Overview
For the polynomial ring one can simply write down the operators one wants: finite sums . That description depends on having coordinates, and it does not survive a change of ring. If is the coordinate ring of a singular variety there are no coordinates and no obvious partial derivatives, yet there is still a sensible notion of differentiating a function on that variety.
The way out is to characterise differential operators by a property they have rather than by a formula they satisfy. The property is this: a differential operator of order fails to be -linear, but it fails in a controlled way - its commutator with multiplication by any element of is a differential operator of order . That is a definition by induction, with -linear operators as the base case, and it uses nothing but the ring structure of .
The definition produces a chain inside , and the union is a subring. Two facts make it a filtered ring rather than a merely increasing chain: composition adds orders, and commutators drop the total order by one. The second fact is what makes the associated graded ring commutative and puts geometry within reach.
This page sets up the definition, proves the two structural propositions, records the equivalent formulation by iterated commutators and Grothendieck's version by principal parts, and shows on that finite order is a genuine restriction: the algebra endomorphism is an operator of infinite order.
Definition
Let be a field of characteristic zero and a commutative -algebra with . Identify with the multiplication operator in ; this is injective. For and write , again an element of .
Operators of order at most Coutinho, Ch. 3 §1
Set . For define, by induction on ,
An operator has order if it lies in but not in . An operator has finite order if it lies in for some .
The ring of differential operators
The ring of differential operators of over is
with the addition and composition it inherits from . That this is closed under composition is Proposition (3.1.2) below and is the only point requiring proof.
A convention worth stating
Coutinho phrases the induction in terms of order exactly : has order zero if it commutes with every , and order if it does not have smaller order but has order less than for all . The two formulations define the same sets . The form used here is more convenient because is then visibly a subspace containing ; the set of operators of order exactly is not a subspace, since a difference of two order- operators can have lower order.
Core Concepts
Order measures the failure of -linearity
An operator of order commutes with all multiplications, so it is -linear, and an -linear endomorphism of is determined by its value at : . Order then says that the failure of -linearity, measured by , is itself -linear - which is the Leibniz rule in disguise. Order says the failure of the failure of ... is -linear, levels down. Order is a measure of how far an operator is from being multiplication by a function.
Why commutators and not something else
On , differentiating a product introduces exactly one extra term: , so . The commutator with strips one derivative and leaves a function. Nothing about coordinates is used in that observation, only that multiplication by and the operator nearly commute. The inductive definition promotes this to the defining property.
Two structural facts, and what they buy
Composition adds order, , which is what makes a ring and a filtered one. Commutators lose an order, , which is what makes the associated graded ring commutative. The second fact is the reason a non-commutative ring like can be studied with commutative algebra at all: pass to symbols, work in a commutative ring, transfer conclusions back. Every dimension theory in this collection depends on it.
Finite order is a restriction
It is easy to forget that is usually much smaller than . For the algebra endomorphism sending to has infinite order, as the worked example verifies. Only the finite-order part is captured, and that is the point: finite order is the algebraic shadow of locality.
Construction and Proof
Each is an -bimodule
is a -subspace of , it contains , and it is stable under left and right multiplication by elements of .
Proof
Linearity of gives the subspace claim by induction. For the inclusion, if then by induction, so . For the bimodule claim, note that commutes with , so and ; induction on finishes it.
Composition adds orderCoutinho (3.1.2)
If and then . In particular is a subring of .
Proof
Induct on . If both operators are multiplications, and so is their composite. Assume the statement for all pairs with smaller total. For , the derivation property of on the associative ring gives
Now and , so by the inductive hypothesis both and lie in . Hence for every , which is precisely the statement .
Commutators drop order
If and with , then .
Proof
Induct on . If then and are multiplications by elements of the commutative ring , so . For the step, use the Jacobi identity in :
The first term pairs with , the second pairs with ; by induction both lie in . Hence for all , so .
The symbol algebra is commutative
The associated graded ring is a commutative -algebra, because the class of in degree is zero by the previous proposition. See the order filtration and symbols for the case , where the graded ring is a polynomial ring in variables.
