Toric Varieties: From Fans to Cones in Algebraic Geometry, Study notes of Mathematics

In this lecture, algebraic geometry professor joe grant explores the relationship between toric varieties and their associated fans. Starting with a lattice n ∼= z2 and a two-dimensional cone σ, the professor derives the dual cone σ∨ and its semigroup sσ. The semigroup algebra csσ is then defined, and a ring homomorphism from c[u, v, w] to csσ is established. The lecture concludes with the definition of uσ, the toric variety associated with σ.

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2010/2011

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Algebraic Geometry Lecture 24 Toric Varieties
Joe Grant1
Last week we went
Toric variety (Toric) fan.
This week we go the other way.
Let our lattice be N
=Z2. Consider the two-dimensional cone σgenerated by (0,1) and (2,1).
Find the dual cone σM=N= Hom(N, Z). Mhas a basis of functionals h1, h2that we’ll
write as h1= (1,0) and h2= (0,1). The dual cone is
{mM:m(s)>0 for every sσ}.
These are the “vectors in Mat most orthogonal to everything in N”. To see σit helps to tensor
with R.
Over R,σRis generated by (1,2) and (1,0). But σitself (which is really M“the dual of
σ”) has three generators, (1,0),(1,2), and (1,1). This gives the semigroup associated to σ, called
Sσ. (If it comes from a fan then it’s finitely generated by Gordon’s theorem.)
Write this group multiplicatively, so (a, b)·(c, d) = (a+c, b +d). Then we can form the
semigroup algebra CSσwhose elements are linear combinations of elements of Sσwith the induced
multiplication.
pRecall group algebras: Let Gbe a finite group, then elements of CGlook like λ1g1+. . . +λngn,
and we multiply them by, for example,
(5g1+ 2g2)(3g3)=53g1g3+ 23g2g3.
Semigroup algebras work the same way.
y
If we write X= (1,0), Y = (0,1), we see Sσhas generators
X, X Y, XY 2.
So CSσ=C[X, X Y, XY 2]. We define a ring homomorphism
C[u, v, w]CSσ
by
u7→ X v 7→ XY w 7→ XY 2.
This is clearly surjective and has kernel huw v2i, so by the first isomorphism theorem,
CSσ
=C[u, v, w]/(uw v2).
Finally to get our toric variety we let
Uσ= Spec CSσ,
then we can see that Uσ={(u, v, w)C3:uw v2= 0}.
1Typed by Lee Butler
1

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Algebraic Geometry Lecture 24 – Toric Varieties

Joe Grant^1

Last week we went Toric variety −→ (Toric) fan.

This week we go the other way.

Let our lattice be N ∼= Z^2. Consider the two-dimensional cone σ generated by (0, 1) and (2, −1). Find the dual cone σ∨^ ⊂ M = N ∨^ = Hom(N, Z). M has a basis of functionals h 1 , h 2 that we’ll write as h 1 = (1, 0) and h 2 = (0, 1). The dual cone is

{m ∈ M : m(s) > 0 for every s ∈ σ}.

These are the “vectors in M at most orthogonal to everything in N ”. To see σ∨^ it helps to tensor with R.

Over R, σ∨^ ⊗ R is generated by (1, 2) and (1, 0). But σ∨^ itself (which is really M ∩“the dual of σ”) has three generators, (1, 0), (1, 2), and (1, 1). This gives the semigroup associated to σ∨, called Sσ. (If it comes from a fan then it’s finitely generated by Gordon’s theorem.)

Write this group multiplicatively, so (a, b) · (c, d) = (a + c, b + d). Then we can form the semigroup algebra CSσ whose elements are linear combinations of elements of Sσ with the induced multiplication.

p Recall group algebras: Let G be a finite group, then elements of CG look like λ 1 g 1 +... + λngn, and we multiply them by, for example,

(5g 1 + 2g 2 )(

− 3 g 3 ) = 5

− 3 g 1 g 3 + 2

− 3 g 2 g 3.

Semigroup algebras work the same way.

y

If we write X = (1, 0), Y = (0, 1), we see Sσ has generators X, XY, XY 2.

So CSσ = C[X, XY, XY 2 ]. We define a ring homomorphism

C[u, v, w] → CSσ

by u 7 → X v 7 → XY w 7 → XY 2.

This is clearly surjective and has kernel 〈uw − v^2 〉, so by the first isomorphism theorem,

CSσ ∼= C[u, v, w]/(uw − v^2 ).

Finally to get our toric variety we let

Uσ = Spec CSσ ,

then we can see that Uσ = {(u, v, w) ∈ C^3 : uw − v^2 = 0}.

(^1) Typed by Lee Butler 1