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Cluster Algebras Lauren K. Williams, Harvard 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 2 3 4 5 6 1 P 13 P 24 = P 12 P 34 + P 14 P 23 P 15 P 46 = P 14 P 56 + P 16 P 45 Lauren K. Williams (Harvard) Cluster Algebras October 2019 1 / 23
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Page 1: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Cluster Algebras

Lauren K. Williams, Harvard

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

P13P24

= P12P34

+ P14P23

P15P

46= P14P

56+ P16P

45

Lauren K. Williams (Harvard) Cluster Algebras October 2019 1 / 23

Page 2: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Overview

Cluster algebras are commutative rings with distinguished generators(cluster variables) having a remarkable combinatorial structure.

The structure of a cluster algebra is encoded by a quiver, and therelations among the cluster variables are encoded by quiver mutation.

Cluster algebras were introduced by Fomin and Zelevinsky in 2000,motivated by total positivity and Lusztig’s canonical basis.

Cluster algebras have since appeared in many other contexts such as:

Poisson geometry

triangulations of surface and Teichmuller theory

mathematical physics: wall-crossing phenomena, quiver gaugetheories, scattering amplitudes, soliton solutions to the KP equation

Lauren K. Williams (Harvard) Cluster Algebras October 2019 2 / 23

Page 3: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Overview

Cluster algebras are commutative rings with distinguished generators(cluster variables) having a remarkable combinatorial structure.

The structure of a cluster algebra is encoded by a quiver, and therelations among the cluster variables are encoded by quiver mutation.

Cluster algebras were introduced by Fomin and Zelevinsky in 2000,motivated by total positivity and Lusztig’s canonical basis.

Cluster algebras have since appeared in many other contexts such as:

Poisson geometry

triangulations of surface and Teichmuller theory

mathematical physics: wall-crossing phenomena, quiver gaugetheories, scattering amplitudes, soliton solutions to the KP equation

Lauren K. Williams (Harvard) Cluster Algebras October 2019 2 / 23

Page 4: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Overview

Cluster algebras are commutative rings with distinguished generators(cluster variables) having a remarkable combinatorial structure.

The structure of a cluster algebra is encoded by a quiver, and therelations among the cluster variables are encoded by quiver mutation.

Cluster algebras were introduced by Fomin and Zelevinsky in 2000,motivated by total positivity and Lusztig’s canonical basis.

Cluster algebras have since appeared in many other contexts such as:

Poisson geometry

triangulations of surface and Teichmuller theory

mathematical physics: wall-crossing phenomena, quiver gaugetheories, scattering amplitudes, soliton solutions to the KP equation

Lauren K. Williams (Harvard) Cluster Algebras October 2019 2 / 23

Page 5: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Overview

Cluster algebras are commutative rings with distinguished generators(cluster variables) having a remarkable combinatorial structure.

The structure of a cluster algebra is encoded by a quiver, and therelations among the cluster variables are encoded by quiver mutation.

Cluster algebras were introduced by Fomin and Zelevinsky in 2000,motivated by total positivity and Lusztig’s canonical basis.

Cluster algebras have since appeared in many other contexts such as:

Poisson geometry

triangulations of surface and Teichmuller theory

mathematical physics: wall-crossing phenomena, quiver gaugetheories, scattering amplitudes, soliton solutions to the KP equation

Lauren K. Williams (Harvard) Cluster Algebras October 2019 2 / 23

Page 6: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Overview

Cluster algebras are commutative rings with distinguished generators(cluster variables) having a remarkable combinatorial structure.

The structure of a cluster algebra is encoded by a quiver, and therelations among the cluster variables are encoded by quiver mutation.

Cluster algebras were introduced by Fomin and Zelevinsky in 2000,motivated by total positivity and Lusztig’s canonical basis.

Cluster algebras have since appeared in many other contexts such as:

Poisson geometry

triangulations of surface and Teichmuller theory

mathematical physics: wall-crossing phenomena, quiver gaugetheories, scattering amplitudes, soliton solutions to the KP equation

Lauren K. Williams (Harvard) Cluster Algebras October 2019 2 / 23

Page 7: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Overview

Cluster algebras are commutative rings with distinguished generators(cluster variables) having a remarkable combinatorial structure.

The structure of a cluster algebra is encoded by a quiver, and therelations among the cluster variables are encoded by quiver mutation.

Cluster algebras were introduced by Fomin and Zelevinsky in 2000,motivated by total positivity and Lusztig’s canonical basis.

Cluster algebras have since appeared in many other contexts such as:

Poisson geometry

triangulations of surface and Teichmuller theory

mathematical physics: wall-crossing phenomena, quiver gaugetheories, scattering amplitudes, soliton solutions to the KP equation

Lauren K. Williams (Harvard) Cluster Algebras October 2019 2 / 23

Page 8: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Overview

Cluster algebras are commutative rings with distinguished generators(cluster variables) having a remarkable combinatorial structure.

The structure of a cluster algebra is encoded by a quiver, and therelations among the cluster variables are encoded by quiver mutation.

Cluster algebras were introduced by Fomin and Zelevinsky in 2000,motivated by total positivity and Lusztig’s canonical basis.

Cluster algebras have since appeared in many other contexts such as:

Poisson geometry

triangulations of surface and Teichmuller theory

mathematical physics: wall-crossing phenomena, quiver gaugetheories, scattering amplitudes, soliton solutions to the KP equation

Lauren K. Williams (Harvard) Cluster Algebras October 2019 2 / 23

Page 9: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Overview

Cluster algebras are commutative rings with distinguished generators(cluster variables) having a remarkable combinatorial structure.

The structure of a cluster algebra is encoded by a quiver, and therelations among the cluster variables are encoded by quiver mutation.

Cluster algebras were introduced by Fomin and Zelevinsky in 2000,motivated by total positivity and Lusztig’s canonical basis.

