Kurs:Vektorbündel und Abschlussoperationen (MSRI 2012)/Abschnitt 1
- Systems of linear equations
We start with some linear algebra. Let be a field. We consider a system of linear homogeneous equations over ,
where the are elements in . The solution set to this system of homogeneous equations is a vector space over (a subvector space of ), its dimension is , where
is the matrix given by these elements. Additional elements give rise to the system of inhomogeneous linear equations,
The solution set of this inhomogeneous system may be empty, but nevertheless it is tightly related to the solution space of the homogeneous system. First of all, there exists an action
because the sum of a solution of the homogeneous system and a solution of the inhomogeneous system is again a solution of the inhomogeneous system. This action is a group action of the group on the set . Moreover, if we fix one solution
(supposing that at least one solution exists), then there exists a bijection
This means that the group acts simply transitive on , and so can be identified with the vector space , however not in a canonical way.
Suppose now that is a geometric object (a topological space, a manifold, a variety, a scheme, the spectrum of a ring) and that instead of elements in the field we have functions
on (which are continuous, or differentiable, or algebraic). We form the matrix of functions , which yields for every point a matrix over . Then we get from these data the space
together with the projection to . For a fixed point , the fiber of over is the solution space to the corresponding system of homogeneous linear equations given by inserting into . In particular, all fibers of the map
are vector spaces (maybe of non-constant dimension). These vector space structures yield an addition[1]
(only points in the same fiber can be added). The mapping
is called the zero-section .
Suppose now that additional functions
are given. Then we can form the set
with the projection to . Again, every fiber of over a point is the solution set to the system of inhomogeneous linear equations which arises by inserting into and . The actions of the fibers on (coming from linear algebra) extend to an action
Also, if a (continuous, differentiable, algebraic) map
with exists, then we can construct a (continuous, differentiable, algebraic) isomorphism between and . However, different from the situation in linear algebra (which corresponds to the situation where is just one point), such a section does rarely exist.
These objects have new and sometimes difficult global properties which we try to understand in these lectures. We will work mainly in an algebraic setting and restrict to the situation where just one equation
is given. Then in the homogeneous case () the fibers are vector spaces of dimension or , and the later holds exactly for the points where . In the inhomogeneous case the fibers are either empty or of dimension or . We give some typical examples.
We consider the line (or etc.) with the (identical) function . For and , i.e. for the homogeneous equation , the geometric object consists of a horizontal line (corresponding to the zero-solution) and a vertical line over . So all fibers except one are zero-dimensional vector spaces. For the inhomogeneous equation , is a hyperbola, and all fibers are zero-dimensional with the exception that the fiber over is empty.
For the homogeneous equation , is just the affine cylinder over the base line. For the inhomogeneous equation , consists of one vertical line, almost all fibers are empty.
Let denote a plane (like ) with coordinate functions and . We consider an inhomogeneous linear equation of type
The fiber of the solution set over a point is one-dimensional, whereas the fiber over has dimension two (for ). Many properties of depend on these four exponents.
In (most of) these example we can observe the following behavior. On an open subset, the dimension of the fibers is constant and equals , whereas the fiber over some special points degenerates to an -dimensional solution set (or becomes empty).
- Forcing algebras
We describe now the algebraic setting of systems of linear equations depending on a base space. For a commutative ring , its spectrum is a topological space on which the ring elements can be considered as functions. The value of at a prime ideal is just the image of under the ring homomorphism . In this interpretation, a ring element is a function with values in different fields. Suppose that contains a field . Then an element gives rise to the ring homomorphism
which gives rise to a scheme morphism
This is another way to consider as a function on with values in the affine line.
The following construction appeared first in the work of Hochster in the context of solid closure.
Let be a commutative ring and let and be elements in . Then the -algebra
is called the forcing algebra of these elements (or these data).
The forcing algebra forces to lie inside the extended ideal (hence the name). For every -algebra such that there exists a (non unique) ring homomorphism by sending to the coefficient in an expression .
The forcing algebra induces the spectrum morphism
Over a point , the fiber of this morphism is given by
and we can write
where means the evaluation of the in the residue class field. Hence the -points in the fiber are exactly the solutions to the inhomogeneous linear equation . In particular, all the fibers are (empty or) affine spaces.
- Forcing algebras and closure operations
Let denote a commutative ring and let be an ideal. Let and let
be the corresponding forcing algebra and
the corresponding spectrum morphism. How are properties of (or of the -algebra ) related to certain ideal closure operations?
We start with some examples. The element belongs to the ideal if and only if we can write with . By the universal property of the forcing algebra this means that there exists an -algebra-homomorphism
hence holds if and only if admits a scheme section. This is also equivalent to
admitting an -module section or being a pure -algebra (so for forcing algebras properties might be equivalent which are not equivalent for arbitrary algebras).