Key Equations
Write . Since is commutative, multiplication operators commute, and consequently the operators commute with one another on :
Unwinding (3.1) gives a non-inductive description, symmetric in its arguments by (3.3):
The first two layers are known explicitly, the second by the lemma on derivations:
The two structural rules are
Grothendieck's equivalent formulation replaces the induction by a single . Let be the multiplication map, , and the module of principal parts, regarded as an -module through the left factor. Then
For this specialises to , recovering (3.5).
Variable Definitions
- the ground field, of characteristic zero
- a commutative -algebra with identity
- all -linear maps , a ring under composition
- an element of , and also the multiplication operator
- the commutator inside
- the map on
- the -space of differential operators of order at most
- the ring of differential operators, the union of the
- the -module of -derivations of
- the module of principal parts of order
Properties and Behaviour
Differential operators localise
Let be a finitely generated commutative -algebra and a multiplicative set. Then for every
The reason is (3.7): is Noetherian, so is a finitely presented -module, and out of a finitely presented module commutes with localisation. Concretely, an operator on extends uniquely to by the quotient rule, and clearing denominators brings any operator on back into after multiplication by an element of .
Products and disjoint unions
. Differential operators cannot mix the two factors: an operator of finite order commutes with the idempotents up to lower order, and the argument in the examples section shows it must preserve each factor. Geometrically, differential operators are local and cannot move mass between connected components.
Domains
If is a domain with fraction field , then restriction gives an isomorphism
Every operator on extends uniquely to by the previous proposition, and the order conditions are inherited by restriction. This is the practical way to compute for a singular affine curve: work with operators with rational coefficients and impose the condition that they preserve . Coutinho sets this out as Exercise 3.7; the version stated there identifies the set as a subring, and the sharper statement is that it is .
What can go wrong
None of the good properties of the Weyl algebra are automatic for a general . need not be Noetherian, need not be finitely generated as a -algebra, and need not be a domain. It also need not be generated by and . All four failures occur already for coordinate rings of singular affine curves; see differential operators on an affine variety.
Examples and Special Cases
and every operator is multiplication, so with for all . The filtration is constant.
, the -th Weyl algebra, and is the span of the with . This is the theorem of Ch. 3 §2 and it needs characteristic zero.
Laurent polynomials
, the localisation of at the powers of , by the localisation proposition. This ring is again simple and Noetherian; it is the ring of operators on the punctured line.
: order does not stabilise upwards
Let . Suppose and, inductively, that . Then is multiplication by some . Evaluating at gives ; evaluating at gives . Combining, , and since the left side lies in and the right side in , both vanish. Hence and , so preserves each factor and acts on each by a scalar: . Therefore , strictly smaller than the four-dimensional .
: order does not stabilise at all
Here has dimension and has dimension . The map with , satisfies and , which is the element of ; so , and . Since has dimension , we get . For a finite-dimensional algebra the filtration exhausts everything, and the notion of order carries no geometric content.
Worked Example
Orders in , computed from the definition alone
- Step 1 - order zero and order one
, since an operator commuting with multiplication by every polynomial is -linear and hence multiplication by its value at . For and , the product rule gives , so . Thus . It is not in because . So has order exactly .
- Step 2 - the order of
Apply to a product: . As operators this reads , so
The right-hand side lies in by Step 1, so . It is not in : taking gives , and , so the double commutator does not vanish. Hence has order exactly , as (3.4) predicts.
- Step 3 - a mixed operator
Let , the Euler operator. Then , an element of , so has order ; it is not order because . The operator has order by the composition rule, and its double commutator with is , confirming the order is exactly and not less.
- Step 4 - an endomorphism of infinite order
Let be the -algebra endomorphism of with , so . Set . Then and
Claim: for every . It holds for ; and if it holds for , then , which is the claim for .
- Step 5 - conclude
Since for every , no iterated commutator of with vanishes. By (3.4), for any . The check at , say, is and , both non-zero.
has order , order , order , order ; and the dilation , although a perfectly good -algebra automorphism of , has infinite order and is therefore not a differential operator. So is a proper subring of , and by the theorem of Ch. 3 §2 it is exactly the Weyl algebra .