Cluster algebras have since appeared in many other contexts such as:

Poisson geometry

triangulations of surface and Teichmuller theory

mathematical physics: wall-crossing phenomena, quiver gaugetheories, scattering amplitudes, soliton solutions to the KP equation

Lauren K. Williams (Harvard) Cluster Algebras October 2019 2 / 23

Page 10: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 11: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 12: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 13: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 14: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 15: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 16: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 17: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 18: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 19: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 20: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 21: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Outline of the talk

Part 0: Motivation from total positivity

The Grassmannian and its positive part

Part I: What is a cluster algebra?

Quivers and quiver mutation

Seeds and seed mutation

Definition of cluster algebra

Example

Part II: Cluster algebras in nature

Cluster algebras and triangulations

Cluster algebras and surfaces

The positive Grassmannian, revisited

Lauren K. Williams (Harvard) Cluster Algebras October 2019 3 / 23

Page 22: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

The Grassmannian Grk,n(R) = {V | V ⊂ Rn, dimV = k}

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Can think of Grk,n(R) as Matk,n/ ∼.

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The totally positive part of the Grassmannian (Grk,n)>0 is the subset ofGrk,n(R) where all Plucker coordinates ∆I (A) > 0.

A k × n matrix A has(

nk

)

Plucker coordinates.How many (and which ones) do we need to test to determine whether Arepresents a point of (Grk,n)>0?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 4 / 23

Page 23: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

The Grassmannian Grk,n(R) = {V | V ⊂ Rn, dimV = k}

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Can think of Grk,n(R) as Matk,n/ ∼.

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The totally positive part of the Grassmannian (Grk,n)>0 is the subset ofGrk,n(R) where all Plucker coordinates ∆I (A) > 0.

A k × n matrix A has(

nk

)

Plucker coordinates.How many (and which ones) do we need to test to determine whether Arepresents a point of (Grk,n)>0?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 4 / 23

Page 24: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

The Grassmannian Grk,n(R) = {V | V ⊂ Rn, dimV = k}

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Can think of Grk,n(R) as Matk,n/ ∼.

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The totally positive part of the Grassmannian (Grk,n)>0 is the subset ofGrk,n(R) where all Plucker coordinates ∆I (A) > 0.

A k × n matrix A has(

nk

)

Plucker coordinates.How many (and which ones) do we need to test to determine whether Arepresents a point of (Grk,n)>0?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 4 / 23

Page 25: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

The Grassmannian Grk,n(R) = {V | V ⊂ Rn, dimV = k}

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Can think of Grk,n(R) as Matk,n/ ∼.

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The totally positive part of the Grassmannian (Grk,n)>0 is the subset ofGrk,n(R) where all Plucker coordinates ∆I (A) > 0.

A k × n matrix A has(

nk

)

Plucker coordinates.How many (and which ones) do we need to test to determine whether Arepresents a point of (Grk,n)>0?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 4 / 23

Page 26: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

The Grassmannian Grk,n(R) = {V | V ⊂ Rn, dimV = k}

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Can think of Grk,n(R) as Matk,n/ ∼.

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The totally positive part of the Grassmannian (Grk,n)>0 is the subset ofGrk,n(R) where all Plucker coordinates ∆I (A) > 0.

A k × n matrix A has(

nk

)

Plucker coordinates.How many (and which ones) do we need to test to determine whether Arepresents a point of (Grk,n)>0?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 4 / 23

Page 27: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

The Grassmannian Grk,n(R) = {V | V ⊂ Rn, dimV = k}

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Can think of Grk,n(R) as Matk,n/ ∼.

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The totally positive part of the Grassmannian (Grk,n)>0 is the subset ofGrk,n(R) where all Plucker coordinates ∆I (A) > 0.

A k × n matrix A has(

nk

)

Plucker coordinates.How many (and which ones) do we need to test to determine whether Arepresents a point of (Grk,n)>0?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 4 / 23

Page 28: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

The Grassmannian Grk,n(R) = {V | V ⊂ Rn, dimV = k}

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Can think of Grk,n(R) as Matk,n/ ∼.

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The totally positive part of the Grassmannian (Grk,n)>0 is the subset ofGrk,n(R) where all Plucker coordinates ∆I (A) > 0.

A k × n matrix A has(

nk

)

Plucker coordinates.How many (and which ones) do we need to test to determine whether Arepresents a point of (Grk,n)>0?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 4 / 23

Page 29: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

The Grassmannian Grk,n(R) = {V | V ⊂ Rn, dimV = k}

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Can think of Grk,n(R) as Matk,n/ ∼.

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The totally positive part of the Grassmannian (Grk,n)>0 is the subset ofGrk,n(R) where all Plucker coordinates ∆I (A) > 0.

A k × n matrix A has(

nk

)

Plucker coordinates.How many (and which ones) do we need to test to determine whether Arepresents a point of (Grk,n)>0?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 4 / 23

Page 30: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

The Grassmannian Grk,n(R) = {V | V ⊂ Rn, dimV = k}

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Can think of Grk,n(R) as Matk,n/ ∼.

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The totally positive part of the Grassmannian (Grk,n)>0 is the subset ofGrk,n(R) where all Plucker coordinates ∆I (A) > 0.

A k × n matrix A has(

nk

)

Plucker coordinates.How many (and which ones) do we need to test to determine whether Arepresents a point of (Grk,n)>0?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 4 / 23

Page 31: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The Plucker coordinates satisfy

∆13(A)∆24(A) = ∆12(A)∆34(A) + ∆14(A)∆23(A).

So if ∆12,∆23,∆34,∆14 and ∆24 are positive, so is ∆13.Or if ∆12,∆23,∆34,∆14 and ∆13 are positive, so is ∆24.

How can we generalize this picture to Gr2,n(R)? Grk,n(R)?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 5 / 23

Page 32: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The Plucker coordinates satisfy

∆13(A)∆24(A) = ∆12(A)∆34(A) + ∆14(A)∆23(A).

So if ∆12,∆23,∆34,∆14 and ∆24 are positive, so is ∆13.Or if ∆12,∆23,∆34,∆14 and ∆13 are positive, so is ∆24.

