Symmetric algebras

Motivation

The tensor algebra construction created, from each R-module M, a "minimal" R-algebra T(M). In other words, beginning from the additive operation in M and the R-scaling on M, it created a structure that also had an internal multiplication (compatible with those structures). Our universal property formally encoded the "minimality" of the construction, in that all R-module morphisms from M to R-algebras A "lifted" to R-algebra morphisms from T(M). There were no additional properties imposed on T(M) other than those required to have an R-algebra. In particular, the R-algebra T(M) was not guaranteed to be commutative (and rarely ever is).

Question

Can we modify our construction so that the R-algebra we obtain is also commutative?

Yes. Let's do just that.

A desired universal property

As with the tensor algebra functor, there is a functor from the category of R-modules to the category of commutative R-algebras. It is analogous to any free construction and the tensor algebra construction, in that it is left adjoint to a forgetful functor:

A universal property of the symmetric algebra

Let U:R-CAlgR-Mod be the forgetful functor from the category of commutative R-algebras to the category of R-modules. Then there is a functor S:R-ModR-CAlg together with a natural bijection

τM,A:HomR-CAlg(S(M),A)HomR-Mod(M,U(A)).

In other words, the functor S is a left adjoint of the forgetful functor U.

As with any object satisfying a universal property, we can now deduce many properties of S(M):

The construction

We already have a construction that takes an R-module M and creates an R-algebra T(M) with most of the properties we want. To obtain a commutative R-algebra, it's reasonable to consider a quotient of T(M) that forces a commutativity relation in the quotient ring.

Definition of symmetric algebra

Suppose R is a commutative ring (with unity) and M is an R-module. Let C(M)T(M) be the ideal generated by elements of the form m1m2m2m1 for m1,m2M. The symmetric algebra of M is quotient

S(M)=T(M)/C(M).

Some notes are in order. First, the ideal C(M) is generated by homogeneous elements of degree 2, which implies C(M) is a graded ideal (with degree k the submodule denoted Ck(M)) and the quotient ring S(M) is a graded ring. The homogeneous component of degree k is

Sk(M)=Tk(M)/Ck(M).

This R-module is called the kth symmetric power of M. One can show that the submodule Ck(M) is generated by all elements of the form

(m1m2mk)(mσ(1)mσ(2)mσ(k)),

where miM and σSk.

Note that since C(M) is generated (as an ideal) by degree 2 homogenous elements, we have C0(M)=C1(M)=0 and hence also have S0(M)=R and S1(M)=M.

Optional notation

It is common to drop the tensor symbol between elements when working in S(M); e.g., to write simply m1m2 rather than m1m2+C(M) for the image in S(M) of the element m1m2T(M).

Example

Let V be an n-dimensional vector space over a field F. Then S(V) is isomorphic as a graded F-algebra to F[x1,,xn]. If B={v1,,vn} is a basis for V as an F-vector space, then a basis for Sk(V) is

{v1a1v2a2vnanai0,a1+a2++an=k}.

In particular, the dimension of the F-vector space Sk(V) is (n+k1n1).


Suggested next notes

Exterior algebras
Symmetric and alternating tensors