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Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic Pullback Line Bundles On Smooth And Compact Normal Toric Varieties Martin Bies Feb 11, 2014 Martin Bies Cohomology Of Holomorphic Pullback LIne Bundles

Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

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Page 1: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Cohomology Of Holomorphic Pullback LineBundles On Smooth And Compact Normal Toric

Varieties

Martin Bies

Feb 11, 2014

Martin Bies Cohomology Of Holomorphic Pullback LIne Bundles

Page 2: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

Section 1

Motivation From Physics

1 / 20

Page 3: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes

1 / 20

Page 4: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes

Intersecting D7-Branes

D7 brane Ba withU (1)a gauge theory La

1 / 20

Page 5: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes

Intersecting D7-Branes

D7 brane Ba withU (1)a gauge theory La

D7 brane Bb withU (1)b gauge theory Lb

1 / 20

Page 6: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes

Intersecting D7-Branes

D7 brane Ba withU (1)a gauge theory La

D7 brane Bb withU (1)b gauge theory Lb

C

1 / 20

Page 7: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes

Intersecting D7-Branes

D7 brane Ba withU (1)a gauge theory La

D7 brane Bb withU (1)b gauge theory Lb

CGauge enhancement on Cdescribed by La|C ⊗ Lb|C

1 / 20

Page 8: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes

Intersecting D7-Branes

D7 brane Ba withU (1)a gauge theory La

D7 brane Bb withU (1)b gauge theory Lb

CGauge enhancement on Cdescribed by La|C ⊗ Lb|C

Consequence hep-th/0403166

Spectrum of masslesszero modes at C

H0 (C, La|C ⊗ Lb|C)H1 (C, La|C ⊗ Lb|C)

1 / 20

Page 9: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes - Simplified Setup

Ba with La

Bb with Lb

C

CY X3

XΣ Simplifying Assumptions

XΣ a smooth and compactnormal toric variety

C, Ba, Bb, X3 ⊂ XΣ

submanifolds

∃L ∈ Pic (XΣ) s.t.L|C = La|C ⊗ Lb|C

New Question

How to compute H i (C , L|C )?

2 / 20

Page 10: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes - Simplified Setup

Ba with La

Bb with Lb

C

CY X3

Simplifying Assumptions

XΣ a smooth and compactnormal toric variety

C, Ba, Bb, X3 ⊂ XΣ

submanifolds

∃L ∈ Pic (XΣ) s.t.L|C = La|C ⊗ Lb|C

New Question

How to compute H i (C , L|C )?

2 / 20

Page 11: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes - Simplified Setup

Ba with La

Bb with Lb

C

CY X3

XΣ Simplifying Assumptions

XΣ a smooth and compactnormal toric variety

C, Ba, Bb, X3 ⊂ XΣ

submanifolds

∃L ∈ Pic (XΣ) s.t.L|C = La|C ⊗ Lb|C

New Question

How to compute H i (C , L|C )?

2 / 20

Page 12: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes - Simplified Setup

Ba with La

Bb with Lb

C

CY X3

XΣ Simplifying Assumptions

XΣ a smooth and compactnormal toric variety

C, Ba, Bb, X3 ⊂ XΣ

submanifolds

∃L ∈ Pic (XΣ) s.t.L|C = La|C ⊗ Lb|C

New Question

How to compute H i (C , L|C )?

2 / 20

Page 13: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes - Simplified Setup

Ba with La

Bb with Lb

C

CY X3

XΣ Simplifying Assumptions

XΣ a smooth and compactnormal toric variety

C, Ba, Bb, X3 ⊂ XΣ

submanifolds

∃L ∈ Pic (XΣ) s.t.L|C = La|C ⊗ Lb|C

New Question

How to compute H i (C , L|C )?

2 / 20

Page 14: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

U(1) Charged Localised Zero Modes - Simplified Setup

Ba with La

Bb with Lb

C

CY X3

XΣ Simplifying Assumptions

XΣ a smooth and compactnormal toric variety

C, Ba, Bb, X3 ⊂ XΣ

submanifolds

∃L ∈ Pic (XΣ) s.t.L|C = La|C ⊗ Lb|C

New Question

How to compute H i (C , L|C )?

