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Lattice Simplices of Bounded Degree Einstein Workshop on Lattice - - PowerPoint PPT Presentation

Lattice Simplices of Bounded Degree Einstein Workshop on Lattice Polytopes 2016 Johannes Hofscheier Otto-von-Guericke-Universit at Magdeburg joint with Akihiro Higashitani Tuesday 13 December 2016 Motivation LLS LSD Deg. 2 Appl. Basic


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SLIDE 1

Otto-von-Guericke-Universit¨ at Magdeburg joint with Akihiro Higashitani

Lattice Simplices of Bounded Degree

Einstein Workshop on Lattice Polytopes 2016 Johannes Hofscheier Tuesday 13 December 2016

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SLIDE 2

Motivation LLS LSD

  • Deg. 2

Appl.

Basic Definitions

Lattice polytope: P = conv(v1, . . . , vn) ⊆ Rd where vi ∈ Zd.

  • Ehrhart polynomial: LP (k) :=
  • kP ∩ Zd

(k ∈ Z≥0). h∗-polynomial:

k≥0 LP (k)tk = h∗

P (t)

(1−t)d+1 for h∗ P ∈ Z≥0[t].

degree of P: deg(P) = deg h∗

P (t).

Johannes Hofscheier LSD

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SLIDE 3

Motivation LLS LSD

  • Deg. 2

Appl.

Motivation

Question A

What are the polynomials which can be interpreted as the h∗-polynomial of a lattice polytope?

Johannes Hofscheier LSD

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SLIDE 4

Motivation LLS LSD

  • Deg. 2

Appl.

Linear Polynomials

P = [0, a] ⊆ R (a ∈ Z) LP (0) = 1

Johannes Hofscheier LSD

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SLIDE 5

Motivation LLS LSD

  • Deg. 2

Appl.

Linear Polynomials

P = [0, a] ⊆ R (a ∈ Z) LP (0) = 1, LP (1) = a + 1

Johannes Hofscheier LSD

slide-6
SLIDE 6

Motivation LLS LSD

  • Deg. 2

Appl.

Linear Polynomials

P = [0, a] ⊆ R (a ∈ Z) LP (0) = 1, LP (1) = a + 1, LP (2) = 2a + 1

Johannes Hofscheier LSD

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SLIDE 7

Motivation LLS LSD

  • Deg. 2

Appl.

Linear Polynomials

P = [0, a] ⊆ R (a ∈ Z) LP (0) = 1, LP (1) = a + 1, LP (2) = 2a + 1, LP (3) = 3a + 1, . . .

Johannes Hofscheier LSD

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SLIDE 8

Motivation LLS LSD

  • Deg. 2

Appl.

Linear Polynomials

P = [0, a] ⊆ R (a ∈ Z) LP (0) = 1, LP (1) = a + 1, LP (2) = 2a + 1, LP (3) = 3a + 1, . . . ⇒ LP (k) = ka + 1

  • k≥0

(ka + 1)tk = a

  • k≥0

ktk +

  • k≥0

tk = a

t (1−t)2 + 1 1−t

= (a−1)t+1

(1−t)2

⇒ h∗

P (t) = (a − 1)t + 1.

Degree 1

All lin. polynomials 1 + at ∈ Z2

≥0[t] can be interpreted as h∗-vectors.

Johannes Hofscheier LSD

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SLIDE 9

Motivation LLS LSD

  • Deg. 2

Appl.

Quadratic Polynomials

Degree 2[Henk & Tagami, Treutlein]

All polynomials 1 + a1t + a2t2 ∈ Z≥0[t] with a1 ≤

  • 7

if a2 = 1 3a2 + 3 if a2 ≥ 2 can be interpreted as h∗-polynomials. (Need polytopes up to dimension 3.)

Johannes Hofscheier LSD

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SLIDE 10

Motivation LLS LSD

  • Deg. 2

Appl.

Simpler Question

Question B

What are the h∗-polynomials coming from lattice simplices?

Johannes Hofscheier LSD

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SLIDE 11

Motivation LLS LSD

  • Deg. 2

Appl.