The radical of an ideal
Now we look at the radical of the ideal ,
The importance of the radical comes mainly from Hilbert's Nullstellensatz, saying that for algebras of finite type over an algebraically closed field there is a natural bijection between radical ideals and closed algebraic zero-sets. So geometrically one can see from an ideal only its radical. As this is quite a coarse closure operation we should expect that this corresponds to a quite coarse property of the morphism as well. Indeed, it is true that if and only if is surjective. This is true since the radical of an ideal is the intersection of all prime ideals in which it is contained. Hence an element belongs to the radical if and only if for all residue class homomorphisms
where is sent to , also is sent to . But this means for the forcing equation that whenever the equation degenerates to , then also the inhomogeneous part becomes zero, and so there will always be a solution to the inhomogeneous equation.
Exercise: Define the radical of a submodule inside a module.
Integral closure of an ideal
Another closure operation is integral closure . It is defined by
This notion is important for describing the normalization of the blow up of the ideal . Another characterization (assume that is noetherian) is that there exists a , not contained in any minimal prime ideal of , such that holds for all . Another equivalent property - the valuative criterion - is that for all ring homomorphisms
to a discrete valuation domain the containment holds.
The characterization of the integral closure in terms of forcing algebras requires some notions from topology. A continuous map
between topological spaces and is called a submersion , if it is surjective and if carries the image topology (quotient topology) under this map. This means that a subset is open if and only if its preimage is open. Since the spectrum of a ring endowed with the Zarisiki topology is a topological space, this notion can be applied to the spectrum morphism of a ring homomorphism. With this notion we can state that if and only if the forcing morphism
is a universal submersion (universal means here that for any ring change to a noetherian ring , the resulting homomorphism still has this property). The relation between these two notions stems from the fact that also for universal submersions there exists a criterion in terms of discrete valuation domains: A morphism of finite type between two affine noetherian schemes is a universal submersion if and only if the base change to any discrete valuation domain yields a submersion. For a morphism
( a discrete valuation domain) to be a submersion means that above the only chain of prime ideals in , namely , there exists a chain of prime ideals in lying over this chain. This pair-lifting property holds for a universal submersion
for any pair of prime ideals in . This property is stronger than lying over (which means surjective) but weaker than the going-down or the going-up property (in the presence of surjectivity).
If we are dealing only with algebras of finite type over the complex numbers , then we may also consider the corresponding complex spaces with their natural topology induced from the euclidean topology of . Then universal submersive with respect to the Zariski topology is the same as submersive in the complex topology (the target space needs to be normal).
Let be a field and consider . Since this is a principal ideal domain, the only interesting forcing algebras (if we are only interested in the local behavior around ) are of the form . For this -algebra admits a section (corresponding to the fact that ), and if there exists an affine line over the maximal ideal . So now assume . If then we have a hyperbola mapping to an affine line, with the fiber over being empty, corresponding to the fact that does not belong to the radical of for . So assume finally . Then belongs to the radical of , but not to its integral closure (which is the identical closure on a one-dimensional regular ring). We can write the forcing equation as . So the spectrum of the forcing algebra consists of a (thickend) line over and of a hyperbola. The forcing morphism is surjective, but it is not a submersion. For example, the preimage of is a connected component hence open, but this single point is not open.
Let be a field and let be the polynomial ring in two variables. We consider the ideal and the element . This element belongs to the radical of this ideal, hence the forcing morphism
is surjective. We claim that it is not a submersion. For this we look at the reduction modulo . In the ideal becomes which does not contain . Hence by the valuative criterion for integral closure, does not belong to the integral closure of the ideal. One can also say that the chain in the affine plane does not have a lift (as a chain) to the spectrum of the forcing algebra.
For the ideal
and the element the situation looks different. Let
be a ring homomorphism to a discrete valuation domain . If or is mapped to , then also is mapped to and hence belongs to the extended ideal. So assume that and , where is a local parameter of and and are units. Then and the exponent is at least the minimum of and , hence
So belongs to the integral closure of and the forcing morphism
is a universal submersion.
Continuous closure
Suppose now that . Then every polynomial can be considered as a continuous function
in the complex topology. If is an ideal and is an element, we say that belongs to the continuous closure of , if there exist continuous functions
such that
(as an identity of functions). The same definition works for -algebras of finite type.
It is not at all clear at once that there may exist polynomials but inside the continuous closure of . For it is easy to show that the continuous closure is (like the integral closure) just the ideal itself. We also remark that when we would only allow holomorphic functions then we could not get something larger. However, with continuous functions
we can for example write
Continuous closure is always inside the integral closure and hence also inside the radical. The element does not belong to the continuous closure of , though it belongs to the integral closure of . In terms of forcing algebras, an element belongs to the continuous closure if and only if the complex forcing mapping
(between the corresponding complex spaces) admits a continuous section.
- ↑ is the fiber product of with itself.