How can we generalize this picture to Gr2,n(R)? Grk,n(R)?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 5 / 23

Page 33: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The Plucker coordinates satisfy

∆13(A)∆24(A) = ∆12(A)∆34(A) + ∆14(A)∆23(A).

So if ∆12,∆23,∆34,∆14 and ∆24 are positive, so is ∆13.Or if ∆12,∆23,∆34,∆14 and ∆13 are positive, so is ∆24.

How can we generalize this picture to Gr2,n(R)? Grk,n(R)?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 5 / 23

Page 34: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The Plucker coordinates satisfy

∆13(A)∆24(A) = ∆12(A)∆34(A) + ∆14(A)∆23(A).

So if ∆12,∆23,∆34,∆14 and ∆24 are positive, so is ∆13.Or if ∆12,∆23,∆34,∆14 and ∆13 are positive, so is ∆24.

How can we generalize this picture to Gr2,n(R)? Grk,n(R)?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 5 / 23

Page 35: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The Plucker coordinates satisfy

∆13(A)∆24(A) = ∆12(A)∆34(A) + ∆14(A)∆23(A).

So if ∆12,∆23,∆34,∆14 and ∆24 are positive, so is ∆13.Or if ∆12,∆23,∆34,∆14 and ∆13 are positive, so is ∆24.

How can we generalize this picture to Gr2,n(R)? Grk,n(R)?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 5 / 23

Page 36: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

The Grassmannian and its positive part

Represent an element of Grk,n(R) by a full-rank k × n matrix A.

(

1 0 −1 −20 1 3 2

)

Given I ∈([n]k

)

, the Plucker coordinate ∆I (A) is the minor of the k × k

submatrix of A in column set I .

The Plucker coordinates satisfy

∆13(A)∆24(A) = ∆12(A)∆34(A) + ∆14(A)∆23(A).

So if ∆12,∆23,∆34,∆14 and ∆24 are positive, so is ∆13.Or if ∆12,∆23,∆34,∆14 and ∆13 are positive, so is ∆24.

How can we generalize this picture to Gr2,n(R)? Grk,n(R)?

Lauren K. Williams (Harvard) Cluster Algebras October 2019 5 / 23

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Quivers

A quiver is a finite directed graph.Multiple edges are allowed.Oriented cycles of length 1 or 2 are forbidden.Two types of vertices: “frozen” and “mutable.”Ignore edges connecting frozen vertices.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 6 / 23

Page 38: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quivers

A quiver is a finite directed graph.Multiple edges are allowed.Oriented cycles of length 1 or 2 are forbidden.Two types of vertices: “frozen” and “mutable.”Ignore edges connecting frozen vertices.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 6 / 23

Page 39: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quivers

A quiver is a finite directed graph.Multiple edges are allowed.Oriented cycles of length 1 or 2 are forbidden.Two types of vertices: “frozen” and “mutable.”Ignore edges connecting frozen vertices.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 6 / 23

Page 40: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quivers

A quiver is a finite directed graph.Multiple edges are allowed.Oriented cycles of length 1 or 2 are forbidden.Two types of vertices: “frozen” and “mutable.”Ignore edges connecting frozen vertices.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 6 / 23

Page 41: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quivers

A quiver is a finite directed graph.Multiple edges are allowed.Oriented cycles of length 1 or 2 are forbidden.Two types of vertices: “frozen” and “mutable.”Ignore edges connecting frozen vertices.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 6 / 23

Page 42: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quiver Mutation

k

Let k be a mutable vertex of Q.

Quiver mutation µk : Q 7→ Q ′ is computed in 3 steps:

1. For each instance of j → k → ℓ, introduce an edge j → ℓ.2. Reverse the direction of all edges incident to k .3. Remove oriented 2-cycles.

Mutation is an involution, i.e. µ2k(Q) = Q for each vertex k .

Two quivers are mutation-equivalent if one can get between them via asequence of mutations. Show aplet.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 7 / 23

Page 43: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quiver Mutation

k

Let k be a mutable vertex of Q.

Quiver mutation µk : Q 7→ Q ′ is computed in 3 steps:

1. For each instance of j → k → ℓ, introduce an edge j → ℓ.2. Reverse the direction of all edges incident to k .3. Remove oriented 2-cycles.

Mutation is an involution, i.e. µ2k(Q) = Q for each vertex k .

Two quivers are mutation-equivalent if one can get between them via asequence of mutations. Show aplet.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 7 / 23

Page 44: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quiver Mutation

k k

Let k be a mutable vertex of Q.

Quiver mutation µk : Q 7→ Q ′ is computed in 3 steps:

1. For each instance of j → k → ℓ, introduce an edge j → ℓ.2. Reverse the direction of all edges incident to k .3. Remove oriented 2-cycles.

Mutation is an involution, i.e. µ2k(Q) = Q for each vertex k .

Two quivers are mutation-equivalent if one can get between them via asequence of mutations. Show aplet.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 7 / 23

Page 45: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quiver Mutation

k k

Let k be a mutable vertex of Q.

Quiver mutation µk : Q 7→ Q ′ is computed in 3 steps:

1. For each instance of j → k → ℓ, introduce an edge j → ℓ.2. Reverse the direction of all edges incident to k .3. Remove oriented 2-cycles.

Mutation is an involution, i.e. µ2k(Q) = Q for each vertex k .

Two quivers are mutation-equivalent if one can get between them via asequence of mutations. Show aplet.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 7 / 23

Page 46: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quiver Mutation

k k k

Let k be a mutable vertex of Q.

Quiver mutation µk : Q 7→ Q ′ is computed in 3 steps:

1. For each instance of j → k → ℓ, introduce an edge j → ℓ.2. Reverse the direction of all edges incident to k .3. Remove oriented 2-cycles.

Mutation is an involution, i.e. µ2k(Q) = Q for each vertex k .

Two quivers are mutation-equivalent if one can get between them via asequence of mutations. Show aplet.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 7 / 23

Page 47: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quiver Mutation

k k k

Let k be a mutable vertex of Q.

