Overview
The elementary theory of algebraic D-modules has a clean shape, and knowing it in advance saves a great deal of time. It divides into two halves of roughly equal length. The first half attaches invariants to a module over the Weyl algebra : a dimension, a multiplicity, a characteristic variety. The second half constructs operations that turn modules over one Weyl algebra into modules over another, following a polynomial map between the underlying affine spaces. The two halves meet in a single theorem: the operations preserve the class of modules picked out by the invariants.
Before either half can begin, the ring itself has to be understood. The opening chapters establish that is a simple Noetherian domain with a canonical form for its elements, and place it inside the wider family of rings of differential operators. That material is short, entirely elementary, and used everywhere afterwards; nothing later can be read without it.
The pay-off comes in two application chapters at the end, which are deliberately unlike each other. One uses a D-module argument to attack the global asymptotic stability of polynomial vector fields, a question in dynamics. The other turns the finiteness properties of holonomic modules into an algorithm that proves combinatorial identities automatically. Between them they demonstrate that the machinery is not self-referential.
The order of the material is almost, but not quite, linear. Three parts of the theory are optional in the strict sense that nothing else depends on them, and identifying those in advance is the single most useful thing a roadmap can do. This page marks them, sets out the milestone theorems, and follows one small module all the way through the theory so that the architecture is visible in a single example.
Core Concepts
Four ideas structure the whole development, and each is introduced exactly once.
The ring is small enough to control
has a canonical form: every operator is uniquely . That single fact makes it a domain, makes it Noetherian, and makes it simple. Simplicity is used constantly, because it forces every non-zero module to be faithful. Everything in the first two chapters exists to establish these properties, and they are never proved again.
Filtrations convert noncommutative questions into commutative ones
is not commutative, but it becomes so in the limit: filter it by degree and the associated graded ring is a polynomial ring in variables. A finitely generated module carries a good filtration, its associated graded module is a finitely generated module over that polynomial ring, and commutative Hilbert-function theory applies. This is the mechanism behind the entire invariant theory. Chapters 7 and 8 build the mechanism; Chapter 9 uses it.
One number decides everything
The dimension , the degree of the Hilbert polynomial, is confined by Bernstein's inequality to . Modules attaining the minimum are holonomic, and they turn out to have every property one could want: finite length, cyclicity, closure under extension. A large fraction of the theory consists of proving that some naturally arising module is holonomic, because that single word carries all the finiteness.
Geometry acts through functors
A polynomial map does not map to , so operations on modules must be built by hand, out of tensor products. The inverse image generalises composing a function with ; the direct image generalises integrating over the fibres. Both are constructed by factoring an arbitrary map into a closed embedding followed by a projection, which is why embeddings get a chapter of their own.
Key Equations
Six formulas recur throughout. Everything on this page can be located by which of them it is about.
the defining relation and the canonical form (Chs. 1-2).
the associated graded ring, a commutative polynomial ring (Ch. 7).
the Hilbert polynomial and the two numerical invariants (Ch. 9).
Bernstein's inequality and the definition it licenses (Chs. 9-10).
the characteristic variety and the geometric reading of the dimension (Ch. 11).
the two operations, in outline (Chs. 14-16).
Variable Definitions
- the ground field, of characteristic zero throughout
- the -th Weyl algebra over
- the ring of differential operators of a commutative -algebra
- ,
- the -th pieces of the Bernstein and order filtrations of
- the -th piece of a good filtration of a module
- the associated graded ring or module of a filtered object
- the Hilbert polynomial of a good filtration
- ,
- the dimension and the multiplicity of
- ,
- the characteristic variety and the characteristic ideal of
- ,
- the inverse and direct image functors attached to a polynomial map
Properties and Behaviour
Five theorems carry the structural weight. Everything else is either preparation for one of them or a consequence of one of them.
Simplicity of the Weyl algebraCoutinho, Ch. 2 §2
For of characteristic zero, the only two-sided ideals of are and . Consequence: every non-zero module is faithful, which is the hypothesis every dimension estimate silently uses.
Existence of the Hilbert polynomialCoutinho, Ch. 9 §1-§2
If is finitely generated with a good filtration , then agrees with a polynomial in for large , and its degree and leading coefficient are independent of the good filtration chosen. Consequence: and are invariants of , not of the presentation.
Bernstein's inequalityCoutinho (9.4.2)
for every non-zero finitely generated -module. Consequence: the definition of holonomicity is not vacuous, and 'minimal dimension' is a meaningful condition.
Kashiwara's theoremCoutinho, Ch. 17 and Ch. 18 §3
For the embedding of a coordinate subspace , the direct image is an equivalence between -modules and those -modules supported on the subspace. Consequence: modules concentrated on a subvariety are completely described by modules on that subvariety, which is what makes induction on dimension possible.
