Ehrhart theory of subdivisions and mixed Hodge theory Eric Katz - - PowerPoint PPT Presentation

ehrhart theory of subdivisions and mixed hodge theory
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Ehrhart theory of subdivisions and mixed Hodge theory Eric Katz - - PowerPoint PPT Presentation

Ehrhart theory of subdivisions and mixed Hodge theory Eric Katz (University of Waterloo) joint with Alan Stapledon (University of Sydney) October 26, 2014 Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 1 / 24 A word on


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Ehrhart theory of subdivisions and mixed Hodge theory

Eric Katz (University of Waterloo) joint with Alan Stapledon (University of Sydney) October 26, 2014

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 1 / 24

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A word on contents...

This talk is about Ehrhart theory. The machinery discussed here naturally belongs in the framework of Eulerian posets.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 2 / 24

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A word on contents...

This talk is about Ehrhart theory. The machinery discussed here naturally belongs in the framework of Eulerian posets. And when I think about Eulerian posets, I like to think about:

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 2 / 24

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A word on contents...

This talk is about Ehrhart theory. The machinery discussed here naturally belongs in the framework of Eulerian posets. And when I think about Eulerian posets, I like to think about:

1 Motives Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 2 / 24

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A word on contents...

This talk is about Ehrhart theory. The machinery discussed here naturally belongs in the framework of Eulerian posets. And when I think about Eulerian posets, I like to think about:

1 Motives 2 Intersection cohomology Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 2 / 24

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SLIDE 6

A word on contents...

This talk is about Ehrhart theory. The machinery discussed here naturally belongs in the framework of Eulerian posets. And when I think about Eulerian posets, I like to think about:

1 Motives 2 Intersection cohomology 3 Mixed Hodge theory Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 2 / 24

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Ehrhart polynomials

Let P ⊂ Rn be a lattice polytope. We can encode the lattice point count

  • f dilates of P in the Ehrhart polynomial.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 3 / 24

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Ehrhart polynomials

Let P ⊂ Rn be a lattice polytope. We can encode the lattice point count

  • f dilates of P in the Ehrhart polynomial.

Theorem (Ehrhart) The function LP(m) = |mP ∩ Zn| is a polynomial in m.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 3 / 24

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Ehrhart polynomials

Let P ⊂ Rn be a lattice polytope. We can encode the lattice point count

  • f dilates of P in the Ehrhart polynomial.

Theorem (Ehrhart) The function LP(m) = |mP ∩ Zn| is a polynomial in m. Now, we can produce the h∗-polynomial by considering the Ehrhart series E(u) =

  • m=0

|mP ∩ Zn|um

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 3 / 24

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Ehrhart polynomials

Let P ⊂ Rn be a lattice polytope. We can encode the lattice point count

  • f dilates of P in the Ehrhart polynomial.

Theorem (Ehrhart) The function LP(m) = |mP ∩ Zn| is a polynomial in m. Now, we can produce the h∗-polynomial by considering the Ehrhart series E(u) =

  • m=0

|mP ∩ Zn|um and as a consequence of Ehrhart’s theorem, it can be written as E(u) = h∗(u) (1 − u)dimP+1 where h∗(t) is a polynomial.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 3 / 24

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Ehrhart polynomials

Let P ⊂ Rn be a lattice polytope. We can encode the lattice point count

  • f dilates of P in the Ehrhart polynomial.

Theorem (Ehrhart) The function LP(m) = |mP ∩ Zn| is a polynomial in m. Now, we can produce the h∗-polynomial by considering the Ehrhart series E(u) =

  • m=0

|mP ∩ Zn|um and as a consequence of Ehrhart’s theorem, it can be written as E(u) = h∗(u) (1 − u)dimP+1 where h∗(t) is a polynomial. The h∗-polynomial is a wonderful invariant. It takes simple values on simple things. Its value on the standard simplex is 1.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 3 / 24

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Ehrhart reciprocity

A truly amazing theorem is Ehrhart reciprocity. It relates the generating function for a lattice polytope with that of its interior.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 4 / 24

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Ehrhart reciprocity

A truly amazing theorem is Ehrhart reciprocity. It relates the generating function for a lattice polytope with that of its interior. Theorem (Ehrhart reciprocity) The function LP(m) obeys LP(−m) = (−1)dim PLP◦(m).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 4 / 24

