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The Polynomial Ring as a Module over the Weyl Algebra

The Weyl algebra An was built as a ring of operators on K[X]=K[x1,…,xn], so the polynomial ring is a left An-module by construction. This page pins down that module: its presentation An/∑iAn∂i, its cyclicity, and why every element of it is a torsion element even though the module is faithful.

Collection Algebraic D-modulesTopic stream weyl-modulesSource Ch. 5 §1Reading time 28 minPage ID KVS-ENG-MATH-0350

Overview

The Weyl algebra An=An(K) is not defined abstractly and then represented; it is defined as a ring of K-linear operators on the polynomial ring K[X]=K[x1,…,xn], namely the subring of EndK(K[X]) generated by the multiplication operators x1,…,xn and the partial derivatives ∂1,…,∂n. The polynomial ring is therefore a left An-module before anything is proved: it is the module the algebra was built to act on.

That makes K[X] 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 1. Its presentation is K[X]≅An/∑i=1nAn∂i, because the annihilator of 1 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, K[X] 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 K[X], since An sits inside EndK(K[X]) 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 K[∂]≅An/∑iAnxi is its Fourier transform; the twisted family An/∑iAn(∂i−gi) is what "multiply by exp∫g" looks like algebraically; and the module of holomorphic functions is the analytic enlargement in which K[X] sits as a very small submodule.

Definition

Throughout, K is a field, taken of characteristic zero wherever simplicity is used, and K[X] abbreviates K[x1,…,xn].

The polynomial moduleCoutinho, Ch. 5 §1

The polynomial module is K[X] equipped with the left An-action determined on generators by

xi⋅f=xif,∂i⋅f=∂f∂xi(1≤i≤n,f∈K[X]).

This is well defined without any verification: the operators on the right are exactly the generators of An inside EndK(K[X]), so the action is the inclusion An↪EndK(K[X]) read as a module structure.

Written out on a general operator in canonical form, the action is

(∑α,βcαβxα∂β)⋅f=∑α,βcαβxα∂|β|f∂xβ,
(5.1)

which is why the canonical form with all x'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 R be a ring and M a left R-module. An element u∈M is a torsion element if its annihilator annR(u)={a∈R:au=0} is a non-zero left ideal. If every element of M is a torsion element, M is a torsion module. Note that u=0 is always a torsion element, with annihilator R.

A caution about the word "module"

K[X] appears in two different roles. As a subring of An 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: An is free of rank one over itself, while K[X] 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 K[X] that way is what converts questions about polynomials into questions about ideals of An. The generator is 1, and the relations satisfied by 1 are exactly ∂i⋅1=0. Saying "the polynomial module is An 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 ∂β acting on monomials drive everything on this page and the next. Applying ∂β to xα gives zero unless β≤α componentwise, and gives the constant α! when β=α. 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 An the annihilators ann(f) are all non-zero, but their intersection over all f∈K[X] is 0: that intersection is a two-sided ideal, and by simplicity of P4 the only two-sided ideals are 0 and An, while 1⋅1=1≠0.

The size of the module

K[X] is infinite dimensional over K, and it has to be: An has no non-zero finite-dimensional representations in characteristic zero, because the trace of [∂i,xi]=1 would have to be both 0 and dim. So K[X] is, in a precise sense, as small as a faithful An-module can be: with respect to the Bernstein filtration it has dimension d(K[X])=n and multiplicity e(K[X])=1, 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 xα∂β form a K-basis of An.

Presentation of the polynomial moduleCoutinho (5.1.2)

K[X] is a cyclic left An-module generated by 1, the annihilator of 1 is the left ideal J=∑i=1nAn∂i, and consequently K[X]≅An/J as left An-modules.

Proof

Consider the An-linear map φ:An→K[X], φ(P)=P⋅1. It is An-linear because the action is associative: φ(QP)=(QP)⋅1=Q⋅φ(P).

Surjectivity. For f∈K[X], the multiplication operator f∈An satisfies φ(f)=f⋅1=f. So φ is onto and K[X]=An⋅1 is cyclic.

