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Shioda projection and torsional coweight data
Definition
Let be a smooth projective complex threefold and let be a smooth projective fourfold with a specified elliptic-fibration-with-section structure as in Elliptic fibration with a section. Assume that is a chosen smooth resolution of a Weierstrass model as in Crepant resolution and matter surface; existence, projectivity, and elliptic flatness are hypotheses on this particular input. Let be the zero-section and let be another specified rational section, viewed by closure as a divisor class. Fix a smooth gauge divisor . The root datum used here is specified by an integer matrix , where , , for , and is symmetric positive definite when . These conditions define finite-type simply-laced Cartan data; no other root-system structure is used below. Let and be real vector spaces with bases and , respectively, and define their bilinear root-coroot pairing by . The simple roots and coroots are these basis vectors. Define the root and coroot lattices by and . If , take , to be the unique endomorphism of the zero space, and all basis-indexed sums to be empty.
Assume the chosen resolution has Cartan divisors and specified integral fibral curves over the generic point of , with . Intersections are degrees of the restricted divisor line bundles; all divisor classes and push-forwards below are taken in rational numerical equivalence, with proper push-forward along . Define the Shioda projection datum of by
For a finite-order section in the Mordell–Weil group of the generic fiber, put and define
The coweight lattice is ; the associated fractional coweight datum is the class of in . For , both and are . No claim that this class is nonzero, that the Shioda assignment is a group homomorphism, or that a physical gauge group is determined is part of this definition.
Definition references
Facts & Assumptions
Given: A specified smooth projective elliptic fourfold with a zero-section, a rational section, one chosen smooth projective resolution, and the finite-type simply-laced Cartan intersection data stated in the Definition.
Elliptic fibration with a section: “An elliptic fibration with section is a flat genus-one fibration together with a specified regular section , meaning .” Its Mordell–Weil group is the group of rational points on the pointed generic fiber.
Crepant resolution and matter surface: “A crepant resolution of is specified data where is smooth, is proper and birational, and .” The supplier does not assert projectivity or elliptic flatness; those are additional hypotheses here.
The sections, divisors, curves, Cartan matrix, and projective morphism between smooth varieties in the Definition are supplied data. In particular, is an explicit convention, not inferred from a Kodaira label.
Proof
The section closures and and the Cartan divisors are divisors on the smooth fourfold; their products with are codimension-two cycle classes. Properness of sends that codimension-two class to a codimension-one class on the threefold base, so its pullback is a divisor class. Each degree is integral, and multiplication by gives rational coefficients. Thus the displayed expression defines a rational numerical divisor class. The existence of the sectioned fibration and of a chosen smooth resolution is precisely the supplied input form in [F1] and [F2]; projectivity and the Cartan data are separately assumed in [A1].
A base-pulled divisor has degree zero on each curve , since maps to a point of . Write . The degree of the first difference in on is . The Cartan correction has degree , using symmetry and . Therefore for every .
For a torsion section , the divisor-degree vector is integral. The coefficient vector satisfies , again using symmetry of the simply-laced Cartan matrix. These pairings are integers, so by its definition. Its class modulo is therefore defined, although it may be zero.
Remarks
This item supplies only a local algebraic definition and the two displayed matrix checks. It does not prove that a given fibration has a projective crepant resolution, that the Mordell–Weil group is finitely generated, that torsion is nonzero, or that the coweight class acts as a gauge-group quotient. Those are separate geometric or physical inputs.