2 / 20

Page 15: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

What Is A Toric Variety? Book by D. Cox, J. Little, H. Schenk ’Toric Varieties’

Toric Varieties Via Homogenisation

Every smooth and compact normal toric variety XΣ is given by

XΣ∼= (Cr − Z ) / (C∗)a

Example: Complex Projective Space

CPn ≡(Cn+1 − {0}

)/C∗

Why Smooth And Compact Normal Toric Varieties?

Let XΣ∼= (Cr − Z ) / (C∗)a. Then it holds

Pic (XΣ) ∼= Za.

H i (XΣ,OXΣ(v)) are finite dimensional vector spaces.

3 / 20

Page 16: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

What Is A Toric Variety? Book by D. Cox, J. Little, H. Schenk ’Toric Varieties’

Toric Varieties Via Homogenisation

Every smooth and compact normal toric variety XΣ is given by

XΣ∼= (Cr − Z ) / (C∗)a

Example: Complex Projective Space

CPn ≡(Cn+1 − {0}

)/C∗

Why Smooth And Compact Normal Toric Varieties?

Let XΣ∼= (Cr − Z ) / (C∗)a. Then it holds

Pic (XΣ) ∼= Za.

H i (XΣ,OXΣ(v)) are finite dimensional vector spaces.

3 / 20

Page 17: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

What Is A Toric Variety? Book by D. Cox, J. Little, H. Schenk ’Toric Varieties’

Toric Varieties Via Homogenisation

Every smooth and compact normal toric variety XΣ is given by

XΣ∼= (Cr − Z ) / (C∗)a

Example: Complex Projective Space

CPn ≡(Cn+1 − {0}

)/C∗

Why Smooth And Compact Normal Toric Varieties?

Let XΣ∼= (Cr − Z ) / (C∗)a. Then it holds

Pic (XΣ) ∼= Za.

H i (XΣ,OXΣ(v)) are finite dimensional vector spaces.

3 / 20

Page 18: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

Example: Computation Of Ambient Space Cohomologies

Ingredients

ambient space CP3

L = OCP3 (1)

cohomCalg hep-th/1003.5217, hep-th/1010.3717, math.AG/1006.0780, hep-th/1006.2392

I implemented a function into Mathematica which computes abasis of cohomology based on cohomCalg.

Result from Mathematica

H0(CP3,OCP3 (1)

)= {α1x1 + α2x2 + α3x3 , αi ∈ C} ∼= C3

H i(CP3,OCP3 (1)

)= 0 for i ≥ 1

4 / 20

Page 19: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

Example: Computation Of Ambient Space Cohomologies

Ingredients

ambient space CP3

L = OCP3 (1)

cohomCalg hep-th/1003.5217, hep-th/1010.3717, math.AG/1006.0780, hep-th/1006.2392

I implemented a function into Mathematica which computes abasis of cohomology based on cohomCalg.

Result from Mathematica

H0(CP3,OCP3 (1)

)= {α1x1 + α2x2 + α3x3 , αi ∈ C} ∼= C3

H i(CP3,OCP3 (1)

)= 0 for i ≥ 1

4 / 20

Page 20: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

Example: Computation Of Ambient Space Cohomologies

Ingredients

ambient space CP3

L = OCP3 (1)

cohomCalg hep-th/1003.5217, hep-th/1010.3717, math.AG/1006.0780, hep-th/1006.2392

I implemented a function into Mathematica which computes abasis of cohomology based on cohomCalg.

Result from Mathematica

H0(CP3,OCP3 (1)

)= {α1x1 + α2x2 + α3x3 , αi ∈ C} ∼= C3

H i(CP3,OCP3 (1)

)= 0 for i ≥ 1

4 / 20

Page 21: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

Example: Computation Of Ambient Space Cohomologies

Ingredients

ambient space CP3

L = OCP3 (1)

cohomCalg hep-th/1003.5217, hep-th/1010.3717, math.AG/1006.0780, hep-th/1006.2392

I implemented a function into Mathematica which computes abasis of cohomology based on cohomCalg.

Result from Mathematica

H0(CP3,OCP3 (1)

)= {α1x1 + α2x2 + α3x3 , αi ∈ C} ∼= C3

H i(CP3,OCP3 (1)

)= 0 for i ≥ 1

4 / 20

Page 22: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Localised Zero Modes In Type IIB CompactificationSimplification: Towards Toric Varieties

Questions so far?

