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On the Negative K-theory of Singular Varieties

Posted on:2013-01-22Degree:Ph.DType:Dissertation
University:University of California, Los AngelesCandidate:Shih, JustinFull Text:PDF
GTID:1450390008487578Subject:Mathematics
Abstract/Summary:
Let X be an integral n-dimensional variety over a field k of characteristic zero, regular in codimension 1 and with singular locus Z. We establish a right exact sequence, coming from the Brown-Gersten spectral sequence, that computes K1-n(X) from KH1-n( X) and NK1-n( X). We then compute each of these pieces separately, and then analyze the map NK1-n( X) → K1-n( X).;We show that the KH1- n(X) contribution almost has a geometric structure. When k is algebraically closed, X is projective, and Z is either smooth over k or of codimension greater than 2, we prove that there is a 1-motive M = [ L → G] over k, and a map G(k) → KH1- n(X) whose kernel and cokernel are finitely generated. Thus the k-points G( k) of the group scheme G approximates KH 1-n(X) up to some finitely generated abelian groups. Furthermore, when n = 3, the sequence L(k) → G(k) → KH-2( X) is exact. In addition, M is computable, as under Deligne's equivalence between torsion-free 1-motives and torsion-free mixed Hodge structures of type {(0, 0), (0, 1), (1, 0), (1, 1)} such that GrW1H is polarizable, the free complex 1-motive (M x k C )fr is the 1-motive that corresponds to the unique largest such H coming from the weight 2 part W 2Hn(X C, Z ) of the nth cohomology group Hn(X C, Z ).;When X is not projective, the result still holds, except that the 1-motive M comes from W2 Hn(X C, Z ) where X is an algebraic compactification of X. Furthermore, the non-lattice parts of the M we get, and hence the map alpha, are independent of the choice of compactification.;For the NK1-n( X) contribution, when Z is an isolated singularity, we show that K1-n( X) is an extension of KH1- n(X) by the cdh-cohomology group Hn-1cdhU,O , where U is any open affine neighborhood of Z. Furthermore, Hn-1cdhU,O is a finite-dimensional k-vector space, whose dimension is the Du Bois invariant b0, n-1 of the isolated singularity Z..;All in all, we have a full computation of K-2 (X) when X is three-dimensional over an algebraically closed field and has only isolated singularities.
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