J⊆kerφ. Each generator satisfies ∂i⋅1=0, so for any Qi∈An we get (∑iQi∂i)⋅1=∑iQi⋅0=0.

kerφ⊆J. Write P in canonical form and group the terms by the ∂-exponent:

P=∑βfβ(x)∂β=f0(x)+∑β≠0fβ(x)∂β.

If β≠0 then βi≥1 for some i, so ∂β=∂β−ei∂i and the term fβ∂β lies in An∂i⊆J. Hence P=f0+Q with Q∈J, and applying φ gives φ(P)=f0. If P∈kerφ then f0=0 and P=Q∈J.

So kerφ=J, and the first isomorphism theorem for modules gives An/J≅K[X].

The decomposition An=K[X]⊕J

The proof shows more than the isomorphism. Every element of An splits uniquely as a polynomial plus an element of J: uniqueness holds because a polynomial lying in J is annihilated by φ and equals its own image. So An=K[X]⊕J as K-vector spaces, and the isomorphism An/J→K[X] is just "take the ∂-free part of the canonical form". This makes membership in J decidable by inspection, with no Gröbner basis computation required.

J is a maximal left ideal

Because K[X] is simple in characteristic zero, An/J has no proper non-zero submodules, so J is a maximal left ideal of An. It is emphatically not a two-sided ideal: the two-sided ideal generated by ∂1,…,∂n contains [∂1,x1]=1 and is therefore all of An.

Key Equations

With multi-index notation α=(α1,…,αn)∈ℕn, xα=x1α1⋯xnαn and α!=α1!⋯αn!, the action on monomials is

∂β⋅xα={α!(α−β)!xα−βifβ≤αcomponentwise,0otherwise.
(5.2)

The two extreme cases of (5.2) are the ones used repeatedly:

∂α⋅xα=α!∈K×(charK=0),∂β⋅xα=0whenever|β|>|α|.
(5.3)

The annihilator of the generator and the resulting presentation are

annAn(1)=∑i=1nAn∂i,K[X]≅An/∑i=1nAn∂i.
(5.4)

A torsion certificate for an arbitrary non-zero polynomial, immediate from (5.3):

∂iN⋅f=0foreveryiandeveryN>degf,soannAn(f)≠0.
(5.5)

Finally, the companion module obtained by dividing by the xi instead of the ∂i:

An/∑i=1nAnxi≅K[∂]=K[∂1,…,∂n],xi⋅∂β=−βi∂β−ei.
(5.6)

Here ei is the i-th standard basis vector and the term is read as zero when βi=0. On K[∂] the roles are exchanged: the partials multiply and the variables differentiate, up to sign.

Variable Definitions

K
the ground field; characteristic zero wherever simplicity or α!≠0 is invoked
K[X]
shorthand for the polynomial ring K[x1,…,xn]
An
the n-th Weyl algebra over K, a subring of EndK(K[X])
xi
the operator "multiply by xi", and also the i-th variable of K[X]
∂i
the operator ∂/∂xi on K[X]
α,β
multi-indices in ℕn, with |α|=α1+…+αn and α!=α1!⋯αn!
xα∂β
the canonical basis monomials of An, all variables written to the left of all partials
J
the left ideal ∑i=1nAn∂i, equal to annAn(1)
annR(u)
the left annihilator {a∈R:au=0} of an element u of a left R-module
gi
polynomials used to twist the action, giving the modules An/∑iAn(∂i−gi)

Properties and Behaviour

Basic properties of K[X] as an An-moduleCoutinho (5.1.1), (5.1.2)

  1. It is cyclic, generated by 1, with annAn(1)=∑iAn∂i.
  2. It is faithful: annAn(K[X])=0.
  3. It is a torsion module: every f satisfies ∂1N⋅f=0 for N>degf.
  4. In characteristic zero it is simple, so every non-zero f generates it.
  5. It is infinite dimensional over K, and as an An-module it is neither free nor projective; over the subring K[X]⊂An it is of course free of rank one.

Why K[X] is not projective over An

Take n=1 and the presentation 0→A1∂→A1→K[x]→0. If K[x] were projective the sequence would split, exhibiting K[x] as a direct summand of the free module A1. But A1 is a domain, so a free module over it has no non-zero torsion elements, while every element of K[x] is torsion. Hence no splitting exists. The same argument works for every n.