Quiver mutation µk : Q 7→ Q ′ is computed in 3 steps:

1. For each instance of j → k → ℓ, introduce an edge j → ℓ.2. Reverse the direction of all edges incident to k .3. Remove oriented 2-cycles.

Mutation is an involution, i.e. µ2k(Q) = Q for each vertex k .

Two quivers are mutation-equivalent if one can get between them via asequence of mutations. Show aplet.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 7 / 23

Page 48: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quiver Mutation

k k k k

Let k be a mutable vertex of Q.

Quiver mutation µk : Q 7→ Q ′ is computed in 3 steps:

1. For each instance of j → k → ℓ, introduce an edge j → ℓ.2. Reverse the direction of all edges incident to k .3. Remove oriented 2-cycles.

Mutation is an involution, i.e. µ2k(Q) = Q for each vertex k .

Two quivers are mutation-equivalent if one can get between them via asequence of mutations. Show aplet.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 7 / 23

Page 49: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quiver Mutation

k k k k

Let k be a mutable vertex of Q.

Quiver mutation µk : Q 7→ Q ′ is computed in 3 steps:

1. For each instance of j → k → ℓ, introduce an edge j → ℓ.2. Reverse the direction of all edges incident to k .3. Remove oriented 2-cycles.

Mutation is an involution, i.e. µ2k(Q) = Q for each vertex k .

Two quivers are mutation-equivalent if one can get between them via asequence of mutations. Show aplet.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 7 / 23

Page 50: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Quiver Mutation

k k k k

Let k be a mutable vertex of Q.

Quiver mutation µk : Q 7→ Q ′ is computed in 3 steps:

1. For each instance of j → k → ℓ, introduce an edge j → ℓ.2. Reverse the direction of all edges incident to k .3. Remove oriented 2-cycles.

Mutation is an involution, i.e. µ2k(Q) = Q for each vertex k .

Two quivers are mutation-equivalent if one can get between them via asequence of mutations. Show aplet.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 7 / 23

Page 51: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seeds

Let F be a field of rational functions in m independent variables over C.A seed in F is a pair (Q, x) consisting of:

a quiver Q on m vertices

an extended cluster x, an m-tuple of algebraically independent (overC) elements of F , indexed by the vertices of Q.

coefficient variables ↔ frozen vertices

cluster variables ↔ mutable vertices

Cluster = {cluster variables }

Extended Cluster = {cluster variables, coefficient variables}

Lauren K. Williams (Harvard) Cluster Algebras October 2019 8 / 23

Page 52: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seeds

Let F be a field of rational functions in m independent variables over C.A seed in F is a pair (Q, x) consisting of:

a quiver Q on m vertices

an extended cluster x, an m-tuple of algebraically independent (overC) elements of F , indexed by the vertices of Q.

coefficient variables ↔ frozen vertices

cluster variables ↔ mutable vertices

Cluster = {cluster variables }

Extended Cluster = {cluster variables, coefficient variables}

Lauren K. Williams (Harvard) Cluster Algebras October 2019 8 / 23

Page 53: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seeds

Let F be a field of rational functions in m independent variables over C.A seed in F is a pair (Q, x) consisting of:

a quiver Q on m vertices

an extended cluster x, an m-tuple of algebraically independent (overC) elements of F , indexed by the vertices of Q.

coefficient variables ↔ frozen vertices

cluster variables ↔ mutable vertices

Cluster = {cluster variables }

Extended Cluster = {cluster variables, coefficient variables}

Lauren K. Williams (Harvard) Cluster Algebras October 2019 8 / 23

Page 54: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seeds

Let F be a field of rational functions in m independent variables over C.A seed in F is a pair (Q, x) consisting of:

a quiver Q on m vertices

an extended cluster x, an m-tuple of algebraically independent (overC) elements of F , indexed by the vertices of Q.

coefficient variables ↔ frozen vertices

cluster variables ↔ mutable vertices

Cluster = {cluster variables }

Extended Cluster = {cluster variables, coefficient variables}

Lauren K. Williams (Harvard) Cluster Algebras October 2019 8 / 23

Page 55: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seeds

Let F be a field of rational functions in m independent variables over C.A seed in F is a pair (Q, x) consisting of:

a quiver Q on m vertices

an extended cluster x, an m-tuple of algebraically independent (overC) elements of F , indexed by the vertices of Q.

coefficient variables ↔ frozen vertices

cluster variables ↔ mutable vertices

Cluster = {cluster variables }

Extended Cluster = {cluster variables, coefficient variables}

Lauren K. Williams (Harvard) Cluster Algebras October 2019 8 / 23

Page 56: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seed mutation

Let k be a mutable vertex in Q and let xk be the corresponding clustervariable. Then the seed mutation µk : (Q, x) 7→ (Q ′, x′) is defined by

Q ′ = µk(Q)

x′ = x ∪ {x ′k} \ {xk}, where

xkx′

k =∏

j←k

xj +∏

j→k

xj (is the exchange relation)

Remark: Mutation is an involution.

Example

Lauren K. Williams (Harvard) Cluster Algebras October 2019 9 / 23

Page 57: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seed mutation

Let k be a mutable vertex in Q and let xk be the corresponding clustervariable. Then the seed mutation µk : (Q, x) 7→ (Q ′, x′) is defined by

Q ′ = µk(Q)

x′ = x ∪ {x ′k} \ {xk}, where

xkx′

k =∏

j←k

xj +∏

j→k

xj (is the exchange relation)

Remark: Mutation is an involution.

Example

Lauren K. Williams (Harvard) Cluster Algebras October 2019 9 / 23

Page 58: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seed mutation

Let k be a mutable vertex in Q and let xk be the corresponding clustervariable. Then the seed mutation µk : (Q, x) 7→ (Q ′, x′) is defined by

Q ′ = µk(Q)

x′ = x ∪ {x ′k} \ {xk}, where

xkx′

k =∏

j←k

xj +∏

j→k

xj (is the exchange relation)

Remark: Mutation is an involution.