Applications and Industry Use
In a mathematics topic, this section covers downstream use inside mathematics, computing and engineering rather than a manufactured product.
- A uniform definition across geometry. The same induction defines on any scheme by sheafifying, which is what makes D-module theory available on varieties rather than just on affine space.
- Singular spaces. For quotient singularities, toric varieties and cones, computed from this definition is the right object; there is no coordinate description to fall back on.
- Invariant differential operators. If a group acts on , the invariants and the operators on are both defined by this induction, and comparing them is the Levasseur-Stafford circle of results in representation theory.
- Rings of differential operators as test objects. Because can fail to be Noetherian or finitely generated, it supplies natural counterexamples in non-commutative ring theory; the Bernstein-Gelfand-Gelfand cubic cone is the standard one.
- Deformation quantisation. The filtration with commutative associated graded ring realises as a deformation of functions on the cotangent space, with the Poisson bracket induced by ; see the Poisson bracket on the symbol algebra.
Design Considerations
For a mathematical object, design considerations are the modelling choices: which ring, which filtration, which category to work in.
Inductive definition or principal parts
Definitions (3.1) and (3.7) agree, and each is better for a different job. The inductive definition is what one uses to prove things about operators, because every proof is an induction on order and each step is a commutator identity. The principal parts definition is what one uses to construct things: it is manifestly functorial, it sheafifies without effort, and it exhibits as a , hence as something computable by linear algebra over once is presented.
Which filtration to carry
The order filtration is intrinsic: it exists for every and needs no coordinates. The Bernstein filtration, which gives and equal weight, is available only for the Weyl algebra and depends on the choice of coordinates, but its pieces are finite dimensional over , which the order filtration's are not. For general there is no analogue of the Bernstein filtration, which is one reason the elementary proof of Bernstein's inequality does not transport to singular varieties.
Left modules or right modules
is a left -module by construction. The definition is symmetric enough that right modules are equally natural, and on a smooth variety the two categories are equivalent via twisting by the canonical module. On a singular that equivalence is unavailable, so the choice of side has to be made explicitly and kept.
Standards and Codes
For mathematics, the relevant standards are notation, numeric and markup standards together with reference implementations.
- ISO 80000-2 governs the symbols , , and the set-theoretic notation used above.
- ISO/IEC 40314 (MathML 3.0) is the encoding of every formula on this page.
- Notation for the operator ring is not standardised. , , and all appear; the superscript convention for order at most is near-universal, but some authors write or for the same thing. This collection uses , and when the same filtration is regarded abstractly.
- Grothendieck's definition in EGA IV §16 is the reference formulation for algebraic geometry, and is the one implemented in schemes-oriented software.
Material Selection
The material of a mathematical construction is its numeric substrate: the ground field, the coefficient ring and the representation used to store it.
- Characteristic zero. The definition (3.1) makes sense over any commutative base, but its content changes. In characteristic , contains the divided-power operators for all , and these are not polynomials in once . So is strictly bigger than the Weyl algebra, and the order filtration has infinite-dimensional pieces even over .
- Base ring. Everything above works with replaced by a commutative base ring and a commutative -algebra, giving . The relative version is what one needs for families and for the parameter in the Bernstein-Sato construction.
- Reduced versus non-reduced. For finite-dimensional algebras the filtration exhausts , so order carries no information. Interesting behaviour begins when has positive Krull dimension.
- Storage. An operator on is normally stored as a representative in the Weyl algebra over , together with ; the representative is not unique, and comparison requires normal-form computation modulo the idealiser of .
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.
Computing for is harder than computing , and is not always a finite problem, since need not be finitely generated. What can be computed is each filtration piece.
- Compute the ideal and a presentation of from generators and relations, or equivalently set up the linear conditions defining .
- Solve as a syzygy computation; this returns as an -module with explicit generators.
- For a domain, use the fraction-field description instead: parametrise operators of order at most with coefficients in and impose for algebra generators of , together with the conditions coming from applied to products.
- Increase and look for stabilisation of the generating set. Stabilisation is not guaranteed, and its failure is exactly the statement that is not finitely generated.