The general torsion lemma behind (2) and (3)Coutinho (5.1.1)

Let R be a ring and M a simple left R-module. Then (i) M≅R/annR(u) for every non-zero u∈M, and (ii) if R is not a division ring, M is a torsion module.

For (i), the map r↦ru is R-linear with image a non-zero submodule, hence all of M; its kernel is annR(u). For (ii), if some non-zero u had annR(u)=0 then M≅R as left modules, so R would have no left ideals other than 0 and R, which for a ring with identity forces R to be a division ring.

Dimension and multiplicity

Filtering K[X] by the good filtration Γm=Bm⋅1 induced by the generator gives Γm={f:degf≤m}, of dimension (m+nn). Hence P4 =n and P6 =1: the polynomial module is holonomic, and of the smallest possible multiplicity.

Examples and Special Cases

n=1: the module K[x]

K[x]≅A1/A1∂. The generator is 1; the element xk generates too, since ∂kxk=k!. A K-basis is 1,x,x2,…, on which ∂ shifts down with a coefficient and x shifts up. This is the algebraic skeleton of the raising and lowering operator picture.

The companion module K[∂]

Dividing by the other half of the generators gives An/∑iAnxi, which as a K-vector space has basis the classes of ∂β, so it may be identified with the polynomial ring K[∂1,…,∂n]. Here the ∂i act by multiplication. To see how xi acts, commute it past ∂β using [xi,∂ik]=−k∂ik−1: modulo ∑jAnxj the term ∂βxi dies and one is left with xi⋅∂β=−βi∂β−ei. So xi acts as −∂/∂ξi in the symbol variables. This module is the Fourier transform of K[X].

Twisting the derivative actionCoutinho, Ch. 5 §1 and §2

Fix g1,…,gn∈K[X] and let Jg=∑iAn(∂i−gi). Every element of An can still be written as f+Q with f∈K[X] and Q∈Jg, so An/Jg≅K[X] as K-vector spaces, by the same "∂-free part" recipe. The xi-action agrees with the usual one, but the derivative action does not:

∂i⋅(f+Jg)=(∂f∂xi+gif)+Jg.

Analytically this is differentiation conjugated by exp(∫g), which is exactly why the gi cannot be arbitrary if one wants an automorphism of An behind the change: the integrability condition ∂gj/∂xi=∂gi/∂xj is needed. Taking each gi∈K[xi] is the easy way to satisfy it.

A module that is cyclic but not simple

For non-constant f∈K[X] the localisation K[X][1/f] is again a left An-module, by the quotient rule, and it is finitely generated. It is not simple: it contains K[X] as a proper non-zero submodule. It is nevertheless still holonomic, which shows how much weaker holonomicity is than simplicity.

Characteristic p breaks simplicity, not the module

The action and the presentation (5.4) hold over any field, since the canonical basis theorem does. Simplicity does not. Over K of characteristic p, the subspace x1pK[X] is an An-submodule, because ∂1(x1ph)=px1p−1h+x1p∂1h=x1p∂1h. It is proper and non-zero, so K[X] is not simple. This is the module-level shadow of the failure of simplicity of P6 itself in characteristic p.

Worked Example

Everything at once, for n=2 and f=x12x2+3x1

  1. Step 1 - the derivative table

    Work in K[x1,x2] over ℚ, with f=x12x2+3x1 of total degree 3. Differentiating directly:

    Operator DD⋅f
    ∂12x1x2+3
    ∂2x12
    ∂122x2
    ∂1∂22x1
    ∂220
    ∂130
    ∂12∂22

    Each entry is a one-line check. For instance ∂12∂2f: first ∂2f=x12 (the term 3x1 has no x2), then ∂12x12=2.

  2. Step 2 - f is a torsion element

    The table already exhibits two non-zero operators killing f, namely ∂13 and ∂22, in line with (5.5). A less obvious one comes from comparing two entries: x2⋅(∂1∂2f)=2x1x2 and x1⋅(∂12f)=2x1x2, so

    (x2∂1∂2−x1∂12)⋅f=2x1x2−2x1x2=0.