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Ehrhart reciprocity

A truly amazing theorem is Ehrhart reciprocity. It relates the generating function for a lattice polytope with that of its interior. Theorem (Ehrhart reciprocity) The function LP(m) obeys LP(−m) = (−1)dim PLP◦(m). Something to think about (when you get unhappy in this talk, and you will get unhappy):

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 4 / 24

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Ehrhart reciprocity

A truly amazing theorem is Ehrhart reciprocity. It relates the generating function for a lattice polytope with that of its interior. Theorem (Ehrhart reciprocity) The function LP(m) obeys LP(−m) = (−1)dim PLP◦(m). Something to think about (when you get unhappy in this talk, and you will get unhappy): What conditions does Ehrhart reciprocity put on h∗? You can express LP◦ in terms of LQ as Q ranges over faces of P and then use inclusion/exclusion. What does that say about h∗?

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 4 / 24

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Subdivsions

Motivating question: what if we have a lattice subdivision of a lattice polytope? We decompose P into smaller lattice polytopes. How can we enrich Ehrhart theory by incoporating the subdivision?

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 5 / 24

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Subdivsions

Motivating question: what if we have a lattice subdivision of a lattice polytope? We decompose P into smaller lattice polytopes. How can we enrich Ehrhart theory by incoporating the subdivision? Here’s a square being subdivided into two triangles.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 5 / 24

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A geometric avatar for the Ehrhart polynomial

We will try to study subdivisions by relating them to geometry. Let us first study h∗ geometrically. By the work of Danilov-Khovanskii, there’s a geometric interpretation of the h∗-polynomial:

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 6 / 24

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A geometric avatar for the Ehrhart polynomial

We will try to study subdivisions by relating them to geometry. Let us first study h∗ geometrically. By the work of Danilov-Khovanskii, there’s a geometric interpretation of the h∗-polynomial: Let X ◦ = {

u∈M αuxu = 0} ⊂ (C∗)n be a hypersurface. The Newton

polytope P of X ◦ is the convex hull of {u ∈ Zn | αu = 0}. Let us suppose that P is full-dimensional and that X ◦ is non-degenerate with respect to its Newton polytope which means that all of its initial degenerations are smooth.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 6 / 24

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A geometric avatar for the Ehrhart polynomial

We will try to study subdivisions by relating them to geometry. Let us first study h∗ geometrically. By the work of Danilov-Khovanskii, there’s a geometric interpretation of the h∗-polynomial: Let X ◦ = {

u∈M αuxu = 0} ⊂ (C∗)n be a hypersurface. The Newton

polytope P of X ◦ is the convex hull of {u ∈ Zn | αu = 0}. Let us suppose that P is full-dimensional and that X ◦ is non-degenerate with respect to its Newton polytope which means that all of its initial degenerations are smooth. The h∗-polynomial will arise from looking at dimensions of graded pieces

  • f the cohomology with compact support, H∗

c (X ◦).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 6 / 24

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Hodge strucutre

If X ◦ were a compact smooth variety, then its cohomology would have a pure Hodge structure. This implies that there’s a decomposition, Hk(Z) =

  • p+q=k

Hp,q(Z). Write hp,q = dim Hp,q(Z).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 7 / 24

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Hodge strucutre

If X ◦ were a compact smooth variety, then its cohomology would have a pure Hodge structure. This implies that there’s a decomposition, Hk(Z) =

  • p+q=k

Hp,q(Z). Write hp,q = dim Hp,q(Z). It is useful to phrase the decomposition in terms of a decreasing filtration F 0 = Hk ⊃ F1 ⊃ · · · ⊃ Fk such that hp,q = dim Grp

F(Hk).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 7 / 24

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Mixed Hodge structure

The cohomology H∗

c (X ◦) has a mixed Hodge structure which is a technical

way of saying linear algebra is much much harder than you ever thought

  • possible. It arises from picking a smooth compactification X ◦.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 8 / 24

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Mixed Hodge structure

The cohomology H∗

c (X ◦) has a mixed Hodge structure which is a technical

way of saying linear algebra is much much harder than you ever thought

  • possible. It arises from picking a smooth compactification X ◦.

This implies that there is an increasing filtration W and a decreasing filtration F on Hk

c such that the associated gradeds with respect to W

have a pure Hodge structure induced by F. We define hp,q(Hk

c (X ◦)) = dim Grp F GrW p+q(Hk c (X ◦)).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 8 / 24

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Mixed Hodge structure

The cohomology H∗

c (X ◦) has a mixed Hodge structure which is a technical

way of saying linear algebra is much much harder than you ever thought

  • possible. It arises from picking a smooth compactification X ◦.

