Fun with k-Algebras
Continuing from last time, suppose we have a bilinear map f from V×W to L where V, W, and L are vector spaces. Then there is a universal property function Φ from V×W to V⊗W and there is a unique linear map g from V⊗W to L such that the diagram below commutes:
Φ
V×W-------> V⊗W
\ |
\ |
\ |
f \ | g
\ |
\ |
_| \/
L
The proof is trivial: "f" is used to define a function from the free vector space F(V×W) to L and then we make a descent by modding by the usual equivalence relation of the tensor product to define the map g.
This all looks a bit pedantic, but the point is that any multiplication rule in an algebra A is a bilinear map from A×A to A and we can now put it in tensor formalism.
In particular consider the algebra A of matrices over a field k. Matrix multiplication is associative, and we also have a unit of the algebra: the diagonal matrix with the where the elements are the identity of k. This is a prototypical example of what is called a k-algebra.
Can we formalize the associativity and the unit using the tensor product language? Indeed we can and here is the formal definition:
A k-algebra is a k-vector space A which has a linear map m:A⊗A→A called the multiplication and a unit u:k→A such that the following diagrams commute:
m⊗1
A⊗A⊗A ----------> A⊗A
| |
| |
1⊗m | | m
| |
| |
\/ \/
A⊗A ----------> A
m
and
A⊗A
_ _
| | |
u⊗1 / | \ 1⊗u
/ | \
k⊗A | m A⊗k
\ | /
\ | /
_| \/ |_
A
Please excuse the sloppiness of the diagrams, it is a real pain to draw them.
So what are those commuting diagrams really saying?
The first one states that:
m(m(a⊗b)⊗c)=m(a⊗m(b⊗c))
In other words: associativity of the multiplication: (a b) c = a (b c)
The second one defines the algebra unit:
u(1k)a=au(1k)
which means that u(1k)=1A
So why do we torture ourselves with this fancy pictorial way of representing trivial properties of algebra? Because now we can do a very powerful thing: reverse the direction of all the arrows. What do get when we do that? We get a brand new concept: the coproduct. Stay tuned next time to explore the wondeful properties of this new mathematical concept.
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