In mathematics, the Noether normalization lemma is a result of commutative algebra, introduced by Emmy Noether in 1926. It states that for any field k, and any finitely generated commutative k-algebra A, there exist elements y1, y2, ..., yd in A that are algebraically independent over k and such that A is a finitely generated module over the polynomial ring S = k[''y''<sub>1</sub>, ''y''<sub>2</sub>, ..., ''y''<sub>''d''</sub>]. The integer d is equal to the Krull dimension of the ring A; and if A is an integral domain, d is also the transcendence degree of the field of fractions of A over k.
d | |
A | |
k |
S\hookrightarrowA
X\to
d | |
A | |
k |
More generally, in the language of schemes, the theorem can equivalently be stated as: every affine k-scheme (of finite type) X is finite over an affine n-dimensional space. The theorem can be refined to include a chain of ideals of R (equivalently, closed subsets of X) that are finite over the affine coordinate subspaces of the corresponding dimensions.
The Noether normalization lemma can be used as an important step in proving Hilbert's Nullstellensatz, one of the most fundamental results of classical algebraic geometry. The normalization theorem is also an important tool in establishing the notions of Krull dimension for k-algebras.
The following proof is due to Nagata, following Mumford's red book. A more geometric proof is given on page 127 of the red book.
The ring A in the lemma is generated as a k-algebra by some elements
y1,...,ym
m=0
k=A
m=1
A\congk[y]/I
I\subsetk[y]
k[y]
I=(f)
f=0
f ≠ 0
1,y,y2,...,ye-1
m\geq2
m-1
x1,...,xd
k[x1,...,xd]
Since otherwise there would be nothing to prove, we can also assume that there is a nonzero polynomial f in m variables over k such that
f(y1,\ldots,ym)=0
zi=yi-
ri-1 | |
y | |
1 |
, 2\lei\lem.
f(y1,z2+
r, | |
y | |
1 |
z3+
r2 | |
y | |
1 |
,\ldots,zm+
rm-1 | |
y | |
1 |
)=0
a
\alpha1 | |
y | |
1 |
m | |
\prod | |
2 |
(zi+
ri-1 | |
y | |
1 |
\alphai | |
) |
a\ink
y1
a
\alpha1+r\alpha2+ … +\alphamrm-1 | |
y | |
1 |
.
y1
y1
f(y1,z2+
r, | |
y | |
1 |
z3+
r2 | |
y | |
1 |
,...,zm+
rm-1 | |
y | |
1 |
)
\alpha1+r\alpha2+ … +\alphamrm-1
c\ink
(\alpha1,...,\alpham)
\alpha1+r\alpha2+ … +\alphamrm-1
1/c
y1
S=k[z2,...,zm]
y1
yi=zi+
ri-1 | |
y | |
1 |
If A is an integral domain, then d is the transcendence degree of its field of fractions. Indeed, A and
S=k[y1,...,yd]
d=0
0\subsetneq(y1)\subsetneq(y1,y2)\subsetneq … \subsetneq(y1,...,yd)
0\subsetneqak{p}1\subsetneq … \subsetneqak{p}m
0\neu\inak{p}1
T=k[u,z2,...,zd]
T/(u)
ak{p}i\capT
m
T/(ak{p}1\capT)
m-1
\operatorname{dim}T/(ak{p}1\capT)\le\operatorname{dim}T/(u)
m-1\led-1
\dimS\led
The following refinement appears in Eisenbud's book, which builds on Nagata's idea: