Tensor algebras
Motivation
Given a commutative ring
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
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
Let
In other words, the functor
Even without having seen the construction yet, such a property gives us a way to think about
- It is an
-algebra that we can associate to the -module ; - The construction is functorial, so that if
is an -module morphism then there is a corresponding -algebra morphism ; -algebra morphisms are in natural bijection with -module morphisms . - The identity
-algebra morphism corresponds to an -module morphism . Classically, this is viewed as an inclusion onto the degree 1 summand. (This is really a component of the unit of the adjunction.) - Since
is a left adjoint it commutes with all colimits; in particular, it commutes with coproducts (which in these categories are called direct sums). In other words .
The construction
Since
Suppose
The elements of
Then define the tensor algebra of
Every element of
As the name implies, the
The multiplication on sums of tensors is defined via the distributive laws. Note that this multiplication satisfies
It's worth noting that, as a ring, the tensor algebra
At some point we should verify that this construction satisfies the claimed universal property. For now, however, let's look at some examples.
Examples
-
Let
and . One can verify that , and so the tensor algebra is simply We can also unwind the multiplication rule. Let's look at a specific example. Two elements in
are and . When we add these two elements we get the element Notice that this is not what we would get conventionally by adding the rational numbers
. When we multiply these two elements we get the element
-
Let
and . One can verify that , and so the tensor algebra is For that final isomorphism, the correspondence is that each finite formal sum
maps to the coset represented by the polynomial . -
Suppose
is a field and is a finite-dimensional -vector space. Let be a basis for as an -vector space. Then a basis for the -vector space is (When
, the basis is simply .) In particular, is an -vector space of dimension .
Suggested next notes
Symmetric algebras
Exterior algebras
Symmetric and alternating tensors