Example

Lauren K. Williams (Harvard) Cluster Algebras October 2019 9 / 23

Page 59: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seed mutation

Let k be a mutable vertex in Q and let xk be the corresponding clustervariable. Then the seed mutation µk : (Q, x) 7→ (Q ′, x′) is defined by

Q ′ = µk(Q)

x′ = x ∪ {x ′k} \ {xk}, where

xkx′

k =∏

j←k

xj +∏

j→k

xj (is the exchange relation)

Remark: Mutation is an involution.

Example

Lauren K. Williams (Harvard) Cluster Algebras October 2019 9 / 23

Page 60: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seed mutation

Let k be a mutable vertex in Q and let xk be the corresponding clustervariable. Then the seed mutation µk : (Q, x) 7→ (Q ′, x′) is defined by

Q ′ = µk(Q)

x′ = x ∪ {x ′k} \ {xk}, where

xkx′

k =∏

j←k

xj +∏

j→k

xj (is the exchange relation)

Remark: Mutation is an involution.

Example

Lauren K. Williams (Harvard) Cluster Algebras October 2019 9 / 23

Page 61: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seed mutation

Let k be a mutable vertex in Q and let xk be the corresponding clustervariable. Then the seed mutation µk : (Q, x) 7→ (Q ′, x′) is defined by

Q ′ = µk(Q)

x′ = x ∪ {x ′k} \ {xk}, where

xkx′

k =∏

j←k

xj +∏

j→k

xj (is the exchange relation)

Remark: Mutation is an involution.

Example

x1 x2 x3

x4 x5 x6

Lauren K. Williams (Harvard) Cluster Algebras October 2019 9 / 23

Page 62: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Seed mutation

Let k be a mutable vertex in Q and let xk be the corresponding clustervariable. Then the seed mutation µk : (Q, x) 7→ (Q ′, x′) is defined by

Q ′ = µk(Q)

x′ = x ∪ {x ′k} \ {xk}, where

xkx′

k =∏

j←k

xj +∏

j→k

xj (is the exchange relation)

Remark: Mutation is an involution.

Example

x1 x2 x3

x4 x5 x6

x1 x3

x4 x5 x6

µ2

x21x3+x5x2

Lauren K. Williams (Harvard) Cluster Algebras October 2019 9 / 23

Page 63: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Definition of cluster algebra

µ3

µ3 µ3

µ1

(Q, x)µ2

µ1µ2

Let (Q, x) be a seed in F , where Q has n mutable vertices.Consider the n-regular tree T with vertices labeled by seeds, obtained byapplying all possible sequences of mutations to (Q, x).Let χ be the union of all cluster variables which appear at all nodes of T.The cluster algebra A = A(Q) is the subring of F which is generated by χ.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 10 / 23

Page 64: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Definition of cluster algebra

µ3

µ3 µ3

µ1

(Q, x)µ2

µ1µ2

Let (Q, x) be a seed in F , where Q has n mutable vertices.Consider the n-regular tree T with vertices labeled by seeds, obtained byapplying all possible sequences of mutations to (Q, x).Let χ be the union of all cluster variables which appear at all nodes of T.The cluster algebra A = A(Q) is the subring of F which is generated by χ.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 10 / 23

Page 65: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Definition of cluster algebra

µ3

µ3 µ3

µ1

(Q, x)µ2

µ1µ2

Let (Q, x) be a seed in F , where Q has n mutable vertices.Consider the n-regular tree T with vertices labeled by seeds, obtained byapplying all possible sequences of mutations to (Q, x).Let χ be the union of all cluster variables which appear at all nodes of T.The cluster algebra A = A(Q) is the subring of F which is generated by χ.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 10 / 23

Page 66: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Definition of cluster algebra

µ3

µ3 µ3

µ1

(Q, x)µ2

µ1µ2

Let (Q, x) be a seed in F , where Q has n mutable vertices.Consider the n-regular tree T with vertices labeled by seeds, obtained byapplying all possible sequences of mutations to (Q, x).Let χ be the union of all cluster variables which appear at all nodes of T.The cluster algebra A = A(Q) is the subring of F which is generated by χ.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 10 / 23

Page 67: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 68: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 69: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1 1 2

1+x2x1

1+x1+x2x1x2

µ2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 70: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1 1 2

1+x2x1

1+x1+x2x1x2

µ2

21

1+x1x2

1+x1+x2x1x2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 71: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1 1 2

1+x2x1

1+x1+x2x1x2

µ2

1 2

1+x1x2

x1

µ2 21

1+x1x2

1+x1+x2x1x2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 72: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1 1 2

1+x2x1

1+x1+x2x1x2

µ2

1 2

x2 x1

µ1 1 2

1+x1x2

x1

µ2 21

1+x1x2

1+x1+x2x1x2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 73: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1 1 2

1+x2x1

1+x1+x2x1x2

µ2

1 2

x2 x1

µ1 1 2

1+x1x2

x1

µ2 21

1+x1x2

1+x1+x2x1x2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 74: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1 1 2

1+x2x1

1+x1+x2x1x2

µ2

1 2

x2 x1

µ1 1 2

1+x1x2

x1

µ2 21

1+x1x2

1+x1+x2x1x2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 75: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1 1 2

1+x2x1

1+x1+x2x1x2

µ2

1 2

x2 x1

µ1 1 2

1+x1x2

x1

µ2 21

1+x1x2

1+x1+x2x1x2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

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Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1 1 2

1+x2x1

1+x1+x2x1x2

µ2

1 2

x2 x1

µ1 1 2

1+x1x2

x1

µ2 21

1+x1x2

1+x1+x2x1x2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 77: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Example

Consider the following seed (Q, x), where x = {x1, x2}.