Macaulay2 provides Dmodules for the smooth polynomial case and Hom computations for principal parts; Singular's dmod.lib and dmodapp.lib cover Weyl-algebra computations. There is no general-purpose algorithm returning for arbitrary singular , and there cannot be one that always terminates with a finite presentation.
A useful sanity check while implementing: must come back as itself, and must come back as . If either fails, the linear conditions have been set up wrongly, most often by forgetting that the commutator is taken with all of and not only with the algebra generators.
Limits of Validity
The definition is completely general; the useful theorems about it are not.
- need not be generated by and . This holds for regular in characteristic zero and fails on singular rings. Assuming it is the single most common error in this area.
- need not be Noetherian or finitely generated. For the cone over a plane cubic, Bernstein, Gelfand and Gelfand showed is neither.
- Commutativity of is used. The proof that and commute, and hence the symmetry in (3.4), uses . For non-commutative one must decide first what a differential operator should mean.
- Finite dimensionality of the filtration pieces fails. is a finitely generated -module in good cases but is essentially never finite dimensional over . Any counting argument in the style of Bernstein's inequality must therefore use a different filtration.
Failure Modes and Common Mistakes
Checking the commutator only against algebra generators
Definition (3.1) quantifies over all . It is true that for it suffices to test , but that is a small lemma resting on the identity and on being an -bimodule; it is not part of the definition. On a quotient ring, testing only lifted generators can give a wrong answer if the relations are not respected.
Assuming , or that it is much smaller
Both extremes occur. For finite dimensional over the two coincide. For the operator ring collapses to . For it is the Weyl algebra, strictly between and . Nothing can be inferred about the size of without looking at .
Reading "order " as a vector space condition
The set of operators of order exactly is not closed under addition: and both have order and their sum has order . Only , the operators of order at most , is a subspace. Statements about symbols are statements about the quotients , not about order- operators as a set.
Carrying the characteristic-zero picture into characteristic
In characteristic the operator is a differential operator of order on that is not in the subring generated by and , because on in that setting. The definition does not change; the answer does. See the Weyl algebra in positive characteristic.
Confusing the order filtration with the Bernstein filtration
is defined for every and its pieces are -modules of infinite -dimension. The Bernstein filtration exists only for , gives and equal weight, and has finite-dimensional pieces. Arguments that count require the latter; arguments that need functoriality require the former.
Historical Notes
The idea of characterising differential operators by iterated commutators appears in the 1950s. Grothendieck gave the definitive algebraic formulation in EGA IV (1967), §16, defining as and proving the composition and commutator rules in that setting. The equivalence with the inductive form is immediate once the ideal is introduced, and the inductive form has been the working definition in the D-module literature ever since.
The theorem that in characteristic zero, which is what ties the intrinsic definition back to the concrete one, is proved on its own page and is the whole point of Coutinho's Chapter 3.
That can be badly behaved was settled quickly. In 1972 Bernstein, Gelfand and Gelfand computed for the cone over a plane cubic curve and found a ring that is neither Noetherian nor finitely generated. In the opposite direction, the good behaviour for regular - generation by and , Noetherianity, simplicity in the irreducible case - is treated in McConnell and Robson, Ch. 15. The pattern that emerged, that regularity is exactly the dividing line, has organised the subject since.
Comparison
| Inductive (commutators) | Grothendieck (principal parts) | Coordinates | |
|---|---|---|---|
| Applies to | any commutative -algebra | any commutative -algebra | polynomial and regular rings only |
| Form | for all | ||
| Best for | proofs by induction on order | functoriality and sheafification | explicit computation |
| Sheafifies | yes, after localising | yes, immediately | only with a chosen atlas |
| Needs char | no | no | yes, to be complete |
| Filtration pieces | -modules | -modules | free -modules |
Key Takeaways
Key points
- and means for every ; is the union.
- Equivalently, has order at most when every iterated commutator with elements of vanishes.
- and .
- Composition adds orders and commutators drop the total order by one, so is a filtered ring with commutative associated graded ring.
- Grothendieck's equivalent definition is , which sheafifies at once.
