensure that is smooth, and that is an snc pair. Indeed, the singular locus of is a union of torus invariant subvarieties (see [CLS11, Proposition 11.1.2]), hence the generic point of a component of the singular locus is the generic point of a stratum of . However, is a dlt pair, thus snc at the generic point of each stratum of .
Remark 2.1.2.
The smoothness of and the assumption that the components of are Cartier divisors imply that is regular at any point of . Indeed, for any point and , let be a local equation of at . As is a regular local ring of dimension , can be extended to form a regular system of parameters for .
We denote by the fan of . Its rays are given by for , with primitive generators ; the maximal cones of are in bijection with the set of unordered -tuples such that . For a maximal cone of , we write .
Lemma 2.1.3.
For any maximal cone of , we have
Proof.
The smoothness of (see Remark 2.1.1) implies that the primitive generators of form a -basis of , which is equivalent to the condition ∎
Let be the normal bundle of in , and denote by the zero section. We write so that . Since any Cartier divisor on is linearly equivalent to a toric one, for any , there exist integers such that
| (2.1.4) |
For we set and verify that
We obtain that and for all in
| (2.1.5) |
The normal bundle is a toric variety of dimension . The corresponding fan lies in and consists of the following cones and their faces (see [CLS11, §7.3] for a reference). Let be the standard basis of ; given a cone , we have
In particular, we denote the rays of by
Proposition 2.1.6.
For any 1-dimensional toric stratum
| (2.1.7) |
Proof.
The map
is -linear, sends all the primitive generators of the rays of to by Eq. 2.1.5, and is compatible with and the fan of . Thus, it induces a toric morphism whose fiber over is the toric boundary of . The base change to is a toric -scheme, whose generic fiber is isomorphic to . The special fiber can be written as , where the combinatoric of intersections between components is exactly the same as in .
We prove Theorem B by constructing a formal isomorphism
More specifically, we proceed as follows. We set the notations and .
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(Sections 2.2 and 2.3) Let be a maximal cone. Denote by and the corresponding toric affine charts in and respectively. This induces an open formal subscheme of , which we denote by . We construct a morphism
in a similar manner to [NXY19]: we construct divisors and on , whose defining equations on the chart yields the morphism . The equations are induced by sections of and : these are first constructed on , then extended to by the nef condition on the conormal bundle assumed in Theorem B, which ensures the vanishing of higher cohomology groups for the tensor powers of .
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(Sections 2.4 and 2.5) Let and be two maximal cones of intersecting along a face of codimension one. We establish relations among the respective divisors and construct sections on from those on . This allows us to prove that the morphisms on the charts ’s can be chosen so that they are compatible on the overlaps . This yields a well defined morphism which extends the identity on and preserves the ideal , so that it turns out to be an isomorphism.