1 2

x1 x2

1 2

1+x2x1

x2

µ1 1 2

1+x2x1

1+x1+x2x1x2

µ2

1 2

x2 x1

µ1 1 2

1+x1x2

x1

µ2 21

1+x1x2

1+x1+x2x1x2

The cluster algebra A(Q) is the subring of F = C(x1, x2) generated by allcluster variables χ = {x1, x2,

1+x2x1

, 1+x1+x2x1x2

, 1+x1x2

.}

Note: every cluster variable is a Laurent polynomial in {x1, x2}.Note: each Laurent polynomial has positive coefficients.Note: there are finitely many cluster variables.The 2-regular tree closes up to form a pentagon.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 11 / 23

Page 78: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Fundamental results

Let A = A(Q) be an arbitrary cluster algebra, with initial seed (Q, x).

Laurent phenomenon (Fomin + Zelevinsky)

Every cluster variable is a Laurent polynomial in the variables from x

(the initial cluster variables).

Positivity Theorem (Lee-Schiffler, Gross-Hacking-Keel)

Each such Laurent polynomial has positive coefficients.

Finite type classification (Fomin + Zelevinsky)

We say A has finite type if there are only finitely many cluster variables.The finite type cluster algebras are classified by Dynkin diagrams.When A is of finite type, the n-regular tree closes up on itself andbecomes the 1-skeleton of a convex polytope.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 12 / 23

Page 79: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Fundamental results

Let A = A(Q) be an arbitrary cluster algebra, with initial seed (Q, x).

Laurent phenomenon (Fomin + Zelevinsky)

Every cluster variable is a Laurent polynomial in the variables from x

(the initial cluster variables).

Positivity Theorem (Lee-Schiffler, Gross-Hacking-Keel)

Each such Laurent polynomial has positive coefficients.

Finite type classification (Fomin + Zelevinsky)

We say A has finite type if there are only finitely many cluster variables.The finite type cluster algebras are classified by Dynkin diagrams.When A is of finite type, the n-regular tree closes up on itself andbecomes the 1-skeleton of a convex polytope.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 12 / 23

Page 80: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Fundamental results

Let A = A(Q) be an arbitrary cluster algebra, with initial seed (Q, x).

Laurent phenomenon (Fomin + Zelevinsky)

Every cluster variable is a Laurent polynomial in the variables from x

(the initial cluster variables).

Positivity Theorem (Lee-Schiffler, Gross-Hacking-Keel)

Each such Laurent polynomial has positive coefficients.

Finite type classification (Fomin + Zelevinsky)

We say A has finite type if there are only finitely many cluster variables.The finite type cluster algebras are classified by Dynkin diagrams.When A is of finite type, the n-regular tree closes up on itself andbecomes the 1-skeleton of a convex polytope.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 12 / 23

Page 81: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Fundamental results

Let A = A(Q) be an arbitrary cluster algebra, with initial seed (Q, x).

Laurent phenomenon (Fomin + Zelevinsky)

Every cluster variable is a Laurent polynomial in the variables from x

(the initial cluster variables).

Positivity Theorem (Lee-Schiffler, Gross-Hacking-Keel)

Each such Laurent polynomial has positive coefficients.

Finite type classification (Fomin + Zelevinsky)

We say A has finite type if there are only finitely many cluster variables.The finite type cluster algebras are classified by Dynkin diagrams.When A is of finite type, the n-regular tree closes up on itself andbecomes the 1-skeleton of a convex polytope.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 12 / 23

Page 82: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Fundamental results

Let A = A(Q) be an arbitrary cluster algebra, with initial seed (Q, x).

Laurent phenomenon (Fomin + Zelevinsky)

Every cluster variable is a Laurent polynomial in the variables from x

(the initial cluster variables).

Positivity Theorem (Lee-Schiffler, Gross-Hacking-Keel)

Each such Laurent polynomial has positive coefficients.

Finite type classification (Fomin + Zelevinsky)

We say A has finite type if there are only finitely many cluster variables.The finite type cluster algebras are classified by Dynkin diagrams.When A is of finite type, the n-regular tree closes up on itself andbecomes the 1-skeleton of a convex polytope.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 12 / 23

Page 83: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Fundamental results

Let A = A(Q) be an arbitrary cluster algebra, with initial seed (Q, x).

Laurent phenomenon (Fomin + Zelevinsky)

Every cluster variable is a Laurent polynomial in the variables from x

(the initial cluster variables).

Positivity Theorem (Lee-Schiffler, Gross-Hacking-Keel)

Each such Laurent polynomial has positive coefficients.

Finite type classification (Fomin + Zelevinsky)

We say A has finite type if there are only finitely many cluster variables.The finite type cluster algebras are classified by Dynkin diagrams.When A is of finite type, the n-regular tree closes up on itself andbecomes the 1-skeleton of a convex polytope.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 12 / 23

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Cluster algebras and triangulations

Fix a triangulation T of a d -gon. We associate to it a quiver QT :

12

3

45

6

7

8

9

10

11

12

13

This gives rise to a cluster algebra A(QT ), with initial seed(QT , {x1, . . . , x2d−3}).

Lauren K. Williams (Harvard) Cluster Algebras October 2019 13 / 23

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Cluster algebras and triangulations

Fix a triangulation T of a d -gon. We associate to it a quiver QT :

12

3

45

6

7

8

9

10

11

12

13

12

3

45

6

7

8

9

10

11

12

13

This gives rise to a cluster algebra A(QT ), with initial seed(QT , {x1, . . . , x2d−3}).

Lauren K. Williams (Harvard) Cluster Algebras October 2019 13 / 23

Page 86: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Cluster algebras and triangulations

Fix a triangulation T of a d -gon. We associate to it a quiver QT :

12

3

45

6

7

8

9

10

11

12

13

12

3

45

6

7

8

9

10

11

12

13

This gives rise to a cluster algebra A(QT ), with initial seed(QT , {x1, . . . , x2d−3}).

Lauren K. Williams (Harvard) Cluster Algebras October 2019 13 / 23

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The set of triangulations of a polygon is connected by flips.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 14 / 23

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The set of triangulations of a polygon is connected by flips.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 14 / 23

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The set of triangulations of a polygon is connected by flips.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 14 / 23

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Flips correspond to mutations.