Question B: Degree 1

All lin. polynomials 1 + at ∈ Z≥0[t] can be interpreted as h∗-polynomials of lattice simplices.

Johannes Hofscheier LSD

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SLIDE 12

Motivation LLS LSD

  • Deg. 2

Appl.

Question B: Degree 2

Interpret h∗ = 1 + a1t + a2t2 ∈ Z≥0[t] as point in the positive

  • rthant a = (a1, a2) ∈ R2

≥0.

M := {a ∈ Z2

≥0 : h∗ P (t)=1+a1t+a2t2 for lattice triangle P ⊆ R2}

Proposition[H.,Nill,Oeberg]

There is a family (σi)i∈Z≥0 of affine cones σi ⊆ R2

≥0 such that

M ∩ σ◦

i = ∅ for all i.

Johannes Hofscheier LSD

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SLIDE 13

Motivation LLS LSD

  • Deg. 2

Appl.

Question B: Degree 2

50 100 150 200 250 50 100 150 200 250 σ1 σ2 σ3 σ0 h∗

1

h∗

2

Johannes Hofscheier LSD

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SLIDE 14

Motivation LLS LSD

  • Deg. 2

Appl.

Simplices of given degree

Question C

What are the simplices of a given degree (any dimension)? Idea: Question C ⇒ Question B.

Johannes Hofscheier LSD

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SLIDE 15

Motivation LLS LSD

  • Deg. 2

Appl.

Idea from Alg. Geom.

  • Alg. Geometer are interested in

Mg,n = {smooth proj. curves C of genus g with n distinct marked points}/ ∼

Johannes Hofscheier LSD

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SLIDE 16

Motivation LLS LSD

  • Deg. 2

Appl.

Idea from Alg. Geom.

  • Alg. Geometer are interested in

Mg,n = {smooth proj. curves C of genus g with n distinct marked points}/ ∼ Completeness is a desirable property. For a (possible) compactification, relax the smoothness condition Mg,n = {proj. connected nodal curves C of genus g with n distinct,

  • nonsing. marked points with a stability condition}/ ∼

Johannes Hofscheier LSD

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SLIDE 17

Motivation LLS LSD

  • Deg. 2

Appl.

“Moduli” of Lattice Simplices

We are interested in M0,s = {lattice simplices ∆ of deg. s with marked vertices}/ ∼ Here “∼” means: “up to affine unimodular transformations”.

Johannes Hofscheier LSD

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SLIDE 18

Motivation LLS LSD

  • Deg. 2

Appl.

“Moduli” of Lattice Simplices

We are interested in M0,s = {lattice simplices ∆ of deg. s with marked vertices}/ ∼ Here “∼” means: “up to affine unimodular transformations”. “genus 0” as a simplex is homeomorphic to a sphere.

Johannes Hofscheier LSD

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SLIDE 19

Motivation LLS LSD

  • Deg. 2

Appl.

“Moduli” of Lattice Simplices

We are interested in M0,s = {lattice simplices ∆ of deg. s with marked vertices}/ ∼ Here “∼” means: “up to affine unimodular transformations”. “genus 0” as a simplex is homeomorphic to a sphere.

Question

What could be M0,s?

Johannes Hofscheier LSD

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SLIDE 20

Motivation LLS LSD

  • Deg. 2

Appl.

Recall Definition

Usually: ∆ = conv(v1, . . . , vd+1) ⊆ Rd d-dimensional lattice simplex if vi ∈ Zd (aff. indep.)

Johannes Hofscheier LSD

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SLIDE 21

Motivation LLS LSD

  • Deg. 2

Appl.

Recall Definition

Usually: ∆ = conv(v1, . . . , vd+1) ⊆ Rd d-dimensional lattice simplex if vi ∈ Zd (aff. indep.) Lattice stays the same: Zd.

Johannes Hofscheier LSD

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SLIDE 22

Motivation LLS LSD

  • Deg. 2

Appl.