This implies that there is an increasing filtration W and a decreasing filtration F on Hk

c such that the associated gradeds with respect to W

have a pure Hodge structure induced by F. We define hp,q(Hk

c (X ◦)) = dim Grp F GrW p+q(Hk c (X ◦)).

Warning: Note that we may have hp,q(Hk(Z)) = 0 even though p + q = k. So there’s a lot more data.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 8 / 24

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Danilov-Khovanskii’s approach

To throw out some of the excess data, we take the Hodge-Deligne numbers ep,q(X ◦) =

  • k

(−1)khp,q(Hk

c (X ◦)).

We want to find ep,q.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 9 / 24

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Danilov-Khovanskii’s approach

To throw out some of the excess data, we take the Hodge-Deligne numbers ep,q(X ◦) =

  • k

(−1)khp,q(Hk

c (X ◦)).

We want to find ep,q. First, ep,q(X ◦) is motivic: if U is an open subset of Z then ep,q(X ◦) = ep,q(U) + ep,q(X ◦ \ U).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 9 / 24

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Danilov-Khovanskii’s approach

To throw out some of the excess data, we take the Hodge-Deligne numbers ep,q(X ◦) =

  • k

(−1)khp,q(Hk

c (X ◦)).

We want to find ep,q. First, ep,q(X ◦) is motivic: if U is an open subset of Z then ep,q(X ◦) = ep,q(U) + ep,q(X ◦ \ U). Now, we can form the Hodge-Deligne polynomial, E(X ◦; u, v) =

  • p,q

ep,qupv q

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 9 / 24

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Danilov-Khovanskii’s approach

To throw out some of the excess data, we take the Hodge-Deligne numbers ep,q(X ◦) =

  • k

(−1)khp,q(Hk

c (X ◦)).

We want to find ep,q. First, ep,q(X ◦) is motivic: if U is an open subset of Z then ep,q(X ◦) = ep,q(U) + ep,q(X ◦ \ U). Now, we can form the Hodge-Deligne polynomial, E(X ◦; u, v) =

  • p,q

ep,qupv q It obeys Poincar´ e duality for closed smooth X, E(X; u, v) = (uv)n−1E(X; u−1, v −1).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 9 / 24

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Danilov-Khovanskii’s approach (cont’d)

One has the Lefschetz hyperplane theorem: for k > n − 1, the natural inclusion i : X ◦ → (C∗)n induces an isomorphism of mixed Hodge structures: i∗ : Hk(X ◦) → Hk+1((C∗)n).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 10 / 24

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Danilov-Khovanskii’s approach (cont’d)

One has the Lefschetz hyperplane theorem: for k > n − 1, the natural inclusion i : X ◦ → (C∗)n induces an isomorphism of mixed Hodge structures: i∗ : Hk(X ◦) → Hk+1((C∗)n). So the high degree terms of H∗(X ◦) are controlled by Lefschetz hyperplane and the low-degree terms are controlled (after compactification) by Poincar´ e-duality, so you should only care about the middle dimension.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 10 / 24

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Danilov-Khovanskii’s approach (cont’d)

One has the Lefschetz hyperplane theorem: for k > n − 1, the natural inclusion i : X ◦ → (C∗)n induces an isomorphism of mixed Hodge structures: i∗ : Hk(X ◦) → Hk+1((C∗)n). So the high degree terms of H∗(X ◦) are controlled by Lefschetz hyperplane and the low-degree terms are controlled (after compactification) by Poincar´ e-duality, so you should only care about the middle dimension. We let the primitive cohomology of X ◦ be Hn−1

prim(X ◦) = ker(i∗ : Hn−1(X ◦) → Hn((C∗)n).

The primitive cohomology has a mixed Hodge structure and we can form the E-polynomial.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 10 / 24

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Danilov-Khovanskii’s approach (cont’d)

One has the Lefschetz hyperplane theorem: for k > n − 1, the natural inclusion i : X ◦ → (C∗)n induces an isomorphism of mixed Hodge structures: i∗ : Hk(X ◦) → Hk+1((C∗)n). So the high degree terms of H∗(X ◦) are controlled by Lefschetz hyperplane and the low-degree terms are controlled (after compactification) by Poincar´ e-duality, so you should only care about the middle dimension. We let the primitive cohomology of X ◦ be Hn−1

prim(X ◦) = ker(i∗ : Hn−1(X ◦) → Hn((C∗)n).

