§ Weak and Strong Nullstllensatz


§ Weak Nulstellensatz: On the tin


For every maximal ideal mk[T1,,Tn]m \subset k[T_1, \dots, T_n] there is a unique akna \in k^n such that m=I({a}) m = I(\{ a \}). This says that any maximal ideal is the ideal of some point.

§ Weak Nullstellensatz: implication 1 (Solutions)

every ideal, since it is contained in a maximal ideal, will have zeroes. Zeroes will always exist in all ideas upto the maximal ideal.

§ Weak Nullstellensatz: Implication 2 (Non-solutions)


If an ideal does not have zeroes, then it must be the full ring. Hence, 1 must be in this ideal. So if I=(f1,f2,,fn)I = (f_1, f_2, \dots, f_n) and the system has no solutions, then II cannot be included in any maximal ideal, hence I=C[X1,,Xn]I = \mathbb C[X_1, \dots, X_n]. Thus, 1I1 \in I, and there exist ciC[X1,,Xn]c_i \in \mathbb C[X_1, \dots, X_n] such that 1=sumifici1 = sum_i f_i c_i.

§ Strong Nullstellensatz: On the Tin


For every ideal JJ, we have that I(V(J))=0JI(V(J)) = |_0^\infty\sqrt J. I am adopting the radical (heh) notation 0x|_0^\infty \sqrt x for the radical, because this matches my intuition of what the radical is doing: it's taking all roots , not just square roots . For example, (8)=(2)\sqrt{(8)} = (2) in Z\mathbb Z.

§ Strong Nullstellensatz: Implication 1 (solutions)


Let J=(f1,,fm)J = (f_1, \dots, f_m). If gg is zero on V(J)V(J) , then gJg \in \sqrt J. Unwrapping this, rN,ciC[X1,,Xn],ifici=gr\exist r \in \mathbb N, \exists c_i \in \mathbb C[X_1, \dots, X_n], \sum_i f_i c_i = g^r.

§ Weak Nullstellensatz: Proof



§ Strong Nullstellensatz: Proof


We use the Rabinowitsch trick .
1=c0(Y,x)(1Yg(x))i=1mci(Y,x)fi(x) 1 = c_0(Y, \vec x) (1 - Yg(\vec x)) \sum_{i=1}^m c_i(Y, \vec x) f_i(\vec x)

Since this holds when x,Y\vec x, Y are arbitrary variables, it continues to hold on substituting Y=1/gY = 1/g, the coefficient c0(1Yg)=c0(1g/g)=c0(11)=0c_0(1-Yg) = c_0(1 - g/g) = c_0(1 - 1) = 0 disappears. This gives: 1=i=1mci(Y,x)fi(x)1 = \sum_{i=1}^m c_i (Y, \vec x) f_i(\vec x)
since Y=1/gY = 1/g, we can write ci(Y=1/g,x)=ni(x)/gir(x)c_i(Y=1/g, \vec x) = n_i(\vec x)/g^r_i(\vec x). By clearing denominators, we get:
1=i=1mni(x)fi(x)/gR(x) 1 = \sum{i=1}^m n_i(\vec x) f_i(\vec x)/ g^R(\vec x)

This means that gR(x)=i=1mni(x)fi(x) g^R(\vec x) = \sum_{i=1}^m n_i(\vec x) f_i(\vec x)

§ Strong Nullstellensatz: algebraic proof



§ Relationship between strong and weak


Strong lets us establish what functions vanish on a variety . Weak let us establish what functions vanish at a point .

§ Strong Nullstellensatz in scheme theory



Holy shit, scheme theory really does convert Nullstellensatz-the-proof into Nullstellensatz-the-definition! I'd never realised this before, but this.. is crazy.
Not only do we get easier proofs, we also get more power! We can reason about generic points such as (x)(x) or (y)(y) which don't exist in variety-land. This is really really cool.