Recall Definition

Usually: ∆ = conv(v1, . . . , vd+1) ⊆ Rd d-dimensional lattice simplex if vi ∈ Zd (aff. indep.) Lattice stays the same: Zd. Vertices change: v1, . . . , vd+1.

Johannes Hofscheier LSD

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SLIDE 23

Motivation LLS LSD

  • Deg. 2

Appl.

Recall Definition

Usually: ∆ = conv(v1, . . . , vd+1) ⊆ Rd d-dimensional lattice simplex if vi ∈ Zd (aff. indep.) Lattice stays the same: Zd. Vertices change: v1, . . . , vd+1.

Idea

Let’s do it vice versa. Lattice changes: Λ. Vertices stay the same: What is a good choice?

Johannes Hofscheier LSD

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SLIDE 24

Motivation LLS LSD

  • Deg. 2

Appl.

Lattice of a Lattice Simplex

From now on: e1, . . . , ed ∈ Rd standard basis vectors. All vertices should be “equivalent” bad choice: 0, e1, . . . , ed. Better choice: e1, . . . , ed+1 ∈ Rd+1 (Dimension increases by 1).

Johannes Hofscheier LSD

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SLIDE 25

Motivation LLS LSD

  • Deg. 2

Appl.

Lattice of a Lattice Simplex

∆ = conv(v1, . . . , vd+1) ⊆ Rd d-dimensional lattice simplex. Cone

  • ver ∆

C = cone({1} × ∆) ⊆ Rd+1. Exists unique linear iso. ϕ: Rd+1 → Rd+1 with (1, vi) → ei. ϕ(∆) = conv(e1, . . . , ed+1) Λ∆ := ϕ(Zd+1) ⊆ Rd lattice

Johannes Hofscheier LSD

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SLIDE 26

Motivation LLS LSD

  • Deg. 2

Appl.

Example

∆ = conv(0, 2e1, 2e2) ⊆ R2 1 −1/2 −1/2

1/2 1/2

  • ϕ

1 1 1

0 2 0 0 0 2

  • =

1 0 0

0 1 0 0 0 1

  • Λ∆ = Z3 + Z

−1

2 1 2

  • + Z

−1

2 1 2

  • Johannes Hofscheier

LSD

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SLIDE 27

Motivation LLS LSD

  • Deg. 2

Appl.

Example

∆ = conv(0, 2e1, 2e2) ⊆ R2 1 −1/2 −1/2

1/2 1/2

  • ϕ

1 1 1

0 2 0 0 0 2

  • =

1 0 0

0 1 0 0 0 1

  • Λ∆ = Z3 + Z

−1

2 1 2

  • + Z

−1

2 1 2

  • short:
  • −1/2 1/2

−1/2 1/2

  • Johannes Hofscheier

LSD

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SLIDE 28

Motivation LLS LSD

  • Deg. 2

Appl.

Properties of Λ∆

Proposition

∆ = conv(v1, . . . , vd+1) ⊆ Rd d-dim. lattice simplex. ϕ: Rd+1 → Rd+1; ϕ(1, vi) = ei. Λ∆ = ϕ

  • Zd+1

.

1 Zd+1 ⊆ Λ∆ 2 Λ∆ ⊆

  • x ∈ Rd+1 : d+1

i=1 xi ∈ Z

  • .

Johannes Hofscheier LSD

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SLIDE 29

Motivation LLS LSD

  • Deg. 2

Appl.

Properties of Λ∆

Proposition

∆ = conv(v1, . . . , vd+1) ⊆ Rd d-dim. lattice simplex. ϕ: Rd+1 → Rd+1; ϕ(1, vi) = ei. Λ∆ = ϕ

  • Zd+1

.

1 Zd+1 ⊆ Λ∆ 2 Λ∆ ⊆

  • x ∈ Rd+1 : d+1

i=1 xi ∈ Z

  • .

Idea of Proof:

1 vi ∈ Zd ⇒ Zd+1 ⊆ Λ∆ 2

ϕ

− → ϕ(∆)

Johannes Hofscheier LSD

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SLIDE 30

Motivation LLS LSD

  • Deg. 2

Appl.