The primitive cohomology has a mixed Hodge structure and we can form the E-polynomial. After hard work, we get a formula for χy of the primitive cohomlogy of X ◦: uEprim(X ◦; u, 1) = (−1)dim P+1h∗

P(u).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 10 / 24

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Batyrev-Borisov’s approach

There’s a big downside to the above approach. It’s hard to get a handle

  • n the full E-polynomial. The combinatorics of picking a smooth

compactification is really unmanageable, so let’s follow Batyrev-Borisov and use intersection cohomology which is a technical way of saying no one expects you to read the papers. Less jocularly, it says that we can pretend things are smooth if we keep track of singularities. In the smooth case, it agrees with usual cohomology.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 11 / 24

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Batyrev-Borisov’s approach

There’s a big downside to the above approach. It’s hard to get a handle

  • n the full E-polynomial. The combinatorics of picking a smooth

compactification is really unmanageable, so let’s follow Batyrev-Borisov and use intersection cohomology which is a technical way of saying no one expects you to read the papers. Less jocularly, it says that we can pretend things are smooth if we keep track of singularities. In the smooth case, it agrees with usual cohomology. We have X ◦ ⊂ (C∗)n. We can compactify (C∗)n to P, the toric variety associated to the Newton polytope P. Let X be the closure of X ◦ in P. It may not be smooth but by nondegeneracy, each open strata of X ◦

Q which

is associated to a face Q ⊆ P is smooth.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 11 / 24

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Batyrev-Borisov’s approach

There’s a big downside to the above approach. It’s hard to get a handle

  • n the full E-polynomial. The combinatorics of picking a smooth

compactification is really unmanageable, so let’s follow Batyrev-Borisov and use intersection cohomology which is a technical way of saying no one expects you to read the papers. Less jocularly, it says that we can pretend things are smooth if we keep track of singularities. In the smooth case, it agrees with usual cohomology. We have X ◦ ⊂ (C∗)n. We can compactify (C∗)n to P, the toric variety associated to the Newton polytope P. Let X be the closure of X ◦ in P. It may not be smooth but by nondegeneracy, each open strata of X ◦

Q which

is associated to a face Q ⊆ P is smooth. So there’s a black box IH∗

c (X). It has a lot of good properties like the

Lefschetz hyperplane theorem and Poincar´ e duality, but it is not motivic.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 11 / 24

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Sum-over-strata formula

What replaces motivicity is a sum-over-strata formula that incorporates singularities: Eint(X; u, v) =

  • Q⊆P

Q=∅

Eint(X ◦

Q)g([Q, P]∗; uv).

Here g([Q, P]∗) is the g-polynomial of the dual Eulerian poset [Q, P]∗. It is exactly the same term that enters into the toric h-vector, and it knows about the singularities along strata. We can invert this formula to solve for Eint(X ◦).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 12 / 24

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Sum-over-strata formula

What replaces motivicity is a sum-over-strata formula that incorporates singularities: Eint(X; u, v) =

  • Q⊆P

Q=∅

Eint(X ◦

Q)g([Q, P]∗; uv).

Here g([Q, P]∗) is the g-polynomial of the dual Eulerian poset [Q, P]∗. It is exactly the same term that enters into the toric h-vector, and it knows about the singularities along strata. We can invert this formula to solve for Eint(X ◦). Oh yeah, Ehrhart reciprocity for X ◦ becomes Poincar´ e-duality for Eint,prim(X; u, 1)!

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 12 / 24

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Local h∗-polynomial

And Eint,prim(X; u, 1) is a cool invariant of the polytope P. It’s called the local h∗-polynomial and it is denoted l∗. Here local will always refer to invariants of closed varieties. That’s an unfortunate naming convention that predates the geometric picture. l∗(P; u) =

  • Q⊆P

(−1)dim P−dim Qh∗(Q; u)g([Q, P]∗; u). It is symmetric and its coefficients are manifestly non-negative. It’s also been called the ˜ S-polynomial of P.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 13 / 24

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Local h∗-polynomial

And Eint,prim(X; u, 1) is a cool invariant of the polytope P. It’s called the local h∗-polynomial and it is denoted l∗. Here local will always refer to invariants of closed varieties. That’s an unfortunate naming convention that predates the geometric picture. l∗(P; u) =

