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in the sense of ]. There are other criteria such as the Kleiman condition and Seshadri condition, to characterise the '''ample cone'''. in the sense of ]. There are other criteria such as the Kleiman condition and Seshadri condition, to characterise the '''ample cone'''.

Also, Laura is ample.


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Revision as of 03:35, 27 October 2006

In mathematics, in algebraic geometry or the theory of complex manifolds, a very ample line bundle L {\displaystyle L} is one with enough sections to set up an embedding of its base variety or manifold M {\displaystyle M} into projective space. That is, considering that for any two sections s {\displaystyle s} and t {\displaystyle t} , the ratio

s t {\displaystyle {s} \over {t}}

makes sense as a well-defined numerical function on M {\displaystyle M} , one can take a basis for all global sections of L {\displaystyle L} on M {\displaystyle M} and try to use them as a set of homogeneous coordinates on M {\displaystyle M} . If the basis is written out as

s 1 ,   s 2 ,   . . . ,   s k {\displaystyle s_{1},\ s_{2},\ ...,\ s_{k}}

where k {\displaystyle k} is the dimension of the space of sections, it makes sense to regard

[ s 1 :   s 2 :   . . . :   s k ] {\displaystyle }

as coordinates on M {\displaystyle M} , in the projective space sense. Therefore this sets up a mapping

M     P k 1 {\displaystyle M\ \rightarrow \ P^{k-1}}

which is required to be an embedding. (In a more invariant treatment, the RHS here is described as the projective space underlying the space of all global sections.)

An ample line bundle L {\displaystyle L} is one which becomes very ample after it is raised to some tensor power, i.e. the tensor product of L {\displaystyle L} with itself enough times has enough sections. These definitions make sense for the underlying divisors (Cartier divisors) D {\displaystyle D} ; an ample D {\displaystyle D} is one for which n D {\displaystyle nD} moves in a large enough linear system. Such divisors form a cone in all divisors, of those which are in some sense positive enough. The relationship with projective space is that the D {\displaystyle D} for a very ample L {\displaystyle L} will correspond to the hyperplane sections (intersection with some hyperplane) of the embedded M {\displaystyle M} .

There is a more general theory of ample vector bundles.

Criteria for ampleness

To decide in practice when a Cartier divisor D corresponds to an ample line bundle, there are some geometric criteria.

For example. for a smooth algebraic surface S, the Nakai-Moishezon criterion states that D is ample if its self-intersection number is strictly positive, and for any irreducible curve C on S we have

D.C > 0

in the sense of intersection theory. There are other criteria such as the Kleiman condition and Seshadri condition, to characterise the ample cone.

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