Note that µ2(QT ) = QT ′ .

Lauren K. Williams (Harvard) Cluster Algebras October 2019 15 / 23

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Flips correspond to mutations.

T

12

3

45

6

7

8

9

10

11

12

13

Note that µ2(QT ) = QT ′ .

Lauren K. Williams (Harvard) Cluster Algebras October 2019 15 / 23

Page 92: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Flips correspond to mutations.

T

12

3

45

6

7

8

9

10

11

12

13

T ′

1

3

45

6

7

8

9

10

11

12

13

2’

Note that µ2(QT ) = QT ′ .

Lauren K. Williams (Harvard) Cluster Algebras October 2019 15 / 23

Page 93: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Flips correspond to mutations.

T

12

3

45

6

7

8

9

10

11

12

13

T ′

1

3

45

6

7

8

9

10

11

12

13

2’

QT

12

3

45

6

7

8

9

10

11

12

13

Note that µ2(QT ) = QT ′ .

Lauren K. Williams (Harvard) Cluster Algebras October 2019 15 / 23

Page 94: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Flips correspond to mutations.

T

12

3

45

6

7

8

9

10

11

12

13

T ′

1

3

45

6

7

8

9

10

11

12

13

2’

QT

12

3

45

6

7

8

9

10

11

12

13

QT ′

1

3

45

6

7

8

9

10

11

12

13

2’

Note that µ2(QT ) = QT ′ .

Lauren K. Williams (Harvard) Cluster Algebras October 2019 15 / 23

Page 95: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Flips correspond to mutations.

T

12

3

45

6

7

8

9

10

11

12

13

T ′

1

3

45

6

7

8

9

10

11

12

13

2’

QT

12

3

45

6

7

8

9

10

11

12

13

QT ′

1

3

45

6

7

8

9

10

11

12

13

2’

Note that µ2(QT ) = QT ′ .

Lauren K. Williams (Harvard) Cluster Algebras October 2019 15 / 23

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Cluster algebras and triangulations of a polygon

T

12

3

45

6

7

8

9

10

11

12

13

Triangulations are connected by flips, and flips ↔ mutations. Moreover:

seeds ↔ the triangulations of the polygon

coefficient variables ↔ the d sides of the polygon

cluster variables ↔ thed(d − 3)

2diagonals of the polygon

Lauren K. Williams (Harvard) Cluster Algebras October 2019 16 / 23

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Cluster algebras and triangulations of a polygon

T

12

3

45

6

7

8

9

10

11

12

13

QT

12

3

45

6

7

8

9

10

11

12

13

Triangulations are connected by flips, and flips ↔ mutations. Moreover:

seeds ↔ the triangulations of the polygon

coefficient variables ↔ the d sides of the polygon

cluster variables ↔ thed(d − 3)

2diagonals of the polygon

Lauren K. Williams (Harvard) Cluster Algebras October 2019 16 / 23

Page 98: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Cluster algebras and triangulations of a polygon

T

12

3

45

6

7

8

9

10

11

12

13

QT

12

3

45

6

7

8

9

10

11

12

13

Triangulations are connected by flips, and flips ↔ mutations. Moreover:

seeds ↔ the triangulations of the polygon

coefficient variables ↔ the d sides of the polygon

cluster variables ↔ thed(d − 3)

2diagonals of the polygon

Lauren K. Williams (Harvard) Cluster Algebras October 2019 16 / 23

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Cluster algebras and triangulations of a polygon

T

12

3

45

6

7

8

9

10

11

12

13

QT

12

3

45

6

7

8

9

10

11

12

13

Triangulations are connected by flips, and flips ↔ mutations. Moreover:

seeds ↔ the triangulations of the polygon

coefficient variables ↔ the d sides of the polygon

cluster variables ↔ thed(d − 3)

2diagonals of the polygon

Lauren K. Williams (Harvard) Cluster Algebras October 2019 16 / 23

Page 100: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Cluster algebras and triangulations of a polygon

T

12

3

45

6

7

8

9

10

11

12

13

QT

12

3

45

6

7

8

9

10

11

12

13

Triangulations are connected by flips, and flips ↔ mutations. Moreover:

seeds ↔ the triangulations of the polygon

coefficient variables ↔ the d sides of the polygon

cluster variables ↔ thed(d − 3)

2diagonals of the polygon

Lauren K. Williams (Harvard) Cluster Algebras October 2019 16 / 23

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Cluster algebras and triangulations of a polygon

T

12

3

45

6

7

8

9

10

11

12

13

QT

12

3

45

6

7

8

9

10

11

12

13

Triangulations are connected by flips, and flips ↔ mutations. Moreover:

seeds ↔ the triangulations of the polygon

coefficient variables ↔ the d sides of the polygon

cluster variables ↔ thed(d − 3)

2diagonals of the polygon

Lauren K. Williams (Harvard) Cluster Algebras October 2019 16 / 23

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Cluster algebras and triangulations of a polygon

T

12

3

45

6

7

8

9

10

11

12

13

QT

12

3

45

6

7

8

9

10

11

12

13

Triangulations are connected by flips, and flips ↔ mutations. Moreover:

seeds ↔ the triangulations of the polygon

coefficient variables ↔ the d sides of the polygon

cluster variables ↔ thed(d − 3)

2diagonals of the polygon

Exchange relation:

i

k

h xhx′

h = xixk + xjxℓℓ j

Lauren K. Williams (Harvard) Cluster Algebras October 2019 16 / 23

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Cluster algebras and triangulations of a polygon

Relabel the triangulation, and coefficient/cluster variables as follows:

This identifies our cluster algebra with the coordinate ring of theGrassmannian C[Gr2,d ]!

Lauren K. Williams (Harvard) Cluster Algebras October 2019 17 / 23

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Cluster algebras and triangulations of a polygon

Relabel the triangulation, and coefficient/cluster variables as follows:

This identifies our cluster algebra with the coordinate ring of theGrassmannian C[Gr2,d ]!

