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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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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