5 / 20

Page 23: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Section 2

The Hypersurface Case

5 / 20

Page 24: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Task

CY X3

Ingredients

Toric variety XΣ

L = OXΣ(D)

s̃1 ∈ H0 (XΣ,OXΣ(S1)) s.t.

X3 = {p ∈ XΣ , s̃1 (p) = 0}

Goal

Compute H i(X3, L|X3

).

6 / 20

Page 25: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Task

CY X3

Ingredients

Toric variety XΣ

L = OXΣ(D)

s̃1 ∈ H0 (XΣ,OXΣ(S1)) s.t.

X3 = {p ∈ XΣ , s̃1 (p) = 0}

Goal

Compute H i(X3, L|X3

).

6 / 20

Page 26: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Task

CY X3

Ingredients

Toric variety XΣ

L = OXΣ(D)

s̃1 ∈ H0 (XΣ,OXΣ(S1)) s.t.

X3 = {p ∈ XΣ , s̃1 (p) = 0}

Goal

Compute H i(X3, L|X3

).

6 / 20

Page 27: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Task

CY X3

Ingredients

Toric variety XΣ

L = OXΣ(D)

s̃1 ∈ H0 (XΣ,OXΣ(S1)) s.t.

X3 = {p ∈ XΣ , s̃1 (p) = 0}

Goal

Compute H i(X3, L|X3

).

6 / 20

Page 28: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Hypersurface Case

Theorem To the proof

The following sequence is sheaf exact

0→ OXΣ(D − S1)︸ ︷︷ ︸=L′

⊗s̃1→ OXΣ(D)︸ ︷︷ ︸

=L

r→ OXΣ(D)|X3

→ 0

Consequence: There is a long exact cohomology sequence

0 H0(XΣ,L′) H0(XΣ,L) H0(X3, L|X3)

H1(XΣ,L′) H1(XΣ,L) H1(X3, L|X3)

H2(XΣ,L′) H2(XΣ,L) H2(X3, L|X3)

α0 β0

δ0

α1

α2

7 / 20

Page 29: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Hypersurface Case

Theorem To the proof

The following sequence is sheaf exact

0→ OXΣ(D − S1)︸ ︷︷ ︸=L′

⊗s̃1→ OXΣ(D)︸ ︷︷ ︸

=L

r→ OXΣ(D)|X3

→ 0

Consequence: There is a long exact cohomology sequence

0 H0(XΣ,L′) H0(XΣ,L) H0(X3, L|X3)

H1(XΣ,L′) H1(XΣ,L) H1(X3, L|X3)

H2(XΣ,L′) H2(XΣ,L) H2(X3, L|X3)

α0 β0

δ0

α1

α2

7 / 20

Page 30: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Hypersurface Case II

The E1-Sheet

0 0 0

H0 (XΣ,L′) H1 (XΣ,L′) H2 (XΣ,L′)

H0 (XΣ,L) H1 (XΣ,L) H2 (XΣ,L)

0 0 0

α0 α1 α2

Compute with Mathematica.

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

0 0 0

H0(X3, L|X3

)H1(X3, L|X3

)

Vi := H i (XΣ,L) /Im(αi)

8 / 20

Page 31: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Hypersurface Case II

The E1-Sheet

0 0 0

H0 (XΣ,L′) H1 (XΣ,L′) H2 (XΣ,L′)

H0 (XΣ,L) H1 (XΣ,L) H2 (XΣ,L)

0 0 0

α0 α1 α2

Compute with Mathematica.

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

0 0 0

H0(X3, L|X3

)H1(X3, L|X3

)

Vi := H i (XΣ,L) /Im(αi)

8 / 20

Page 32: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Hypersurface Case II

The E1-Sheet

0 0 0

H0 (XΣ,L′) H1 (XΣ,L′) H2 (XΣ,L′)

H0 (XΣ,L) H1 (XΣ,L) H2 (XΣ,L)

0 0 0

α0 α1 α2

Compute with Mathematica.

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

0 0 0

H0(X3, L|X3

)

H1(X3, L|X3

)

Vi := H i (XΣ,L) /Im(αi)

8 / 20

Page 33: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Hypersurface Case II

The E1-Sheet

0 0 0

H0 (XΣ,L′) H1 (XΣ,L′) H2 (XΣ,L′)

H0 (XΣ,L) H1 (XΣ,L) H2 (XΣ,L)

0 0 0

α0 α1 α2

Compute with Mathematica.