    So annA2(f) is a large left ideal, not just the obvious high-order derivatives.

  3. Step 3 - f generates the whole module

    The monomial of maximal degree in f is x12x2, with α=(2,1) and coefficient 1. By (5.3), ∂αxα=α!=2!⋅1!=2, while ∂α kills every other monomial of f (here 3x1, which ∂2 already destroys). So ∂12∂2⋅f=2, confirming the last row of the table, and

    D⋅f=1withD=12∂12∂2∈A2.

    Since 1 generates K[x1,x2], we get A2f∋1 and therefore A2f=K[x1,x2]. Note where characteristic zero entered: we divided by α!=2.

  4. Step 4 - reading off a maximal left ideal

    Because f generates, K[x1,x2]≅A2/annA2(f) and that annihilator is maximal. One element of it is forced by Step 3: from Df=1 we get f(Df)=f, hence

    (fD−1)⋅f=f⋅1−f=0,fD−1=12(x12x2+3x1)∂12∂2−1.

    This operator is non-zero (its canonical form has the basis monomial 12x12x2∂12∂2 with non-zero coefficient) and it has order 3, so it is genuinely different from the operators found in Step 2.

  5. Step 5 - the presentation in action

    Take P=x1∂22+x2∂1+x1x2∈A2. Its ∂-free part is f0=x1x2, and indeed P⋅1=0+0+x1x2. Splitting as in the construction, P=x1x2+Q with Q=(x1∂2)∂2+x2∂1∈J=A2∂1+A2∂2. So the class of P in A2/J corresponds to the polynomial x1x2, exactly as (5.4) predicts, and no computation harder than reading the canonical form was needed.

Result

For f=x12x2+3x1: 12∂12∂2⋅f=1, so A2f=K[x1,x2] and f generates; simultaneously ∂13,∂22,x2∂1∂2−x1∂12 and 12f∂12∂2−1 all annihilate f, so f is a torsion element. A single polynomial is thus both a generator of the whole module and a torsion element - the combination that characterises a simple torsion module over a non-division ring.

Applications and Industry Use

In a mathematics topic, this section covers downstream use inside mathematics, computing and engineering rather than a manufactured product.

The polynomial module is the coefficient object against which most concrete D-module computations are run.

  • Polynomial solutions of a system. If P1,…,Pr∈An and M=An/∑jAnPj is the module of the system, then HomAn(M,K[X]) is canonically the space of polynomial solutions {f:Pjf=0∀j}, because a homomorphism is determined by the image of the generator and the relations become the equations. This is the identity that turns solving into a Hom computation; see solutions as homomorphisms.
  • Holonomic rank and D-finiteness. Replacing K[X] by larger solution modules - rational functions, formal power series, holomorphic functions - keeps the same formalism and changes only how many solutions are found. K[X] is the smallest useful choice and detects exactly the polynomial solutions.
  • Symbolic summation and integration. The closure properties used by Zeilberger's algorithm are proved for modules built from K[X] by localisation and twisting, so the properties of this module propagate directly into the algorithms.
  • Quantum mechanics. The action here is the polynomial-algebraic form of the Schrödinger representation, with position acting by multiplication and momentum by differentiation; see the quantum origins page. The absence of finite-dimensional representations is the algebraic content of the fact that position and momentum cannot both be bounded operators.

Design Considerations

For a mathematical object, design considerations are the modelling choices: which ring, which filtration, which category to work in.

Which side the module acts on

K[X] is naturally a left module because operators compose on the left of the function they act on. The presentation (5.4) uses left ideals throughout, and ∑iAn∂i is not the same set as ∑i∂iAn. When a construction later needs a right module - for instance in direct images - the correct move is to apply the transposition anti-automorphism or a side-changing functor, not to reinterpret the same ideal on the other side.

Which presentation to carry

The same module has many presentations, and they are not equally useful. An/∑iAn∂i makes the constant 1 the generator and makes membership in the ideal decidable by inspection. Taking a different generator, say xγ, produces a much more complicated annihilator that encodes the same module. As a rule, present a cyclic module by a generator whose annihilator you can describe, not by whichever generator appears first.