Correspondence

Definition

A lattice Λ∆ ⊆ Rd+1 we call simplicial if

1 Zd+1 ⊆ Λ∆. 2 Λ∆ ⊆

  • x ∈ Rd+1 : d+1

i=1 xi ∈ Z

  • .

Johannes Hofscheier LSD

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SLIDE 31

Motivation LLS LSD

  • Deg. 2

Appl.

Correspondence

Definition

A lattice Λ∆ ⊆ Rd+1 we call simplicial if

1 Zd+1 ⊆ Λ∆. 2 Λ∆ ⊆

  • x ∈ Rd+1 : d+1

i=1 xi ∈ Z

  • .

Theorem

The assignment ∆ → Λ∆ induces a bijection d-dim. lattice sim- plices ∆ ⊆ Rd

  • / ∼1↔

simplicial lattices Λ ⊆ Rd+1

  • / ∼2

1 ∼1= up to affine unimodular equivalence 2 ∼2= up to permutation of the coordinates Johannes Hofscheier LSD

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SLIDE 32

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

Cℓ := {C ⊆ X closed subgroup} X :=

  • x ∈ Rd+1 : d+1

i=1 xi ∈ Z

  • ⊆ Rd+1 closed subgp.

Johannes Hofscheier LSD

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SLIDE 33

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

Cℓ := {C ⊆ X closed subgroup} X :=

  • x ∈ Rd+1 : d+1

i=1 xi ∈ Z

  • ⊆ Rd+1 closed subgp.

Chabauty topology

Basis of neighborhoods of C ∈ Cℓ NK,U(C) where K ⊆ X compact and U ⊆ X open with 0 ∈ U.

Johannes Hofscheier LSD

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SLIDE 34

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

Cℓ := {C ⊆ X closed subgroup} X :=

  • x ∈ Rd+1 : d+1

i=1 xi ∈ Z

  • ⊆ Rd+1 closed subgp.

Chabauty topology

Basis of neighborhoods of C ∈ Cℓ NK,U(C) = {D ∈ Cℓ: C ∩ K ⊆ D + U, }. where K ⊆ X compact and U ⊆ X open with 0 ∈ U.

Johannes Hofscheier LSD

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SLIDE 35

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

Cℓ := {C ⊆ X closed subgroup} X :=

  • x ∈ Rd+1 : d+1

i=1 xi ∈ Z

  • ⊆ Rd+1 closed subgp.

Chabauty topology

Basis of neighborhoods of C ∈ Cℓ NK,U(C) = {D ∈ Cℓ: C ∩ K ⊆ D + U, D ∩ K ⊆ C + U}. where K ⊆ X compact and U ⊆ X open with 0 ∈ U.

Johannes Hofscheier LSD

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SLIDE 36

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

K ⊆ X compact, U ⊆ X open with 0 ∈ U. NK,U(C) = {D ∈ Cℓ: C ∩ K ⊆ D + U, D ∩ K ⊆ C + U}. C

Johannes Hofscheier LSD

slide-37
SLIDE 37

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

K ⊆ X compact, U ⊆ X open with 0 ∈ U. NK,U(C) = {D ∈ Cℓ: C ∩ K ⊆ D + U, D ∩ K ⊆ C + U}. C D

Johannes Hofscheier LSD

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SLIDE 38

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

K ⊆ X compact, U ⊆ X open with 0 ∈ U. NK,U(C) = {D ∈ Cℓ: C ∩ K ⊆ D + U, D ∩ K ⊆ C + U}. C D K

Johannes Hofscheier LSD

slide-39
SLIDE 39

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

K ⊆ X compact, U ⊆ X open with 0 ∈ U. NK,U(C) = {D ∈ Cℓ: C ∩ K ⊆ D + U, D ∩ K ⊆ C + U}. C D K C ∩ K ⊆ D + U

Johannes Hofscheier LSD

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SLIDE 40

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

K ⊆ X compact, U ⊆ X open with 0 ∈ U. NK,U(C) = {D ∈ Cℓ: C ∩ K ⊆ D + U, D ∩ K ⊆ C + U}. C D K C ∩ K ⊆ D + U

Johannes Hofscheier LSD

slide-41
SLIDE 41

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

K ⊆ X compact, U ⊆ X open with 0 ∈ U. NK,U(C) = {D ∈ Cℓ: C ∩ K ⊆ D + U, D ∩ K ⊆ C + U}. C D K C ∩ K ⊆ D + U D ∩ K ⊆ C + U

Johannes Hofscheier LSD

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SLIDE 42

Motivation LLS LSD

  • Deg. 2

Appl.