  • Q⊆P

(−1)dim P−dim Qh∗(Q; u)g([Q, P]∗; u). It is symmetric and its coefficients are manifestly non-negative. It’s also been called the ˜ S-polynomial of P. To find E(X ◦; u, v), you use Danilov-Khovanskii to find E(X ◦; u, 1), sum-over-strata to find Eint(X; u, 1), use the pure Hodge structure to find E(X; u, v), and then invert the sum-over-strata formula.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 13 / 24

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Degenerating Hypersurfaces

Now, here’s where we get into our work. Subdivided polytopes have a geometric avatar, degenerating hypersurfaces.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 14 / 24

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Degenerating Hypersurfaces

Now, here’s where we get into our work. Subdivided polytopes have a geometric avatar, degenerating hypersurfaces. One can add an auxiliary parameter t and look at f ∈ C((t))[x1, . . . , xn]. Here, we think of t as the coordinate on a punctured disc around 0 and we have a family of hypersurfaces Xt = V (ft) ⊂ (C∗)n.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 14 / 24

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Degenerating Hypersurfaces

Now, here’s where we get into our work. Subdivided polytopes have a geometric avatar, degenerating hypersurfaces. One can add an auxiliary parameter t and look at f ∈ C((t))[x1, . . . , xn]. Here, we think of t as the coordinate on a punctured disc around 0 and we have a family of hypersurfaces Xt = V (ft) ⊂ (C∗)n. Silly example: Let f (x1, x2) = 1 + x1 + x2 + tx1x2.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 14 / 24

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Degenerating Hypersurfaces

Now, here’s where we get into our work. Subdivided polytopes have a geometric avatar, degenerating hypersurfaces. One can add an auxiliary parameter t and look at f ∈ C((t))[x1, . . . , xn]. Here, we think of t as the coordinate on a punctured disc around 0 and we have a family of hypersurfaces Xt = V (ft) ⊂ (C∗)n. Silly example: Let f (x1, x2) = 1 + x1 + x2 + tx1x2. For t = 0, this is a conic that naturally compactifies to a (1, 1)-curve in P1 × P1, so a four-times punctured P1.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 14 / 24

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Degenerating Hypersurfaces

Now, here’s where we get into our work. Subdivided polytopes have a geometric avatar, degenerating hypersurfaces. One can add an auxiliary parameter t and look at f ∈ C((t))[x1, . . . , xn]. Here, we think of t as the coordinate on a punctured disc around 0 and we have a family of hypersurfaces Xt = V (ft) ⊂ (C∗)n. Silly example: Let f (x1, x2) = 1 + x1 + x2 + tx1x2. For t = 0, this is a conic that naturally compactifies to a (1, 1)-curve in P1 × P1, so a four-times punctured P1. As t goes to 0, our cur ambient P1 × P1 degenerates to two P2’s joined along a line. Our curve degenerates into two twice-punctured lines joined along a node.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 14 / 24

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Newton subdivision

There’s a combinatorial object associated to degenerating hypersurfaces, the Newton subdivision.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 15 / 24

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Newton subdivision

There’s a combinatorial object associated to degenerating hypersurfaces, the Newton subdivision. Let f ∈ C((t))[x1, . . . , xn]. Write f =

  • auxu.

For au ∈ C((t)), let val(au) be the smallest exponent of t with non-zero

  • coefficient. Consider the function

u → val(au).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 15 / 24

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SLIDE 48

Newton subdivision

There’s a combinatorial object associated to degenerating hypersurfaces, the Newton subdivision. Let f ∈ C((t))[x1, . . . , xn]. Write f =

  • auxu.

For au ∈ C((t)), let val(au) be the smallest exponent of t with non-zero

  • coefficient. Consider the function

u → val(au). The upper hull is the convex hull of all points lying above the graph of this

  • function. Its lower faces induce a subdivision of P. Subdivisions that arise

in this fashion are called regular.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 15 / 24

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SLIDE 49

Newton subdivision

There’s a combinatorial object associated to degenerating hypersurfaces, the Newton subdivision. Let f ∈ C((t))[x1, . . . , xn]. Write f =

  • auxu.

