Tensor algebras

Motivation


Given a commutative ring R and two R-modules M and N, the R-module M⊗RN satisfies a universal property that captures the idea of being able to multiply elements in M with elements in N. In the special case M=N, the module M⊗RM gives us a way to compute products of elements in M. It doesn't quite give us a ring structure on M, however, since it doesn't allow us to multiply together more than two elements in M.

Question

Can we amplify our tensor product construction to obtain a module with a full ring structure, capturing the desire of layering a multiplicative operation on the R-module M?

Yes. Let's see how.

A desired universal property


With the above motivation in mind, we are looking for a functor from the category of R-modules to the category of R-algebras that is "free" in the same sense as the free R-module construction on a set S; i.e., that is left adjoint to the corresponding forgetful functor.

A universal property of the tensor algebra

Let U:R-Alg→R-Mod be the forgetful functor from the category of R-algebras to the category of R-modules. Then there is functor T:R-Mod→R-Alg together with a natural bijection

τM,A:HomR-Alg(T(M),A)→∼HomR-Mod(M,U(A)).

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

Even without having seen the construction yet, such a property gives us a way to think about T(M):

The construction


Since M⊗RM captures the idea of multiplying two elements in M, the construction/definition below probably comes as no surprise.

Definition of tensor algebra

Suppose R is a commutative ring (with unity) and M is an R-module. Set T0(M)=R and for each positive integer i define the ith tensor power of M to be the R-module

Ti(M)=M⊗RM⊗R⋯⊗RM⏟i times.

The elements of Ti(M) are called i-tensors.

Then define the tensor algebra of M to be the R-module

T(M)=⨁i=0∞Ti(M).

Every element of T(M) is a finite formal linear combination of i-tensors.

As the name implies, the R-module T(M) has a (natural) structure of an R-algebra. The multiplication on simple tensors is defined by concatenation of tensors:

(m1⊗⋯⊗mi)⋅(m1′⊗⋯⊗mj′):=m1⊗⋯⊗mi⊗m1′⊗⋯⊗mj′.

The multiplication on sums of tensors is defined via the distributive laws. Note that this multiplication satisfies Ti(M)Tj(M)⊆Ti+j(M). In other words, the tensor algebra T(M) has the structure of a graded ring.

It's worth noting that, as a ring, the tensor algebra T(M) is generated by the elements of T0(M)=R and T1(M)=M.

At some point we should verify that this construction satisfies the claimed universal property. For now, however, let's look at some examples.

Examples


  1. Let R=Z and M=Q/Z. One can verify that Q/Z⊗ZQ/Z≃0, and so the tensor algebra is simply

    T(Q/Z)≃Z⊕(Q/Z).

    We can also unwind the multiplication rule. Let's look at a specific example. Two elements in Z⊕(Q/Z) are 2⊕[13] and 3⊕[45]. When we add these two elements we get the element

    (2+3)⊕[13+45]=5⊕[1715]=5⊕[215].

    Notice that this is not what we would get conventionally by adding the rational numbers (2+13)+(3+45)=6+215.

    When we multiply these two elements we get the element

    (2⊕[13])⊗(3⊕[45])=(2⋅3)⊕(2⋅[45]+3⋅[13])⊕([13]⊗[45])=6⊕[135]⊕0=6⊕[35].
  2. Let R=Z and M=Zn. One can verify that Zn⊗ZZn≃Zn, and so the tensor algebra is

    T(Zn)≃Z⊕Zn⊕Zn⊕⋯≃Z[x]/(nx).

    For that final isomorphism, the correspondence is that each finite formal sum c0⊕[c1]⊕[c2]⊕⋯ maps to the coset represented by the polynomial c0+c1x+c2x2+⋯.

  3. Suppose R=k is a field and V is a finite-dimensional k-vector space. Let B={v1,…,vn} be a basis for V as an k-vector space. Then a basis for the F-vector space Ti(V) is

    {vj1⊗vj2⊗⋯⊗vji∣vjl∈B}.

    (When i=0, the basis is simply {1}.) In particular, Ti(V) is a k-vector space of dimension ni.

Suggested next notes


Symmetric algebras
Exterior algebras
Symmetric and alternating tensors