Chabauty Topology

K ⊆ X compact, U ⊆ X open with 0 ∈ U. NK,U(C) = {D ∈ Cℓ: C ∩ K ⊆ D + U, D ∩ K ⊆ C + U}. C D K C ∩ K ⊆ D + U D ∩ K ⊆ C + U

Johannes Hofscheier LSD

slide-43
SLIDE 43

Motivation LLS LSD

  • Deg. 2

Appl.

Simplicial Lattices

Proposition

C :=

  • C ∈ Cℓ: Zd+1 ⊆ C
  • ⊆ Cℓ closed

D := {C ∈ Cℓ discrete} ⊆ Cℓ open and dense. In particular

  • Λ ⊆ Rd+1 simplicial lattice
  • = D ∩ C ⊆ Cℓ is locally

closed.

Johannes Hofscheier LSD

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SLIDE 44

Motivation LLS LSD

  • Deg. 2

Appl.

Degree

Definition

Degree deg(C) of C ∈ C : deg(C) := max d+1

i=1 xi : (x1, . . . , xd+1) ∈ C ∩ [0, 1[d+1

  • .

Proposition

For ∆ ⊆ Rd a d-dim. lattice simplex, we have deg(Λ∆) = deg(∆).

Johannes Hofscheier LSD

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SLIDE 45

Motivation LLS LSD

  • Deg. 2

Appl.

The Moduli Space

Clearly: M0,s = M0,≤s \ M0,≤s−1. M0,≤s turns out to have better topological properties.

Johannes Hofscheier LSD

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SLIDE 46

Motivation LLS LSD

  • Deg. 2

Appl.

The Moduli Space

Clearly: M0,s = M0,≤s \ M0,≤s−1. M0,≤s turns out to have better topological properties.

Proposition

M0,≤s(d) := {C ∈ C : deg(C) ≤ s} ⊆ C closed.

Proposition

The assignment ∆ → Λ∆ induces a bijection between the d-dim. lattice simplices with deg(∆) ≤ s and M0,≤s(d) ∩ D.

Johannes Hofscheier LSD

slide-47
SLIDE 47

Motivation LLS LSD

  • Deg. 2

Appl.

Lattice Pyramids

Definition

Let ∆ ⊆ Rd be a lattice polytope. Lattice pyramid over ∆: conv(∆ × {0}, ed+1) ⊆ Rd+1.

Johannes Hofscheier LSD

slide-48
SLIDE 48

Motivation LLS LSD

  • Deg. 2

Appl.

Lattice Pyramids

Definition

Let ∆ ⊆ Rd be a lattice polytope. Lattice pyramid over ∆: conv(∆ × {0}, ed+1) ⊆ Rd+1. ∆ = conv(±e1 ± e2) ⊆ R2 ∆ × {0}

Johannes Hofscheier LSD

slide-49
SLIDE 49

Motivation LLS LSD

  • Deg. 2

Appl.

Lattice Pyramids

Definition

Let ∆ ⊆ Rd be a lattice polytope. Lattice pyramid over ∆: conv(∆ × {0}, ed+1) ⊆ Rd+1. ∆ = conv(±e1 ± e2) ⊆ R2 ∆ × {0}

Johannes Hofscheier LSD

slide-50
SLIDE 50

Motivation LLS LSD

  • Deg. 2

Appl.