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

0 0 0

H0(X3, L|X3

)H1(X3, L|X3

)

Vi := H i (XΣ,L) /Im(αi)

8 / 20

Page 34: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

A Computational Example

Ingredients

Toric ambient space XΣ = CP2 × CP1 × CP1

s̃1 = C1x1 + C2x2 + C3x3 ∈ H0 (XΣ,OXΣ(1, 0, 0))

L = OXΣ(1, 0,−2)

Result

cohomCalg left an unconstraint constant A2 in the result.

My notebook computed this constant to be 0 forpseudo-random Ci ∈ (0, 1). So in this case

H0(XΣ, L|X3

)= 0, H1

(XΣ, L|X3

)= 2

9 / 20

Page 35: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

A Computational Example

Ingredients

Toric ambient space XΣ = CP2 × CP1 × CP1

s̃1 = C1x1 + C2x2 + C3x3 ∈ H0 (XΣ,OXΣ(1, 0, 0))

L = OXΣ(1, 0,−2)

Result

cohomCalg left an unconstraint constant A2 in the result.

My notebook computed this constant to be 0 forpseudo-random Ci ∈ (0, 1). So in this case

H0(XΣ, L|X3

)= 0, H1

(XΣ, L|X3

)= 2

9 / 20

Page 36: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

The Principle Answer Is . . .The Practical Answer

Questions?

10 / 20

Page 37: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Section 3

The Codimension Two Case

10 / 20

Page 38: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Task

CY X3CY X3

Ba

Ingredients

Toric variety XΣ

L = OXΣ(D)

Polynomial s̃1 s.t.X3 = {s̃1 = 0}Polynomial s̃2 s.t.Ba = {s̃1 = s̃2 = 0}

Task

Compute H i(Ba, L|Ba

).

11 / 20

Page 39: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Task

CY X3CY X3

Ba

Ingredients

Toric variety XΣ

L = OXΣ(D)

Polynomial s̃1 s.t.X3 = {s̃1 = 0}Polynomial s̃2 s.t.Ba = {s̃1 = s̃2 = 0}

Task

Compute H i(Ba, L|Ba

).

11 / 20

Page 40: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Task

CY X3

CY X3

Ba

Ingredients

Toric variety XΣ

L = OXΣ(D)

Polynomial s̃1 s.t.X3 = {s̃1 = 0}

Polynomial s̃2 s.t.Ba = {s̃1 = s̃2 = 0}

Task

Compute H i(Ba, L|Ba

).

11 / 20

Page 41: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Task

CY X3CY X3

Ba

Ingredients

Toric variety XΣ

L = OXΣ(D)

Polynomial s̃1 s.t.X3 = {s̃1 = 0}Polynomial s̃2 s.t.Ba = {s̃1 = s̃2 = 0}

Task

Compute H i(Ba, L|Ba

).

11 / 20

Page 42: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Task

CY X3CY X3

Ba

Ingredients

Toric variety XΣ

L = OXΣ(D)

Polynomial s̃1 s.t.X3 = {s̃1 = 0}Polynomial s̃2 s.t.Ba = {s̃1 = s̃2 = 0}

Task

Compute H i(Ba, L|Ba

).

11 / 20

Page 43: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Codimension 2 Case

Theorem

The following sequence is sheaf exact

0→ L′⊗

s̃2

−s̃1

−−−−−−−−→ V1

⊗(s̃1 ,̃s2)−−−−−→ L r→ L|Ba → 0

where

L′ = O (D − S1 − S2)

V1 = O (D − S1)⊕O (D − S2)

Watch out!

There is no associated long exact sequence in cohomology.

12 / 20

Page 44: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Codimension 2 Case

Theorem

The following sequence is sheaf exact

0→ L′⊗

s̃2

−s̃1

−−−−−−−−→ V1

⊗(s̃1 ,̃s2)−−−−−→ L r→ L|Ba → 0

where

L′ = O (D − S1 − S2)

V1 = O (D − S1)⊕O (D − S2)

Watch out!

There is no associated long exact sequence in cohomology.

12 / 20

Page 45: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Spectral Sequence Construction Book by D. Cox, J. Little, H. Schenk ’toric varieties’,

’Aspects of (2,0) string compactifications’ by B. Green, J. Distler

Rough Picture

q

p

r

E 1,00

E 1,10

E 1,20

Ep,q0 are Abelian groups.