- Finite order is a real restriction: the dilation on has infinite order.
- Nothing about Noetherianity, finite generation or generation by derivations follows from the definition; those need regularity of .
FAQs
Why start the induction at ?
It makes the single clause (3.1) cover as well: for all says exactly that is -linear, so . Without the convention one has to state the base case separately, as Coutinho does.
Is it enough to test the commutator against a set of algebra generators of ?
For yes, and that is how computations are done. The reason is that is an -bimodule and , so the condition propagates from generators to products. For a general presented as the reduction is not automatic and the relations must be taken into account.
How does this recover the usual definition on ?
It gives and , but only in characteristic zero, and the proof is not formal: it needs two lemmas, one saying an operator commuting with all is a polynomial, the other a discrete Poincaré lemma. See the Weyl algebra as a ring of differential operators.
Is always bigger than the ring generated by and its derivations?
It always contains it, and the containment is an equality exactly when is regular (in characteristic zero, for finitely generated reduced algebras). For singular the containment is usually strict; the cusp is the smallest standard example.
Does the definition depend on being commutative?
Yes, in two places. The identification uses that -linear endomorphisms of are multiplications, and the symmetry of (3.4) uses that the operators commute. Non-commutative analogues exist but require choices.
Why is it important that commutators drop the order?
Because it makes commutative. Every dimension, multiplicity and characteristic variety argument in D-module theory is carried out in that commutative graded ring and then transferred back. Without the drop there would be no commutative shadow to work in.
Can be infinite dimensional over ?
Almost always. Already is infinite dimensional. Finite dimensionality of filtration pieces is a feature of the Bernstein filtration on the Weyl algebra, not of the order filtration.
Does the ring of differential operators determine ?
Not in general, and this is a delicate question. Non-isomorphic rings can have isomorphic rings of differential operators - for instance certain non-isomorphic affine curves. Recovering requires remembering more structure, such as the filtration together with the action on .
References
- S. C. Coutinho, A Primer of Algebraic D-modules, London Mathematical Society Student Texts 33, Cambridge University Press, 1995 - Ch. 3 §1, with Lemma (3.1.1) and Proposition (3.1.2); Exercises 3.2, 3.3, 3.7.
- A. Grothendieck, Éléments de géométrie algébrique IV, quatrième partie, Publications Mathématiques de l'IHÉS 32 (1967), §16 - the definition of by principal parts.
- J. C. McConnell and J. C. Robson, Noncommutative Noetherian Rings, Graduate Studies in Mathematics 30, revised edition, American Mathematical Society, 2001 - Ch. 15, for rings of differential operators over commutative rings.
- J.-E. Björk, Rings of Differential Operators, North-Holland Mathematical Library 21, North-Holland, 1979 - Ch. 1, for the filtration and the graded ring.
- I. N. Bernstein, I. M. Gelfand and S. I. Gelfand, Differential operators on a cubic cone, Russian Mathematical Surveys 27 (1972), 169-174.
- S. P. Smith and J. T. Stafford, Differential operators on an affine curve, Proceedings of the London Mathematical Society (3) 56 (1988), 229-259.
- R. Hotta, K. Takeuchi and T. Tanisaki, D-modules, Perverse Sheaves, and Representation Theory, Progress in Mathematics 236, Birkhäuser, 2008 - Ch. 1, for the sheaf-theoretic version.
- ISO/IEC 40314:2016, Information technology - Mathematical Markup Language (MathML) Version 3.0, International Organization for Standardization.
- ISO 80000-2:2019, Quantities and units - Part 2: Mathematics, International Organization for Standardization.
AI Suggested Questions
- Prove that for it suffices to test the commutator condition against , and identify where the bimodule property is used.
- Verify directly from (3.1) that has order on by computing two iterated commutators.
- Deduce (3.5) from (3.7) by computing explicitly.
- Show that in general, following the argument given for .
- Find an operator of order on that is not a polynomial in the derivations of that ring, and verify its order.
- Show that in characteristic the divided-power operator has order and is not in the subring generated by and .
- Prove that equals whenever is finite dimensional over .