For au ∈ C((t)), let val(au) be the smallest exponent of t with non-zero

  • coefficient. Consider the function

u → val(au). The upper hull is the convex hull of all points lying above the graph of this

  • function. Its lower faces induce a subdivision of P. Subdivisions that arise

in this fashion are called regular. Regular subdivisions can be studied as an object like Newton polytopes.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 15 / 24

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Example of Newton subdivision

Example: Let us consider f (x1, x2) = 1 + x1 + x2 + tx1x2. Here is the function and its associated subdivision.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 16 / 24

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Example of Newton subdivision

Example: Let us consider f (x1, x2) = 1 + x1 + x2 + tx1x2. Here is the function and its associated subdivision. 1 Here you can see the ambient P1 × P1 degenerating into two P2’s joined along a P1.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 16 / 24

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Example of Newton subdivision

Example: Let us consider f (x1, x2) = 1 + x1 + x2 + tx1x2. Here is the function and its associated subdivision. 1 Here you can see the ambient P1 × P1 degenerating into two P2’s joined along a P1. In general, under an appropriate non-degeneracy condition, one can complete the family over the puncture. Then the central fiber X ◦

0 is

stratified by open varieties X ◦

F corresponding to cells F in the interior of P.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 16 / 24

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Monodromy Filtration

If we have a family X ◦

t , there is an additional filtration on the cohomology.

View the family over the punctured disc. The cohomology H∗

c (X ◦ t ) gives a

locally trivial fiber bundle over the punctured disc. Consequently, one can parallel transport around the puncture.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 17 / 24

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Monodromy Filtration

If we have a family X ◦

t , there is an additional filtration on the cohomology.

View the family over the punctured disc. The cohomology H∗

c (X ◦ t ) gives a

locally trivial fiber bundle over the punctured disc. Consequently, one can parallel transport around the puncture. This gives a monodromy operation T : H∗

c (X ◦ t ) → H∗ c (X ◦ t ).

By possibly replacing T by T m for some m ∈ Z≥1, we can suppose T is

  • unipotent. Set N = log(T) which is nilpotent. There is an additional

filtration coming from the Jordan decomposition of N.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 17 / 24

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SLIDE 55

Monodromy Filtration

If X ◦

t were compact, then one could put an increasing monodromy

filtration M on Hk(X ◦

t ),

0 ⊆ M0 ⊆ M1 ⊆ · · · ⊆ M2k = Hk

c (X ◦),

with associated graded pieces GrM

l

:= Ml/Ml−1, satisfying the following properties for any non-negative integer l,

1 N(Ml) ⊆ Ml−2, 2 the induced map Nl : GrM

k+l → GrM k−l is an isomorphism.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 18 / 24

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SLIDE 56

Monodromy Filtration

If X ◦

t were compact, then one could put an increasing monodromy

filtration M on Hk(X ◦

t ),

0 ⊆ M0 ⊆ M1 ⊆ · · · ⊆ M2k = Hk

c (X ◦),

with associated graded pieces GrM

l

:= Ml/Ml−1, satisfying the following properties for any non-negative integer l,

1 N(Ml) ⊆ Ml−2, 2 the induced map Nl : GrM

k+l → GrM k−l is an isomorphism.

These conditions (which look like the Lefschetz hyperplane theorem) put a unimodality condition on the ranks of GrM

l .

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 18 / 24

slide-57
SLIDE 57

Monodromy Filtration

If X ◦

t were compact, then one could put an increasing monodromy

filtration M on Hk(X ◦

t ),

0 ⊆ M0 ⊆ M1 ⊆ · · · ⊆ M2k = Hk

c (X ◦),

with associated graded pieces GrM

l

:= Ml/Ml−1, satisfying the following properties for any non-negative integer l,

1 N(Ml) ⊆ Ml−2, 2 the induced map Nl : GrM

k+l → GrM k−l is an isomorphism.

These conditions (which look like the Lefschetz hyperplane theorem) put a unimodality condition on the ranks of GrM

l .

This monodromy filtration together with the Hodge filtration produces the limit mixed Hodge strucutre.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 18 / 24

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SLIDE 58

Mixed Monodromy Filtration

Since X ◦

t is not compact, we have to do something different.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 19 / 24

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SLIDE 59

Mixed Monodromy Filtration

Since X ◦

t is not compact, we have to do something different.

By results of Steenbrink-Zucker, there is an increasing monodromy filtration M on Hk

c (Zt) and an increasing weight filtration W and a

decreasing Hodge filtration F.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 19 / 24

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SLIDE 60

Mixed Monodromy Filtration

Since X ◦

t is not compact, we have to do something different.

