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DerivedAlgGeo.AlgebraicGeometry.Numerical.Stability.DivisorialMukai

√td_X read off a numerical realization, and Bridgeland's K3 charge #

CentralCharge/Divisorial/Mukai.lean owns the Mukai vector and the Mukai charge on an abstract real divisor space, parameterized by a supplied SqrtTodd: the codimension-one class √td₁ and the number ∫√td₂. This file supplies that datum from geometry rather than by hand, using the sqrtToddComp of Numerical/Mukai/SqrtTodd.lean, and identifies the result on a K3.

Three things are proved.

What this does not do, and what has since been done elsewhere #

The statements below hold for any realization of any NumericalVarietyData 2 satisfying IsK3; this file constructs none.

Two gaps this section used to record are now closed, in the examples rather than here. Examples/Surface/RankOneRealization.lean constructs the numerical realization of the K3 model of Models/Surface/K3.lean, and Examples/Surface/K3MukaiComparison.lean compares the real Mukai extension used here with the integral Mukai.MukaiLattice of GrothendieckGroup/MukaiVector.lean, through the lattice map that Numerical/Mukai/Integral.lean asks for. Both remain outside this file, which stays free of any particular model.

√td_X as a surface Mukai vector sees it: the realized codimension-one component and the integrated codimension-two component.

Equations
Instances For

    On a K3 the realized square root is 1 + [pt]. This is K3.sqrtToddComp_one and K3.degree_sqrtToddComp_two in the shape the Mukai vector consumes.

    On a K3 the Mukai vector is (rank, c₁, ∫ch₂ + rank).

    The third Mukai coordinate is the repository's K3.mukaiS, namely s = rank + ∫ch₂. This is what identifies the vector built here with the one GrothendieckGroup/MukaiVector.lean already uses.

    The same coordinate, as the integer s = χ − rank of K3.mukaiSInt, once Hirzebruch--Riemann--Roch is supplied.

    Bridgeland's K3 charge is the ordinary divisorial charge minus the rank. The two presentations differ by an additive term linear in the class, not by a scalar, so their walls differ.