Lattice Pyramids

Definition

Let ∆ ⊆ Rd be a lattice polytope. Lattice pyramid over ∆: conv(∆ × {0}, ed+1) ⊆ Rd+1. ∆ = conv(±e1 ± e2) ⊆ R2 ∆ × {0}

Johannes Hofscheier LSD

slide-51
SLIDE 51

Motivation LLS LSD

  • Deg. 2

Appl.

Simplices of given Degree

Proposition

The d-dim. lattice simplex ∆ ⊆ Rd is a lattice pyramid iff πi(Λ∆) = Z where πi : Rd+1 → R; x → xi for i = 1, . . . , d + 1.

Theorem[Nill]

Let ∆ ⊆ Rd be a d-dim. lattice simplex. If d ≥ 4 deg(∆) − 1, then ∆ is a lattice pyramid.

Corollary

M0,≤s ⊆ P

  • R4s−1

(power set).

Johannes Hofscheier LSD

slide-52
SLIDE 52

Motivation LLS LSD

  • Deg. 2

Appl.

Finiteness

Proposition [Chabauty]

X locally compact ⇒ Cℓ is compact. In particular M0,≤s ⊆ Cℓ compact. Partial ordering on Cℓ: C ≤ D: ⇔ C ⊆ D (C, D ∈ Cℓ).

Theorem

The set of maximal elements in M0,≤s is finite.

Johannes Hofscheier LSD

slide-53
SLIDE 53

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof

Set M :=

  • C ∈ M0,≤s maximal
  • .

Johannes Hofscheier LSD

slide-54
SLIDE 54

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof

Set M :=

  • C ∈ M0,≤s maximal
  • .

Assume |M| = ∞.

Johannes Hofscheier LSD

slide-55
SLIDE 55

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof

Set M :=

  • C ∈ M0,≤s maximal
  • .

Assume |M| = ∞. M0,≤s compact ⇒ M has a limit point, say C0 ∈ M0,≤s

Johannes Hofscheier LSD

slide-56
SLIDE 56

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof

Set M :=

  • C ∈ M0,≤s maximal
  • .

Assume |M| = ∞. M0,≤s compact ⇒ M has a limit point, say C0 ∈ M0,≤s, i. e., there is a sequence (Cn)n∈Z>0 ⊆ M with Cn = C0 for all n and Cn → C0.

Johannes Hofscheier LSD

slide-57
SLIDE 57

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof

Set M :=

  • C ∈ M0,≤s maximal
  • .

Assume |M| = ∞. M0,≤s compact ⇒ M has a limit point, say C0 ∈ M0,≤s, i. e., there is a sequence (Cn)n∈Z>0 ⊆ M with Cn = C0 for all n and Cn → C0.

Chabauty-Pontryagin Duality[Cornulier]

The duality map ∗:

  • cl. subgrp. ⊆ Rd+1

  • cl. subgrp. ⊆ Rd+1

; C → C∗ :=

  • x ∈ Rd+1 :

d+1

  • i=1

xiyi ∈ Z ∀y ∈ C

  • is an involutory homeomorphism.

Johannes Hofscheier LSD

slide-58
SLIDE 58

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof (continued)

Hence C∗

n → C∗ 0.

Johannes Hofscheier LSD

slide-59
SLIDE 59

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof (continued)

Hence C∗

n → C∗ 0.

C∗

i ⊆ Zd+1 for all i ∈ Z≥0

Johannes Hofscheier LSD

slide-60
SLIDE 60

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof (continued)

Hence C∗

n → C∗ 0.

C∗

i ⊆ Zd+1 for all i ∈ Z≥0 ⇒ for every compact K ⊆ Rd+1 there

is N > 0 such that C∗

n ∩ K = C∗ 0 ∩ K for n ≥ N.

Johannes Hofscheier LSD

slide-61
SLIDE 61

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof (continued)

Hence C∗

n → C∗ 0.

C∗

i ⊆ Zd+1 for all i ∈ Z≥0 ⇒ for every compact K ⊆ Rd+1 there

is N > 0 such that C∗

n ∩ K = C∗ 0 ∩ K for n ≥ N.

For K big enough C∗

0 ∩ K contains a basis of C∗ 0.