By results of Steenbrink-Zucker, there is an increasing monodromy filtration M on Hk

c (Zt) and an increasing weight filtration W and a

decreasing Hodge filtration F. (A twist of) the monodromy filtration has the above properties on the W -associated gradeds.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 19 / 24

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SLIDE 61

Mixed Monodromy Filtration

Since X ◦

t is not compact, we have to do something different.

By results of Steenbrink-Zucker, there is an increasing monodromy filtration M on Hk

c (Zt) and an increasing weight filtration W and a

decreasing Hodge filtration F. (A twist of) the monodromy filtration has the above properties on the W -associated gradeds. This gives us tons of structure. We can refine the Hodge numbers even further: hp,q,r(Z)k = dim(Grp

F GrM(r) p+q GrW r Hk(Z)).

and form refined Hodge-Deligne numbers: ep,q,r(Z) =

  • (−1)khp,q,r(Z)k.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 19 / 24

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SLIDE 62

Bittner’s Motivic Nearby Fiber

We can write down Hodge-Deligne polynomials with respect to (F, W ), (F, M), and an even monster three-variable Hodge-Deligne polynomial incorporating F, W , M.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 20 / 24

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SLIDE 63

Bittner’s Motivic Nearby Fiber

We can write down Hodge-Deligne polynomials with respect to (F, W ), (F, M), and an even monster three-variable Hodge-Deligne polynomial incorporating F, W , M. There’s a nice formula for the Hodge-Deligne polynomial E(X∞; u, v) with respect to the limit mixed Hodge structure. It arises from Steenbrink’s spectral sequence but was put in particularly appealing form by the work

  • f Bittner:

E(X ◦

∞; u, v) =

  • F⊂P◦

E(X ◦

F; u, v)(1 − uv)n−dim F.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 20 / 24

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SLIDE 64

Bittner’s Motivic Nearby Fiber

We can write down Hodge-Deligne polynomials with respect to (F, W ), (F, M), and an even monster three-variable Hodge-Deligne polynomial incorporating F, W , M. There’s a nice formula for the Hodge-Deligne polynomial E(X∞; u, v) with respect to the limit mixed Hodge structure. It arises from Steenbrink’s spectral sequence but was put in particularly appealing form by the work

  • f Bittner:

E(X ◦

∞; u, v) =

  • F⊂P◦

E(X ◦

F; u, v)(1 − uv)n−dim F.

Note that on the left-hand side, we use the limit mixed Hodge structure while on the right, we use the usual mixed Hodge structure. And we can compute this.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 20 / 24

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SLIDE 65

Refined invariants

And now, if we want to compute more refined invariants, we can invoke intersection cohomology magic. By a result of Saito (in French and in Saito), the compactly-supported intersection cohomology of the family X ◦

t

carries the appropriate refined limit mixed Hodge structure (F, W , M).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 21 / 24

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SLIDE 66

Refined invariants

And now, if we want to compute more refined invariants, we can invoke intersection cohomology magic. By a result of Saito (in French and in Saito), the compactly-supported intersection cohomology of the family X ◦

t

carries the appropriate refined limit mixed Hodge structure (F, W , M). The analogous sum-over-strata formula holds. So we can compactify to

  • Xt. Then (F, M) is a pure Hodge structure with all the interesting

primitive stuff in middle dimension. Then, we folow the same recipe as before, and we write down E(X ◦; u, v, w). Or just concentrate on the primitve cohomology, Eprim(X ◦; u, v, w).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 21 / 24

slide-67
SLIDE 67

Refined invariants

And now, if we want to compute more refined invariants, we can invoke intersection cohomology magic. By a result of Saito (in French and in Saito), the compactly-supported intersection cohomology of the family X ◦

t

carries the appropriate refined limit mixed Hodge structure (F, W , M). The analogous sum-over-strata formula holds. So we can compactify to

  • Xt. Then (F, M) is a pure Hodge structure with all the interesting

primitive stuff in middle dimension. Then, we folow the same recipe as before, and we write down E(X ◦; u, v, w). Or just concentrate on the primitve cohomology, Eprim(X ◦; u, v, w). This three-variable polynomial has tons of structure. Its coefficients are ranks of graded bits (wrt (F, W , M)) and so are non-negative. On the closed analogue, there are symmetry properties coming from Poincar´ e