Polynomials or symbols

K[X] and K[∂] are exchanged by the Fourier automorphism but are not isomorphic as An-modules: in one the generator is killed by all the ∂i, in the other by all the xi. Choosing between them is choosing which half of the generators you want to act by multiplication, and constant-coefficient problems are usually easier on K[∂].

Computational Notes

Read this as the manufacturing section of the template: how the object is actually built by machine, at what cost, and where the computation stops being decidable.

Three tasks come up constantly, and only one of them is expensive.

  1. Apply an operator to a polynomial. Put the operator in canonical form and use (5.1) term by term. Cost is linear in the number of terms of the operator times the cost of differentiating a polynomial.
  2. Decide membership in J=∑iAn∂i. Free: put the operator in canonical form and check whether the ∂-free part is zero. No Gröbner basis is needed, because {xα∂β:β≠0} is already a basis of J.
  3. Compute annAn(f) for a given polynomial f. This is the expensive one. It is a syzygy computation in the Weyl algebra and needs a non-commutative Gröbner basis with respect to a term order refining the chosen filtration. The answer is always a maximal left ideal in characteristic zero, but writing generators for it is not cheap.

Every general-purpose D-module package represents this module the same way, as the cyclic module presented by the ideal of the partials, and reports d=n, e=1, holonomic rank 1. Implementations include the Dmodules package in Macaulay2, dmod.lib in Singular, and the ore_algebra package in SageMath. A useful correctness check on any of them: the reported holonomic rank of An/∑iAn∂i must be 1, since the only solutions of ∂if=0 for all i are the constants.

Failure Modes and Common Mistakes

Writing "the ideal generated by ∂1,…,∂n" without saying which kind

The left ideal ∑iAn∂i is proper and maximal. The two-sided ideal generated by the same elements is all of An, since it contains ∂1x1−x1∂1=1. So the phrase "An modulo the ideal generated by the partials" is either the polynomial module or the zero module depending on a word that is often left out. Always write the left ideal explicitly.

Treating K[X] as a subring of An when a module is meant

As a subring, K[X]⊂An is closed under multiplication and contains no information about differentiation. As a module, K[X] is a quotient of An on which the partials act non-trivially. Statements such as "K[X] is a free An-module of rank one" arise from conflating them and are false: the generator 1 has non-zero annihilator, and K[X] is not even projective.

Assuming the annihilator of a polynomial is generated by high-order derivatives

For f of degree d the operators ∂β with |β|>d certainly annihilate f, but the left ideal I they generate is not the annihilator. I kills every polynomial of degree at most d at once, so it sits inside the two distinct maximal left ideals ann(1) and ann(f) - distinct because ∂1 lies in the first and not the second when f has a linear term. A left ideal contained in two different maximal left ideals is not itself maximal. A genuine annihilator always contains operators mixing x's and ∂'s, as Steps 2 and 4 of the worked example show.

Applying an operator without first putting it in canonical form

∂1x1 and x1∂1 are different operators: on f=1 the first gives 1 and the second gives 0. Formula (5.1) is valid only once all variables are to the left of all partials. Reordering must be done with [∂i,xj]=δij, never by treating the symbols as commuting.

Historical Notes

The action of multiplication and differentiation on polynomials is far older than D-module theory; it is what Heisenberg's commutation relation [∂,x]=1 describes, and Hermann Weyl's 1928 analysis of the canonical commutation relations is why the algebra carries his name. The observation that no finite-dimensional space can carry such an action - the trace argument - is essentially contemporary with the relation itself, and it is the first indication that the polynomial module, or something at least as large, is unavoidable.

The algebraic reading of the polynomial ring as a cyclic module with a specified annihilator belongs to the ring-theoretic study of An that began in earnest with Dixmier's 1968 paper on A1. Classification results for A1-modules were obtained by Block around 1980; the general problem of classifying simple An-modules remains open, which is one reason the explicit families built from K[X] by twisting retain their interest. In the D-module tradition proper, the polynomial module is the structure sheaf of affine space read algebraically, and Bernstein's 1971-72 work made it the base case from which the localisations K[X][1/f] and the modules K[X][1/f]fs are built.

