Length of extremal rays and generalized adjunction
Length of extremal rays and generalized adjunction
复制标题
极值射线的长度和广义附加
DOI:
10.1007/bf01215656
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发表时间:
1989
影响因子:
0.8
通讯作者:
J. Wiśniewski
中科院分区:
文献类型:
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作者:
J. Wiśniewski
In this paper we apply Mori Theory to consider a generalization of adjunction. The linear system IKx+ HI" adjoint" to an ample divisor H on a surface X was originally investigated in modern terms by Sommese [Sol] and Van de Ven [VdV]. Most of the studies concerning adjunction were devoted to singular surfaces and threefolds. Recent generalization of adjunction ([Io],[So2],[Fu]) deals with polarized pairs (X, H), where X is a variety of dimension n and H is an ample divisor on X. A part of the problem is to give a classification of the pairs (X, H) for which the divisor Kx+ rH is not semi-ample (or: not ample), for" sufficiently large" r. In this paper we consider an ample and spanned vector bundle E of (" sufficiently large") rank r on a smooth variety X, and study when the adjoint divisor K x+ clE is not numerically effective. The answer we obtain is as follows: only these manifolds which admit a polarization H such that Kx+ rH is not semiample, can have E such that K x+ clE is not effective. Our main tool is Mori Theory.By Mori Theory we understand the results and techniques concerning the cone of curves on a manifold X whose canonical divisor K x is not numerically effective. Although the original purpose for considering the numerical properties of curves was the proof of Frankel-Hartshorne Conjecture,[Mol], and afterwards, the classification of 3-folds,[Mo2], the scope of Mori Theory seems to be much larger. In particular, as it was noticed by several authors (eg [L+ Pl,[Io]), Mori Theory seems to be very useful in investigating adjunction. In Section 1 we give an outline of Mori Theory and other related results. We introduce the notion of the length of an extremal ray,(1.9), which is used in the further arguments. In Section 2 we prove some results on manifolds having extremal rays of" sufficiently large" length,(2.4),(2.5). In particular, we consider the case of manifolds with ample second exterior power of the tangent bundle, A2TX,(2.8). We prove that in the dimension 3 these are only the projective space and the hyperquadric,(2.9).
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