  • daulity. It has unimodality properties coming from N.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 21 / 24

slide-68
SLIDE 68

Refined invariants

And now, if we want to compute more refined invariants, we can invoke intersection cohomology magic. By a result of Saito (in French and in Saito), the compactly-supported intersection cohomology of the family X ◦

t

carries the appropriate refined limit mixed Hodge structure (F, W , M). The analogous sum-over-strata formula holds. So we can compactify to

  • Xt. Then (F, M) is a pure Hodge structure with all the interesting

primitive stuff in middle dimension. Then, we folow the same recipe as before, and we write down E(X ◦; u, v, w). Or just concentrate on the primitve cohomology, Eprim(X ◦; u, v, w). This three-variable polynomial has tons of structure. Its coefficients are ranks of graded bits (wrt (F, W , M)) and so are non-negative. On the closed analogue, there are symmetry properties coming from Poincar´ e

  • daulity. It has unimodality properties coming from N.

For example, we immediately get the theorem that if a lattice polytope P has a regular unimodular subdivision, then l∗(P; u) is unimodal.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 21 / 24

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SLIDE 69

Back to combinatoricsl

We can define all of these invariants combinatorially. Let S be a lattice polyhedral subdivision of a lattice polytope P. Then the limit mixed h∗-polynomial of (P, S) is h∗(P, S; u, v) :=

  • F∈S

v dim F+1l∗(F; uv −1)h(lkS(F); uv). where h is the h-polynomial of an Eulerian poset.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 22 / 24

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SLIDE 70

Back to combinatoricsl

We can define all of these invariants combinatorially. Let S be a lattice polyhedral subdivision of a lattice polytope P. Then the limit mixed h∗-polynomial of (P, S) is h∗(P, S; u, v) :=

  • F∈S

v dim F+1l∗(F; uv −1)h(lkS(F); uv). where h is the h-polynomial of an Eulerian poset. The local limit mixed h∗-polynomial of (P, S) is l∗(P, S; u, v) :=

  • Q⊆P

(−1)dim P−dim Qh∗(Q, S|Q; u, v)g([Q, P]∗; uv).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 22 / 24

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SLIDE 71

Back to combinatoricsl

We can define all of these invariants combinatorially. Let S be a lattice polyhedral subdivision of a lattice polytope P. Then the limit mixed h∗-polynomial of (P, S) is h∗(P, S; u, v) :=

  • F∈S

v dim F+1l∗(F; uv −1)h(lkS(F); uv). where h is the h-polynomial of an Eulerian poset. The local limit mixed h∗-polynomial of (P, S) is l∗(P, S; u, v) :=

  • Q⊆P

(−1)dim P−dim Qh∗(Q, S|Q; u, v)g([Q, P]∗; uv). The refined limit mixed h∗-polynomial of (P, S) is h∗(P, S; u, v, w) =

  • Q⊆P

wdim Q+1l∗(Q, S|Q; u, v)g([Q, P]; uvw2).

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 22 / 24

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SLIDE 72

Disclaimer

Our machinery is very general. It works for Eulerian posets. We can plug in different things instead of h∗.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 23 / 24

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SLIDE 73

Disclaimer

Our machinery is very general. It works for Eulerian posets. We can plug in different things instead of h∗. If instead of plugging in h∗, we plugged in the cohomology of (C∗)n, we are studying the intersection cohomology of toric varieties, and we get things like h-polynomials.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 23 / 24

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SLIDE 74

Disclaimer

Our machinery is very general. It works for Eulerian posets. We can plug in different things instead of h∗. If instead of plugging in h∗, we plugged in the cohomology of (C∗)n, we are studying the intersection cohomology of toric varieties, and we get things like h-polynomials. If we have a sch¨

  • n subvariety of (K∗)n for a valued field K, we can plug in

its intersection cohomology. Then we have a way of keeping track of the graded bits of its limit mixed Hodge strucutre.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 23 / 24

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SLIDE 75

Thanks!

  • K. and Alan Stapledon, Tropical geometry, the motivic nearby fiber and

limit mixed Hodge numbers of hypersurfaces, arXiv:1404.3000. Eric Katz and Alan Stapledon, Local h-polynomials and the Ehrhart theory

  • f lattice subdivisions, in progress.

Eric Katz (Waterloo) Mixed Ehrhart Theory October 26, 2014 24 / 24