Johannes Hofscheier LSD

slide-62
SLIDE 62

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof (continued)

Hence C∗

n → C∗ 0.

C∗

i ⊆ Zd+1 for all i ∈ Z≥0 ⇒ for every compact K ⊆ Rd+1 there

is N > 0 such that C∗

n ∩ K = C∗ 0 ∩ K for n ≥ N.

For K big enough C∗

0 ∩ K contains a basis of C∗ 0.

We obtain C∗

0 ⊆ C∗ n for n >

> 0. So Cn C0. Contradiction to maximality.

Johannes Hofscheier LSD

slide-63
SLIDE 63

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof (continued)

Hence C∗

n → C∗ 0.

C∗

i ⊆ Zd+1 for all i ∈ Z≥0 ⇒ for every compact K ⊆ Rd+1 there

is N > 0 such that C∗

n ∩ K = C∗ 0 ∩ K for n ≥ N.

For K big enough C∗

0 ∩ K contains a basis of C∗ 0.

We obtain C∗

0 ⊆ C∗ n for n >

> 0. So Cn C0. Contradiction to maximality.

Remark

Could be also proved using a result due to Lawrence.

Johannes Hofscheier LSD

slide-64
SLIDE 64

Motivation LLS LSD

  • Deg. 2

Appl.

Degree 1

Theorem [Batyrev, Nill]

A lattice simplex of degree ≤ 1 is either a lattice pyramid over an interval or a lattice pyramid over twice a unimodular simplex.

Corollary

The maximal elements in M0,≤1 ⊆ P

  • R3

are the following:

  • − 1

2 1 2 0 − 1 2 0 1 2

  • and

Z3 + R(e1 − e2) =: ( 1 −1 0 )

Johannes Hofscheier LSD

slide-65
SLIDE 65

Motivation LLS LSD

  • Deg. 2

Appl.

Degree 2 case

Recall: a1, . . . , ap, b1, . . . , bq ∈ Rd+1 linearly indep.      

— a1 —

. . .

— ap — — b1 —

. . .

— bq —

      :=

p

  • i=1

Zai ⊕

q

  • j=1

Rbj

Johannes Hofscheier LSD

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SLIDE 66

Motivation LLS LSD

  • Deg. 2

Appl.

Degree 2 case (continued)

Theorem[Higashitani, H.]

The maximal elements in M0,≤2 ⊆ P

  • R7

are the following:

1

  • −1 1 0 0 0 0

−1 0 1 0 0 0

  • 2
  • 1 −1

0 0 0 0 0 −1 1 0 0

1

2 1 2 0 0 0 1 2 0 1 2 0 0 1 −1 0 0 0 0

1

2 0 0 1 2 0 0 1 1 −2 0 0 0

  • +9 more
  • discr. subgrp.

3

  • 0 0

1 2 1 2 0 0 0 0 0 1 2 1 2 0 1 −1 0 0 0 0

1

2 1 2 1 2 1 2 0 0 0 0 1 2 1 4 1 4 0

1

3 2 3 1 3 2 3 0 0 0 0 1 3 1 3 1 3 0

1 2 0 1 2 0 0 0 0 1 2 0 1 2 0 0 0 0 1 2 1 4 1 4 0

 

4 All other max. subgrp. are discrete and contained in 1

2Z7.

Johannes Hofscheier LSD

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SLIDE 67

Motivation LLS LSD

  • Deg. 2

Appl.

Cayley Conjecture

Definition

∆ ⊆ Rd is a Cayley Polytope of lattice polytopes ∆1, . . . , ∆k ⊆ Rm if k ≥ 2 and ∆ is unimodularly equivalent to conv(∆1 × e1, . . . , ∆k × ek) ⊆ Rm × Rk.

Johannes Hofscheier LSD

slide-68
SLIDE 68

Motivation LLS LSD

  • Deg. 2

Appl.

Cayley Conjecture

Definition

∆ ⊆ Rd is a Cayley Polytope of lattice polytopes ∆1, . . . , ∆k ⊆ Rm if k ≥ 2 and ∆ is unimodularly equivalent to conv(∆1 × e1, . . . , ∆k × ek) ⊆ Rm × Rk. ∆1, ∆2 ⊆ R two (lattice) intervals.

