Overview
The Weyl algebra is not defined abstractly and then represented; it is defined as a ring of -linear operators on the polynomial ring , namely the subring of generated by the multiplication operators and the partial derivatives . The polynomial ring is therefore a left -module before anything is proved: it is the module the algebra was built to act on.
That makes the prototype for the whole theory, and it is worth extracting exactly what kind of module it is. Three facts settle almost everything. It is cyclic, generated by the constant polynomial . Its presentation is , because the annihilator of is precisely the left ideal generated by the partials. And it is simple in characteristic zero — every non-zero polynomial generates the whole module — which is proved on the simplicity page.
Two features are worth flagging at once because they are easy to get backwards. First, is a torsion module: every polynomial is killed by some non-zero operator (take enough derivatives). Second, it is nevertheless faithful: no non-zero operator kills all of , since sits inside by definition. Torsion is a statement about elements one at a time; faithfulness is a statement about the module as a whole, and here the two point in opposite directions.
Almost every other module in this collection is built from this one. The module is its Fourier transform; the twisted family is what "multiply by " looks like algebraically; and the module of holomorphic functions is the analytic enlargement in which sits as a very small submodule.
Definition
Throughout, is a field, taken of characteristic zero wherever simplicity is used, and abbreviates .
The polynomial moduleCoutinho, Ch. 5 §1
The polynomial module is equipped with the left -action determined on generators by
This is well defined without any verification: the operators on the right are exactly the generators of inside , so the action is the inclusion read as a module structure.
Written out on a general operator in canonical form, the action is
which is why the canonical form with all 's to the left of all 's is the convenient one: it displays the operator in the form in which it is applied.
Torsion element, torsion module
Let be a ring and a left -module. An element is a torsion element if its annihilator is a non-zero left ideal. If every element of is a torsion element, is a torsion module. Note that is always a torsion element, with annihilator .
A caution about the word "module"
appears in two different roles. As a subring of it is the commutative subalgebra generated by the multiplication operators. As a module it is the object defined above. The two are different structures on the same underlying set, and the module is not the ring acting on itself: is free of rank one over itself, while is not even projective (see Properties).
Core Concepts
Why a quotient and not a subobject
A cyclic module is always a quotient of the ring by a left ideal, and reading that way is what converts questions about polynomials into questions about ideals of . The generator is , and the relations satisfied by are exactly . Saying "the polynomial module is modulo the left ideal of the partials" is the algebraic form of the sentence "a polynomial is determined by its derivatives at the origin, and the constant function is the one all of whose derivatives vanish".
Differentiation lowers degree, and that is the whole story
Two elementary facts about acting on monomials drive everything on this page and the next. Applying to gives zero unless componentwise, and gives the constant when . Enough differentiation therefore destroys any given polynomial (torsion) but can also extract a non-zero constant from it (simplicity). Which of the two happens depends only on how many derivatives you take and in which directions.
Torsion versus faithful
It is tempting to read "torsion module" as "the module is annihilated by something". It is not. Over the annihilators are all non-zero, but their intersection over all is : that intersection is a two-sided ideal, and by simplicity of P4 the only two-sided ideals are and , while .
The size of the module
is infinite dimensional over , and it has to be: has no non-zero finite-dimensional representations in characteristic zero, because the trace of would have to be both and . So is, in a precise sense, as small as a faithful -module can be: with respect to the Bernstein filtration it has dimension and multiplicity , the minimum allowed by Bernstein's inequality.
Construction and Proof
There is really only one thing to prove, and it is the presentation (5.4). The proof rests entirely on the canonical basis theorem: the monomials form a -basis of .
Presentation of the polynomial moduleCoutinho (5.1.2)
is a cyclic left -module generated by , the annihilator of is the left ideal , and consequently as left -modules.
Proof
Consider the -linear map , . It is -linear because the action is associative: .
Surjectivity. For , the multiplication operator satisfies . So is onto and is cyclic.
. Each generator satisfies , so for any we get .
. Write in canonical form and group the terms by the -exponent:
If then for some , so and the term lies in . Hence with , and applying gives . If then and .
So , and the first isomorphism theorem for modules gives .
The decomposition
The proof shows more than the isomorphism. Every element of splits uniquely as a polynomial plus an element of : uniqueness holds because a polynomial lying in is annihilated by and equals its own image. So as -vector spaces, and the isomorphism is just "take the -free part of the canonical form". This makes membership in decidable by inspection, with no Gröbner basis computation required.
is a maximal left ideal
Because is simple in characteristic zero, has no proper non-zero submodules, so is a maximal left ideal of . It is emphatically not a two-sided ideal: the two-sided ideal generated by contains and is therefore all of .
Key Equations
With multi-index notation , and , the action on monomials is
The two extreme cases of (5.2) are the ones used repeatedly:
The annihilator of the generator and the resulting presentation are
A torsion certificate for an arbitrary non-zero polynomial, immediate from (5.3):
Finally, the companion module obtained by dividing by the instead of the :
Here is the -th standard basis vector and the term is read as zero when . On the roles are exchanged: the partials multiply and the variables differentiate, up to sign.
Variable Definitions
- the ground field; characteristic zero wherever simplicity or is invoked
- shorthand for the polynomial ring
- the -th Weyl algebra over , a subring of
- the operator "multiply by ", and also the -th variable of
- the operator on
- multi-indices in , with and
- the canonical basis monomials of , all variables written to the left of all partials
- the left ideal , equal to
- the left annihilator of an element of a left -module
- polynomials used to twist the action, giving the modules
Properties and Behaviour
Basic properties of as an -moduleCoutinho (5.1.1), (5.1.2)
- It is cyclic, generated by , with .
- It is faithful: .
- It is a torsion module: every satisfies for .
- In characteristic zero it is simple, so every non-zero generates it.
- It is infinite dimensional over , and as an -module it is neither free nor projective; over the subring it is of course free of rank one.
Why is not projective over
Take and the presentation . If were projective the sequence would split, exhibiting as a direct summand of the free module . But is a domain, so a free module over it has no non-zero torsion elements, while every element of is torsion. Hence no splitting exists. The same argument works for every .
The general torsion lemma behind (2) and (3)Coutinho (5.1.1)
Let be a ring and a simple left -module. Then (i) for every non-zero , and (ii) if is not a division ring, is a torsion module.
For (i), the map is -linear with image a non-zero submodule, hence all of ; its kernel is . For (ii), if some non-zero had then as left modules, so would have no left ideals other than and , which for a ring with identity forces to be a division ring.
