Kurs:Vector bundles, forcing algebras and local cohomology (Medellin 2012)/Lecture 3

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Geometric vector bundles

We have seen that the fibers of the spectrum of a forcing algebra are (empty or) affine spaces. However, this is not only fiberwise true, but more general: If we localize the forcing algebra at we get

since we can write

So over every the spectrum of the forcing algebra is an -dimensional affine space over the base. So locally, restricted to , we have isomorphisms

On the intersections we get two identifications with affine space, and the transition morphisms are linear if , but only affine-linear in general (because of the translation with ).

So the forcing algebra has locally the form and its spectrum has locally the form . This description holds on the union . Moreover, in the homogeneous case () the transition mappings are linear. Hence , where is the spectrum of a homogeneous forcing algebra, is a geometric vector bundle according to the following definition.



Definition  

Let denote a scheme. A scheme equipped with a morphism

is called a geometric vector bundle of rank over if there exists an open covering and -isomorphisms

such that for every open affine subset the transition mappings

are linear automorphisms, i.e. they are induced by an automorphism of the polynomial ring given by .

Here we can restrict always to affine open coverings. If is separated then the intersection of two affine open subschemes is again affine and then it is enough to check the condition on the intersections. The trivial bundle of rank is the -dimensional affine space over , and locally every vector bundle looks like this. Many properties of an affine space are enjoyed by general vector bundles. For example, in the affine space we have the natural addition

and this carries over to a vector bundle, that is, we have an addition

The reason for this is that the isomorphisms occurring in the definition of a geometric vector bundle are linear, hence the addition on coming from an isomorphism with some affine space over is independent of the choosen isomorphism. For the same reason there is a unique closed subscheme of called the zero-section which is locally defined to be . Also, multiplication by a scalar, i.e. the mapping

carries over to a scalar multiplication

In particular, for every point the fiber is an affine space over .

For a geometric vector bundle and an open subset one sets

so this is the set of sections in over . This gives in fact for every scheme over a set-valued sheaf. Because of the observations just mentioned, these sections can also be added and multiplied by elements in the structure sheaf, and so we get for every vector bundle a locally free sheaf, which is free on the open subsets where the vector bundle is trivial.


Definition  

A coherent -module on a scheme is called locally free of rank , if there exists an open covering and -module-isomorphisms for every .

Vector bundles and locally free sheaves are essentially the same objects.


Theorem

Let denote a scheme.

Then the category of locally free sheaves on and the category of geometric vector bundles on are equivalent.

A geometric vector bundle corresponds to the sheaf of its sections, and a locally free sheaf corresponds to the (relative) spectrum of the symmetric algebra of the dual module .

The free sheaf of rank corresponds to the affine space over .



Torsors of vector bundles

We have seen that

acts on the spectrum of a forcing algebra by addition. The restriction of to is a vector bundle, and restricted to becomes a -torsor.


Definition  

Let denote a geometric vector bundle over a scheme . A scheme together with an action

is called a geometric (Zariski)-torsor for (or a -principal fiber bundle or a principal homogeneous space) if there exists an open covering and isomorphisms

such that the diagrams (we set and )

commute, where is the addition on the vector bundle.

The torsors of vector bundles can be classified in the following way.


Proposition  

Let denote a noetherian separated scheme and let

denote a geometric vector bundle on with sheaf of sections .

Then there exists a correspondence between first cohomology classes and geometric -torsors.

Proof  

We describe only the correspondence. Let denote a -torsor. Then there exists by definition an open covering such that there exist isomorphisms

which are compatible with the action of on itself. The isomorphisms induce automorphisms

These automorphisms are compatible with the action of on itself, and this means that they are of the form

with suitable sections . This family defines a Čech cocycle for the covering and gives therefore a cohomology class in .
For the reverse direction, suppose that the cohomology class is represented by a Čech cocycle for an open covering . Set . We take the morphisms

given by to glue the together to a scheme over . This is possible since the cocycle condition guarantees the glueing condition for schemes.

The action of on itself glues also together to give an action on .


It follows immediately that for an affine scheme (i.e. a scheme of type ) there is no non-trivial torsor for any vector bundle. There will however be in general many non-trivial torsors on the punctured spectrum (and on a projective variety).


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