Derive E0 cohomologies.

Write those into sheet E1.

Derive E1 cohomologies.

. . .

13 / 20

Page 46: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E1-Sheet

0 0 0

H0 (XΣ,L′) H1 (XΣ,L′) H2 (XΣ,L′)

H0 (XΣ,V1) H1 (XΣ,V1) H2 (XΣ,V1)

H0 (XΣ,L) H1 (XΣ,L) H2 (XΣ,L)

0 0 0

β0 β1 β2

α0 α1 α2

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

Definitions

Vi := ker(βi)/im

(αi)Wi := H i (XΣ,L) /im

(βi)

14 / 20

Page 47: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E1-Sheet

0 0 0

H0 (XΣ,L′) H1 (XΣ,L′) H2 (XΣ,L′)

H0 (XΣ,V1) H1 (XΣ,V1) H2 (XΣ,V1)

H0 (XΣ,L) H1 (XΣ,L) H2 (XΣ,L)

0 0 0

β0 β1 β2

α0 α1 α2

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

Definitions

Vi := ker(βi)/im

(αi)Wi := H i (XΣ,L) /im

(βi)

14 / 20

Page 48: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E1-Sheet

0 0 0

H0 (XΣ,L′) H1 (XΣ,L′) H2 (XΣ,L′)

H0 (XΣ,V1) H1 (XΣ,V1) H2 (XΣ,V1)

H0 (XΣ,L) H1 (XΣ,L) H2 (XΣ,L)

0 0 0

β0 β1 β2

α0 α1 α2

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

Definitions

Vi := ker(βi)/im

(αi)Wi := H i (XΣ,L) /im

(βi)

14 / 20

Page 49: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E1-Sheet

0 0 0

H0 (XΣ,L′) H1 (XΣ,L′) H2 (XΣ,L′)

H0 (XΣ,V1) H1 (XΣ,V1) H2 (XΣ,V1)

H0 (XΣ,L) H1 (XΣ,L) H2 (XΣ,L)

0 0 0

β0 β1 β2

α0 α1 α2

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

Definitions

Vi := ker(βi)/im

(αi)Wi := H i (XΣ,L) /im

(βi)

14 / 20

Page 50: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

α0(2) α1

(2)

The E3-Sheet

0 0 0

ker(α0)

ker(α1

(2)

)ker(α2

(2)

)

V0 V1 V2

W̃0 W̃1 W̃2

0 0 0

H0(Ba, L|Ba

)H1(Ba, L|Ba

)H2(Ba, L|Ba

)

Definition

W̃i := Wi/Im(αi

(2)

)

15 / 20

Page 51: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

α0(2) α1

(2)

The E3-Sheet

0 0 0

ker(α0)

ker(α1

(2)

)ker(α2

(2)

)

V0 V1 V2

W̃0 W̃1 W̃2

0 0 0

H0(Ba, L|Ba

)H1(Ba, L|Ba

)H2(Ba, L|Ba

)

Definition

W̃i := Wi/Im(αi

(2)

)

15 / 20

Page 52: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

α0(2) α1

(2)

The E3-Sheet

0 0 0

ker(α0)

ker(α1

(2)

)ker(α2

(2)

)

V0 V1 V2

W̃0 W̃1 W̃2

0 0 0

H0(Ba, L|Ba

)H1(Ba, L|Ba

)H2(Ba, L|Ba

)

Definition

W̃i := Wi/Im(αi

(2)

)15 / 20

Page 53: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

α0(2) α1

(2)

The E3-Sheet

0 0 0

ker(α0)

ker(α1

(2)

)ker(α2

(2)

)

V0 V1 V2

W̃0 W̃1 W̃2

0 0 0

H0(Ba, L|Ba

)

H1(Ba, L|Ba

)H2(Ba, L|Ba

)

Definition

W̃i := Wi/Im(αi

(2)

)15 / 20

Page 54: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

α0(2) α1

(2)

The E3-Sheet

0 0 0

ker(α0)

ker(α1

(2)

)ker(α2

(2)

)

V0 V1 V2

W̃0 W̃1 W̃2

0 0 0

H0(Ba, L|Ba

)H1(Ba, L|Ba

)

H2(Ba, L|Ba

)

Definition

W̃i := Wi/Im(αi

(2)