Comparison

The standard first modules over An (over a field of characteristic zero; the last row is over A1(ℂ)).
ModulePresentationCyclicSimpleTorsiond(M)
K[X]An/∑iAn∂iyesyesyesn
K[∂]An/∑iAnxiyesyesyesn
K[X]σ, σ an automorphismAn/σ−1(∑iAn∂i)yesyesyesn
An itselfAn/0yesnono2n
K[X][1/f], f≠0 non-constantcyclic, holonomicyesnoyesn
ℋ(U), holomorphic functionsnone finitenonononot defined

Key Takeaways

Key points

  • K[X] is a left An-module by construction: An was defined as a subring of EndK(K[X]), with xi multiplying and ∂i differentiating.
  • It is cyclic on the generator 1, whose annihilator is the left ideal ∑i=1nAn∂i, giving K[X]≅An/∑iAn∂i.
  • The proof is one application of the canonical basis theorem: split an operator into its ∂-free part plus a member of the ideal.
  • Every polynomial is a torsion element, yet the module is faithful - torsion is a condition on elements, not on the module.
  • In characteristic zero the module is simple, and the ideal ∑iAn∂i is therefore a maximal left ideal; in characteristic p simplicity fails, though the presentation survives.
  • Dividing by the xi instead gives K[∂], the Fourier transform of K[X], on which the partials multiply and the variables differentiate with a sign.
  • K[X] is holonomic with d=n and e=1, the smallest invariants a non-zero module over An can have.

FAQs

Do I need to check that the action is well defined?

No, provided the Weyl algebra is defined as a subring of EndK(K[X]), which is the definition used in this collection. The action is then the inclusion itself. If instead you define An by generators and relations, you must check that multiplication and differentiation satisfy those relations - which is the content of [∂i,xj]=δij as operators, verified by the product rule.

How can K[X] be a torsion module and faithful at the same time?

Torsion means each element separately has a non-zero annihilator; faithfulness means the intersection of all those annihilators is zero. For f of degree d, ∂1d+1 kills f but kills nothing of higher degree, so the annihilators shrink to nothing as f ranges over the module. Over a commutative domain this behaviour cannot occur for a finitely generated module, which is where the intuition misleads.

Is K[X] finitely generated as an An-module?

Yes, by a single element - it is cyclic. That is compatible with being infinite dimensional over K, because An is itself infinite dimensional over K.

Why is ∑iAn∂i a maximal left ideal?

Because the quotient by it is K[X], which is a simple module in characteristic zero. Left ideals containing J correspond to submodules of An/J, and a simple module has only the two trivial submodules.

What replaces K[X] when I want more solutions than the polynomial ones?

Formal power series, convergent power series, rational functions K[X][1/f], or - over ℂ in one variable - the holomorphic functions ℋ(U). Each is an An-module by the same formulas, and the solution space of a system grows as the module does. The polynomial module is the smallest of them.

Is K[X] isomorphic to K[∂] as an An-module?

No. Their annihilator ideals are ∑iAn∂i and ∑iAnxi, and these are different maximal left ideals; an isomorphism of cyclic modules would force the annihilators of corresponding generators to coincide. They are, however, related by an automorphism of An: K[∂] is the Fourier twist of K[X].

Does the presentation change in characteristic p?

No. The proof uses only that {xα∂β} is a K-basis of An, which holds in any characteristic. What fails in characteristic p is simplicity, and hence the maximality of the ideal: x1pK[X] is a proper non-zero submodule.

What is the analogue for An/∑iAn(∂i−gi)?

As a K-vector space it is again K[X], by the same splitting argument, but the derivative acts by f↦∂f/∂xi+gif. When the gi satisfy the integrability condition ∂gi/∂xj=∂gj/∂xi these modules are exactly the twists of K[X] by automorphisms fixing the xi, and deciding when two of them are isomorphic produces infinitely many pairwise non-isomorphic simple modules.

