Ambient deformations for exceptional sets in two-manifolds
Ambient deformations for exceptional sets in two-manifolds
复制标题
两个歧管中特殊组的环境变形
DOI:
10.1007/bf02139700
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发表时间:
1979
影响因子:
3.1
通讯作者:
Henry B. Laufer
中科院分区:
文献类型:
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作者:
Henry B. Laufer
Let M be a strictly pseudoconvex two-dimensional manifold with connected exceptional set A. Let o):,//~ Q be the versal deformation of M, where we ignore what happens near the boundary of M [27, Theorem 1, p. 217],[29]. Let re: M~ V be the blow-down of A in M, p= zr (A).~ z is then a resolution of the Stein normal two-dimensional space V. Let r:~"~ U be the versal deformation of (V, p). Let Mq=(n 1 (@ Let T be the reduced subspace of Q on which dimHl (Mq. 6) is constant. This is the maximal reduced subspace of Q over which oJ can be simultaneously blown-down [51, 39]. The induced map T--~ U is finite onto its image [3, 4]. Thus by studying T and the M, v we may obtain information about some of the singularities near to p.Specifically. Let Aq be the exceptional set in Mq. Let Aq. i be an irreducible component of A 0. Then (Proposition2. 3), Aq. i is homologous in,~/to a cycle Di> 0 on A with)~(D3=-89 i 9 D~+ D~. K)=< 1. There are only finitely many such Di. Conversely, let D> 0 be a cycle on A. Kodaira's theory for lifting submanifolds [18] may be modified so as to apply to D. Details in the analytic category are carried out in [30]. Wahl [53] has an independent treatment in the algebraic category. Let 3-be the sheaf of germs of infinitesimal deformations of D. Suppose that HI (D, j)---0. Then there are only first obstructions to lifting D. The above general results apply well to describe nearby exceptional sets Aq, qGr, in case the original singularity p is rational [2] or minimally elliptic [25] and the fundamental cycle Z is almost reduced (Definition3. 2), ie has coefficients of l except for non-singular rational A i with Ai. A~=-2. Examples of such singularities include the rational double points [2], the rational triple points [2], the quotient singularities [5], and the unimodal and bimodal singularities [1], Tables4. 1 and 4.2. For such singularities, the cycles D which are homologous to irreducible components Aq, i, q~ T, besides having z (D)=< 1, additionally satisfy D< Z (Lemma3. 1, Propositions4. 4 and 4.5), and have H~(D,, Y)= 0 (Proposition 3.3 and Proposition 4.6). We say (Definition 3.5) that a
DOI:
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发表时间:
2005
期刊:
影响因子:
--
作者:
T. Kobayashi;T. Oshima
通讯作者:
T. Oshima