Localized Chern Class
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In algebraic geometry, a localized Chern class is a variant of a Chern class, that is defined for a chain complex of vector bundles as opposed to a single vector bundle. It was originally introduced in Fulton's ''intersection theory'', as an algebraic counterpart of the similar construction in
algebraic topology Algebraic topology is a branch of mathematics that uses tools from abstract algebra to study topological spaces. The basic goal is to find algebraic invariant (mathematics), invariants that classification theorem, classify topological spaces up t ...
. The notion is used in particular in the
Riemann–Roch-type theorem In algebraic geometry, there are various generalizations of the Riemann–Roch theorem; among the most famous is the Grothendieck–Riemann–Roch theorem, which is further generalized by the formulation due to Fulton et al. Formulation due to Bau ...
. S. Bloch later generalized the notion in the context of
arithmetic scheme In mathematics, Arakelov theory (or Arakelov geometry) is an approach to Diophantine geometry, named for Suren Arakelov. It is used to study Diophantine equations in higher dimensions. Background The main motivation behind Arakelov geometry is th ...
s (schemes over a Dedekind domain) for the purpose of giving #Bloch's conductor formula that computes the non-constancy of Euler characteristic of a degenerating family of algebraic varieties (in the mixed characteristic case).


Definitions

Let ''Y'' be a pure-dimensional regular scheme of finite type over a field or discrete valuation ring and ''X'' a closed subscheme. Let E_ denote a complex of vector bundles on ''Y'' :0 = E_ \to E_n \to \dots \to E_m \to E_ = 0 that is exact on Y - X. The localized Chern class of this complex is a class in the
bivariant Chow group In mathematics, a bivariant theory was introduced by Fulton and MacPherson , in order to put a ring structure on the Chow group of a singular variety, the resulting ring called an operational Chow ring. On technical levels, a bivariant theory is a ...
of X \subset Y defined as follows. Let \xi_i denote the tautological bundle of the
Grassmann bundle Hermann Günther Grassmann (german: link=no, Graßmann, ; 15 April 1809 – 26 September 1877) was a German polymath known in his day as a linguist and now also as a mathematician. He was also a physicist, general scholar, and publisher. His mat ...
G_i of rank \operatorname E_i sub-bundles of E_i \otimes E_. Let \xi = \prod (-1)^i \operatorname_i^*(\xi_i). Then the ''i''-th localized Chern class c_^Y(E_) is defined by the formula: :c_^Y(E_) \cap \alpha = \eta_*(c_i(\xi) \cap \gamma) where \eta: G_n \times_Y \dots \times_Y G_m \to X is the projection and \gamma is a cycle obtained from \alpha by the so-called
graph construction Graph may refer to: Mathematics *Graph (discrete mathematics), a structure made of vertices and edges **Graph theory, the study of such graphs and their properties *Graph (topology), a topological space resembling a graph in the sense of discre ...
.


Example: localized Euler class

Let f: X \to S be as in #Definitions. If ''S'' is smooth over a field, then the localized Chern class coincides with the class :(-1)^ \mathbf(s_f) where, roughly, s_f is the section determined by the differential of ''f'' and (thus) \mathbf(s_f) is the class of the singular locus of ''f''. Consider an infinite dimensional bundle E over an infinite dimensional manifold M with a section s with Fredholm derivative. In practice this situation occurs whenever we have system of PDE’s which are elliptic when considered modulo some gauge group action. The zero set Z(s) is then the moduli space of solutions modulo gauge, and the index of the derivative is the virtual dimension. The localized Euler class of the pair (E,s) is a homology class with closed support on the zero set of the section. Its dimension is the index of the derivative. When the section is transversal, the class is just the fundamental class of the zero set with the proper orientation. The class is well behaved in one parameter families and therefore defines the “right” fundamental cycle even if the section is no longer transversal.


Bloch's conductor formula

This formula enables us to compute the conductor that measures the wild ramification by using the sheaf of differential 1-forms. S. Bloch conjectures a formula for the Artin conductor of the ℓ-adic etale cohomology of a regular model of a variety over a local field and proves it for a curve. The deepest result about the Bloch conductor is its equality with the Artin conductor, defined in terms of the l-adic cohomology of X, in certain cases.


References

*S. Bloch, “Cycles on arithmetic schemes and Euler characteristics of curves,” Algebraic geometry, Bowdoin, 1985, 421–450, Proc. Symp. Pure Math. 46, Part 2, Amer. Math. Soc., Providence, RI, 1987. *, section B.7 *K. Kato and T. Saito, “On the conductor formula of Bloch,” Publ. Math. IHES 100 (2005), 5-151. {{algebraic-geometry-stub Algebraic geometry