Weyl algebra
Abstract definition
Let be a field and be an -vector space![]()
with basis
, where is some non-empty
index set
![]()
. Let be the tensor algebra of and let
be the ideal in generated by the set
where
is the Kronecker delta symbol. Then the quotient
is the
-th Weyl algebra.
A more concrete definition
If the field has characteristic zero we have the following more
concrete definition. Let be the polynomial
ring![]()
over in indeterminates labeled by . For any , let denote the partial differential operator with
respect to . Then the -th Weyl algebra is the set of all
differential operators of the form
where the summation variable is a multi-index with
entries, is the degree of , and . The algebra![]()
structure
![]()
is defined by the usual operator multiplication, where the
coefficients are identified with the operators of left
multiplication with them for conciseness of notation. Since the
derivative of a polynomial
![]()
is again a polynomial, it is clear that
is closed under
that multiplication.
The equivalence of these definitions can be seen by replacing the
generators with left multiplication by the indeterminates ,
the generators with the partial differential operator
, and the tensor product
with operator multiplication, and
observing that . If, however,
the characteristic of is positive, the resulting homomorphism
![]()
to is not injective
, since for example the expressions
and commute, while and
do not.
| Title | Weyl algebra |
|---|---|
| Canonical name | WeylAlgebra |
| Date of creation | 2013-03-22 15:27:19 |
| Last modified on | 2013-03-22 15:27:19 |
| Owner | GrafZahl (9234) |
| Last modified by | GrafZahl (9234) |
| Numerical id | 5 |
| Author | GrafZahl (9234) |
| Entry type | Definition |
| Classification | msc 16S36 |
| Classification | msc 16S32 |
| Related topic | HeisenbergAlgebra |
| Related topic | UniversalEnvelopingAlgebra |