)15 / 20

Page 55: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

The Codimension 2 Strategy

The E2-Sheet

0 0 0

ker(α0)

ker(α1)

ker(α2)

V0 V1 V2

W0 W1 W2

0 0 0

α0(2) α1

(2)

The E3-Sheet

0 0 0

ker(α0)

ker(α1

(2)

)ker(α2

(2)

)

V0 V1 V2

W̃0 W̃1 W̃2

0 0 0

H0(Ba, L|Ba

)H1(Ba, L|Ba

)H2(Ba, L|Ba

)

Definition

W̃i := Wi/Im(αi

(2)

)15 / 20

Page 56: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Example With Knight’s Move I

Ingredients

Toric ambient space XΣ = CP1 × CP1 × CP1

S1 = (1, 0, 1) and S2 = (0, 0, 1)

L = OXΣ(1, 1, 0)

E2-Sheet

L′ 0 P1 0 0

V1 0 0 0 0

L P2 0 0 0

H0 H1 H2 H3

α0(2)

16 / 20

Page 57: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Example With Knight’s Move I

Ingredients

Toric ambient space XΣ = CP1 × CP1 × CP1

S1 = (1, 0, 1) and S2 = (0, 0, 1)

L = OXΣ(1, 1, 0)

E2-Sheet

L′ 0 P1 0 0

V1 0 0 0 0

L P2 0 0 0

H0 H1 H2 H3

α0(2)

16 / 20

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Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Example With Knight’s Move II

Spaces And Polynomials

s̃1 = C4x1x5 + C2x2x5 + C3x1x6 + C1x2x6

s̃2 = C6x5 + C5x6

P1 ={A1 · x4

x5x6+ A2 · x3

x5x6, Ai ∈ C

}P2 = {A3 · x2x4 + A4 · x2x3 + A5x1x4 + A6x1x3 , Ai ∈ C}

It turns out that . . .

α0(2) : P1 → P2 is given by

α0(2) = x1x5x6 [C4C5 − C3C6] + x2x5x6 [C2C5 − C1C6]

Note

α0(2) respects the symmetries in P1 and P2.

17 / 20

Page 59: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Example With Knight’s Move II

Spaces And Polynomials

s̃1 = C4x1x5 + C2x2x5 + C3x1x6 + C1x2x6

s̃2 = C6x5 + C5x6

P1 ={A1 · x4

x5x6+ A2 · x3

x5x6, Ai ∈ C

}P2 = {A3 · x2x4 + A4 · x2x3 + A5x1x4 + A6x1x3 , Ai ∈ C}

It turns out that . . .

α0(2) : P1 → P2 is given by

α0(2) = x1x5x6 [C4C5 − C3C6] + x2x5x6 [C2C5 − C1C6]

Note

α0(2) respects the symmetries in P1 and P2.

17 / 20

Page 60: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Example With Knight’s Move II

Spaces And Polynomials

s̃1 = C4x1x5 + C2x2x5 + C3x1x6 + C1x2x6

s̃2 = C6x5 + C5x6

P1 ={A1 · x4

x5x6+ A2 · x3

x5x6, Ai ∈ C

}P2 = {A3 · x2x4 + A4 · x2x3 + A5x1x4 + A6x1x3 , Ai ∈ C}

It turns out that . . .

α0(2) : P1 → P2 is given by

α0(2) = x1x5x6 [C4C5 − C3C6] + x2x5x6 [C2C5 − C1C6]

Note

α0(2) respects the symmetries in P1 and P2.

17 / 20

Page 61: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Open Questions

Fact hep-th/0808.3621, book by T. Huebsch ’Calabi-Yau Manifolds: A Bestiary for Physicists’

The cohomologies H i (CPn,L) are labeled by representationsof U (1)× U (n).

⇒ The cohomologies H i(CP1 × CP1 × CP1,L

)have

(anti)-symmetrisation properties.

Question To the definition

Is every smooth and compact normal toric variety XΣ a generalisedFlag variety?

18 / 20

Page 62: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Towards Spectral SequencesOpen Question

Open Questions

Fact hep-th/0808.3621, book by T. Huebsch ’Calabi-Yau Manifolds: A Bestiary for Physicists’

The cohomologies H i (CPn,L) are labeled by representationsof U (1)× U (n).

⇒ The cohomologies H i(CP1 × CP1 × CP1,L

)have

(anti)-symmetrisation properties.

