Properties of the Tensor Product

Here are various results about the tensor product, one of my favorite mathematical constructions.


Lemma:

Let AA be a ring with elements f,gf, g. Then A/(f)AA/(g)A/(f,g)A/(f)\otimes_{A}A/(g)\cong A/(f, g), where we give the quotients the natural AA-algebra structure.

Proof. We can always write an element aba\otimes b of A/(f)AA/(g)A/(f)\otimes_AA/(g) as ba1b'a\otimes 1 for some lift bAb'\in A of bb, because the maps which we use to make A/(f)A/(f) and A/(g)A/(g) into AA-algebras are surjective. Explicitly, we can lift bb to an element bb' of AA with ab=a(b1)=(ba)1a\otimes b = a\otimes (b'\cdot 1) = (b'\cdot a)\otimes 1 (where \cdot is the action of AA on A/(g)A/(g) or A/(f)A/(f), as appropriate). From this, we see that the map AA/(f)AA/(g)A\to A/(f)\otimes_AA/(g) by the rule cc1c\mapsto c\otimes 1 is surjective. Suppose c=af+bgc= af+bg. Then c(af+bg)A1=afA1+1Abg=0c\mapsto (af+bg)\otimes_A1=af\otimes_A1 + 1\otimes_Abg = 0. Similarly, if c1=0c\otimes 1 = 0, then we must have c=t1A1+1v1=0+0c = t\cdot 1\otimes_A 1+ 1\otimes v\cdot 1 = 0+0 for t,vAt,v\in A; the only way for this to happen is if t(f)t\in (f) and v(g)v\in (g). Thus the ideal of this map is (f,g)(f, g), and we are done.