Johannes Hofscheier LSD

slide-69
SLIDE 69

Motivation LLS LSD

  • Deg. 2

Appl.

Cayley Conjecture

Definition

∆ ⊆ Rd is a Cayley Polytope of lattice polytopes ∆1, . . . , ∆k ⊆ Rm if k ≥ 2 and ∆ is unimodularly equivalent to conv(∆1 × e1, . . . , ∆k × ek) ⊆ Rm × Rk. ∆1, ∆2 ⊆ R two (lattice) intervals.

∆1 × e1 Johannes Hofscheier LSD

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SLIDE 70

Motivation LLS LSD

  • Deg. 2

Appl.

Cayley Conjecture

Definition

∆ ⊆ Rd is a Cayley Polytope of lattice polytopes ∆1, . . . , ∆k ⊆ Rm if k ≥ 2 and ∆ is unimodularly equivalent to conv(∆1 × e1, . . . , ∆k × ek) ⊆ Rm × Rk. ∆1, ∆2 ⊆ R two (lattice) intervals.

∆2 × e2 ∆1 × e1 Johannes Hofscheier LSD

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SLIDE 71

Motivation LLS LSD

  • Deg. 2

Appl.

Cayley Conjecture

Definition

∆ ⊆ Rd is a Cayley Polytope of lattice polytopes ∆1, . . . , ∆k ⊆ Rm if k ≥ 2 and ∆ is unimodularly equivalent to conv(∆1 × e1, . . . , ∆k × ek) ⊆ Rm × Rk. ∆1, ∆2 ⊆ R two (lattice) intervals.

∆2 × e2 ∆1 × e1 Johannes Hofscheier LSD

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SLIDE 72

Motivation LLS LSD

  • Deg. 2

Appl.

Cayley Conjecture

“Weak” Cayley Conjecture[Dickenstein, Nill]

A d-dim. lattice polytpe with degree s is a Cayley polytope, if d > 2s.

Proposition[Higashitani,H.]

The “Weak” Cayley Conjecture holds for degree 2 simplices.

Johannes Hofscheier LSD

slide-73
SLIDE 73

Motivation LLS LSD

  • Deg. 2

Appl.

Idea of Proof

Proposition

Let Λ ∈ C ∩ D ⊆ Rd+1. Λ corresponds to a Cayley polytope iff there is a proper subset I {1, . . . , d + 1} such that fI(Λ) ⊆ Z where fI : Λ → R; x →

i∈I xi.

Need to consider dim. at least 5, i. e., the max. subgrp. satisfy Λ ⊆ 1

2Z7.

Example (6-dim.):  

1 2 1 2 1 2 1 2 0 0 0 1 2 1 2 0 0 1 2 1 2 0 1 2 0 1 2 0 1 2 0 1 2

  for instance I = {1, 2, 3, 4}.

Johannes Hofscheier LSD

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SLIDE 74

Motivation LLS LSD

  • Deg. 2

Appl.

Not realizable h∗-vectors

50 100 150 200 250 50 100 150 200 250 σ1 σ2 σ3 σ0 h∗

1

h∗

2

Johannes Hofscheier LSD

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SLIDE 75

Motivation LLS LSD

  • Deg. 2

Appl.

Not realizable h∗-vectors

50 100 150 200 250 50 100 150 200 250 σ1 σ2 σ3 σ′

1

σ′

2

σ′

3

h∗

1

h∗

2

Johannes Hofscheier LSD

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SLIDE 76

Motivation LLS LSD

  • Deg. 2

Appl.

Not realizable h∗-vectors

50 100 150 200 250 50 100 150 200 250 σ1 σ2 σ3 σ′

1

σ′

2

σ′

3

h∗

1

h∗

2

Johannes Hofscheier LSD

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SLIDE 77

Motivation LLS LSD

  • Deg. 2

Appl.

Thank you!

Johannes Hofscheier LSD