Related Engineering Topics

  • The Weyl Algebra Defined as a Ring of Operators

    Where the action on K[X] comes from: An is a subring of EndK(K[X]).

    Prerequisite
  • Why the Polynomial Ring Is a Simple Weyl Module

    The proof that every non-zero polynomial generates, and what it needs from the ground field.

    Next step
  • Twisting a Weyl Module by an Automorphism

    How to bend the derivative action and produce new simple modules, including K[∂].

    Next step
  • When Are Two Twisted Modules Isomorphic?

    An infinite family of pairwise non-isomorphic simple modules built from this one.

    Consequence
  • Holomorphic Functions as a Module over the Weyl Algebra

    The analytic enlargement: neither simple nor torsion, and not cyclic.

    Contrast

References

  1. S. C. Coutinho, A Primer of Algebraic D-modules, London Mathematical Society Student Texts 33, Cambridge University Press, 1995 - Ch. 5 §1, Lemma (5.1.1) and Proposition (5.1.2).
  2. S. C. Coutinho, A Primer of Algebraic D-modules, Cambridge University Press, 1995 - Ch. 1, for the construction of An inside EndK(K[X]) and the canonical basis.
  3. P. M. Cohn, Algebra, Volume 1, second edition, Wiley, 1982 - Ch. 10, for the module-theoretic background assumed here (cyclic modules, annihilators, the isomorphism theorems).
  4. J. Dixmier, Sur les algèbres de Weyl, Bulletin de la Société Mathématique de France 96 (1968), 209-242 - the systematic study of A1 and its modules.
  5. J.-E. Björk, Rings of Differential Operators, North-Holland Mathematical Library 21, North-Holland, 1979 - Ch. 1, for the polynomial module in the filtered setting.
  6. J. C. McConnell and J. C. Robson, Noncommutative Noetherian Rings, revised edition, Graduate Studies in Mathematics 30, American Mathematical Society, 2001 - Ch. 1 and Ch. 8, for annihilators and the ring-theoretic context.
  7. R. Hotta, K. Takeuchi and T. Tanisaki, D-modules, Perverse Sheaves, and Representation Theory, Progress in Mathematics 236, Birkhäuser, 2008 - Ch. 1, for the polynomial module as the structure sheaf of affine space.
  8. ISO 80000-2:2019, Quantities and units - Part 2: Mathematics, International Organization for Standardization - notation for ∂, ℕ and operator names.

AI Suggested Questions

  • Show directly that {xα∂β:β≠0} is a K-basis of the left ideal ∑iAn∂i.
  • Compute a generating set for annA1(x2) and check that the quotient is isomorphic to K[x].
  • Verify the identity xi⋅∂β=−βi∂β−ei in An/∑jAnxj for n=1 and β=3.
  • Prove that K[X] is not a projective An-module for general n, extending the argument given for n=1.
  • Show that in characteristic p the submodules x1kpK[X] form a strictly decreasing chain, so K[X] is not even of finite length.
  • Compute HomA1(A1/A1(x∂−2),K[x]) and interpret the answer as a space of polynomial solutions.
  • Give a good filtration on K[X] different from Γm=Bm⋅1 and check that the dimension and multiplicity are unchanged.

On this page

  1. Overview
  2. Definition
  3. Core Concepts
  4. Construction and Proof
  5. Key Equations
  6. Variable Definitions
  7. Properties and Behaviour
  8. Examples and Special Cases
  9. Worked Example
  10. Applications and Industry Use
  11. Design Considerations
  12. Computational Notes
  13. Failure Modes and Common Mistakes
  14. Historical Notes
  15. Comparison
  16. Key Takeaways
  17. FAQs
  18. Related Engineering Topics
  19. References
  20. AI Suggested Questions

Part of the KEVOS® Engineering › Mathematics knowledge library, collection Algebraic D-modules.

This page is original explanatory prose. Source results are attributed in the References section; the underlying textbook is in copyright and is cited, not reproduced.

Page ID KVS-ENG-MATH-0350 Taxonomy /engineering/mathematics Category ID ENG / ENG-MATH Level Foundation Reading time 28 min Page version 1.0.0 Content version 2026.08 Reviewed 2026-08-09

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