Question To the definition

Is every smooth and compact normal toric variety XΣ a generalisedFlag variety?

18 / 20

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Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Section 4

Summary And Future Work

18 / 20

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Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Summary

Take-Away-Message

Computing the spectrum of massless zero modes requiresspectral sequence technology.

The existing Koszul extension of cohomCalg leavesunconstraint constants in these computations.

⇒ My notebook computes the E1-sheet and thereby fixes many,but not all, of these constants.

19 / 20

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Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Future Works

Open Tasks

Prove of disprove that every smooth and compact normaltoric variety XΣ is a generalised Flag variety.

Extend the functionality of the notebook beyondhypersurfaces.

Improve the performance of the notebook.

Apply the notebook to model building.

20 / 20

Page 66: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Future Works

Open Tasks

Prove of disprove that every smooth and compact normaltoric variety XΣ is a generalised Flag variety.

Extend the functionality of the notebook beyondhypersurfaces.

Improve the performance of the notebook.

Apply the notebook to model building.

20 / 20

Page 67: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Future Works

Open Tasks

Prove of disprove that every smooth and compact normaltoric variety XΣ is a generalised Flag variety.

Extend the functionality of the notebook beyondhypersurfaces.

Improve the performance of the notebook.

Apply the notebook to model building.

20 / 20

Page 68: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Future Works

Open Tasks

Prove of disprove that every smooth and compact normaltoric variety XΣ is a generalised Flag variety.

Extend the functionality of the notebook beyondhypersurfaces.

Improve the performance of the notebook.

Apply the notebook to model building.

20 / 20

Page 69: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Motivation From PhysicsThe Hypersurface Case

The Codimension Two CaseSummary And Future Work

Thank you for your attention! Questions?

20 / 20

Page 70: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Proof I

Claim

Let X a smooth and compact normal toric variety given by

XΣ∼= (Cr − Z ) / (C∗)a

We pick s̃1 ∈ H0 (XΣ,OXΣ(S1)) non-trivial and define

X3 = {p ∈ XΣ , s̃1 (p) = 0}

Then for any divisor class D ∈ Cl (XΣ) the following sequence issheaf exact

0→ OXΣ(D − S1)

⊗s̃1→ OXΣ(D)

r→ OXΣ(D)|X3

→ 0

21 / 20

Page 71: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Proof II Back to orginal material.

Proof

Sheaf exactness is a local property. So let p ∈ XΣ a point.Then we have to show that the following sequence is exact

0→ OXΣ,p

[̃s1]p→ OXΣ,pr→ OXΣ,p/

([̃s1]p

)→ 0

Note that OXΣ,p is the local power series ring. This ring is anintegral domain. Therefore [̃s1]p is not a zero- divisor, so that

the map OXΣ,p

[̃s1]p→ OXΣ,p is injective.

The map OXΣ,pr→ OXΣ,p/

([̃s1]p

)is surjective.

22 / 20

Page 72: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Generalised Flag Varieties To the conjecture

Definition

A simply connected, compact, complex, homogeneous G -space istermed a generalised Flag variety.

Example

It holdsCPn ∼= U (n + 1) / (U (1)× U (n))

Consequence

The cohomology groups H i (CPn,OCPn (k)) are labeled byrepresentations of U (1)× U (n) for all k ∈ Z.

23 / 20

Page 73: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Generalised Flag Varieties To the conjecture

Definition

A simply connected, compact, complex, homogeneous G -space istermed a generalised Flag variety.

Example

It holdsCPn ∼= U (n + 1) / (U (1)× U (n))

Consequence

The cohomology groups H i (CPn,OCPn (k)) are labeled byrepresentations of U (1)× U (n) for all k ∈ Z.

23 / 20

Page 74: Cohomology Of Holomorphic Pullback Line Bundles On Smooth ... · Motivation From Physics The Hypersurface Case The Codimension Two Case Summary And Future Work Cohomology Of Holomorphic

Generalised Flag Varieties To the conjecture

Definition

A simply connected, compact, complex, homogeneous G -space istermed a generalised Flag variety.

Example

It holdsCPn ∼= U (n + 1) / (U (1)× U (n))

Consequence

The cohomology groups H i (CPn,OCPn (k)) are labeled byrepresentations of U (1)× U (n) for all k ∈ Z.

23 / 20