Lauren K. Williams (Harvard) Cluster Algebras October 2019 17 / 23

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Cluster algebras and triangulations of a polygon

Relabel the triangulation, and coefficient/cluster variables as follows:

p

p

p

p

pp

p

p

p

p p

p

1 2

3

4

56

7

8

12

23

34

45

56

67

78 17 16

13

36

35

p18

p

p

p

p

p

p

p

18p

12

23

34

45

56

67

78

p

p

p

16

1713

This identifies our cluster algebra with the coordinate ring of theGrassmannian C[Gr2,d ]!

Lauren K. Williams (Harvard) Cluster Algebras October 2019 17 / 23

Page 106: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Cluster algebras and triangulations of a polygon

Relabel the triangulation, and coefficient/cluster variables as follows:

p

p

p

p

pp

p

p

p

p p

p

1 2

3

4

56

7

8

12

23

34

45

56

67

78 17 16

13

36

35

p18

p

p

p

p

p

p

p

18p

12

23

34

45

56

67

78

p

p

p

16

1713

Exchange relation:

bpaba

d pcd

pac pacpbd = pabpcd + pbcpadpbcpad

c

This identifies our cluster algebra with the coordinate ring of theGrassmannian C[Gr2,d ]!

Lauren K. Williams (Harvard) Cluster Algebras October 2019 17 / 23

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Cluster algebras and triangulations of a polygon

Relabel the triangulation, and coefficient/cluster variables as follows:

p

p

p

p

pp

p

p

p

p p

p

1 2

3

4

56

7

8

12

23

34

45

56

67

78 17 16

13

36

35

p18

p

p

p

p

p

p

p

18p

12

23

34

45

56

67

78

p

p

p

16

1713

Exchange relation:

bpaba

d pcd

pac pacpbd = pabpcd + pbcpadpbcpad

c

This identifies our cluster algebra with the coordinate ring of theGrassmannian C[Gr2,d ]!

Lauren K. Williams (Harvard) Cluster Algebras October 2019 17 / 23

Page 108: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Cluster algebras and triangulations of a polygon

Relabel the triangulation, and coefficient/cluster variables as follows:

p

p

p

p

pp

p

p

p

p p

p

1 2

3

4

56

7

8

12

23

34

45

56

67

78 17 16

13

36

35

p18

p

p

p

p

p

p

p

18p

12

23

34

45

56

67

78

p

p

p

16

1713

Exchange relation:

bpaba

d pcd

pac pacpbd = pabpcd + pbcpadpbcpad

c

This identifies our cluster algebra with the coordinate ring of theGrassmannian C[Gr2,d ]! Every cluster (triangulation) gives rise to apositivity test for membership in (Gr2,d )>0.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 17 / 23

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Cluster algebras and triangulations of a polygon

Relabel the triangulation, and coefficient/cluster variables as follows:

p

p

p

p

pp

p

p

p

p p

p

1 2

3

4

56

7

8

12

23

34

45

56

67

78 17 16

13

36

35

p18

p

p

p

p

p

p

p

18p

12

23

34

45

56

67

78

p

p

p

16

1713

Exchange relation:

bpaba

d pcd

pac pacpbd = pabpcd + pbcpadpbcpad

c

This identifies our cluster algebra with the coordinate ring of theGrassmannian C[Gr2,d ]! Every cluster (triangulation) gives rise to apositivity test for membership in (Gr2,d )>0. (Why?)

Lauren K. Williams (Harvard) Cluster Algebras October 2019 17 / 23

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Cluster algebras and triangulations of a polygon

The cluster algebra associated to C[Gr2,d ] can be visualized using theassociahedron:

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

P13P24

= P12P34

+ P14P23

P15P

46= P14P

56+ P16P

45

Lauren K. Williams (Harvard) Cluster Algebras October 2019 18 / 23

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Two generalizations of this cluster algebra

| |

Cluster algebra fromtriangulations of a polygon

C[Gr2,d ]

Lauren K. Williams (Harvard) Cluster Algebras October 2019 19 / 23

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Two generalizations of this cluster algebra

| |

Cluster algebra fromtriangulations of a polygon

C[Gr2,d ]

Cluster algebra fromtriangulations of a Riemann surface

Teichmuller theory

Lauren K. Williams (Harvard) Cluster Algebras October 2019 19 / 23

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Two generalizations of this cluster algebra

| |

Cluster algebra fromtriangulations of a polygon

C[Gr2,d ]

Cluster algebra fromtriangulations of a Riemann surface

Teichmuller theory

The coordinate ringC[Grk,d ]

Lauren K. Williams (Harvard) Cluster Algebras October 2019 19 / 23

Page 114: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

First generalization: polygon surface

Recall that given a triangulation of a polygon, we can construct a quiverand an associated cluster algebra.

Idea: if we have an oriented surface with some marked points, we cantriangulate it, and construct a quiver as before!

To be continued in the next lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 20 / 23

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First generalization: polygon surface

Recall that given a triangulation of a polygon, we can construct a quiverand an associated cluster algebra.

T

12

3

45

6

7

8

9

10

11

12

13

QT

12

3

45

6

7

8

9

10

11

12

13

Idea: if we have an oriented surface with some marked points, we cantriangulate it, and construct a quiver as before!

To be continued in the next lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 20 / 23

Page 116: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

First generalization: polygon surface

Recall that given a triangulation of a polygon, we can construct a quiverand an associated cluster algebra.

T

12

3

45

6

7

8

9

10

11

12

13

QT

12

3

45

6

7

8

9

10

11

12

13

Idea: if we have an oriented surface with some marked points, we cantriangulate it, and construct a quiver as before!

To be continued in the next lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 20 / 23

Page 117: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

First generalization: polygon surface

Recall that given a triangulation of a polygon, we can construct a quiverand an associated cluster algebra.

T

12

3

45

6

7

8

9

10

11

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13

QT

12

3

45

6

7

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9

10

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12

13

Idea: if we have an oriented surface with some marked points, we cantriangulate it, and construct a quiver as before!

To be continued in the next lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 20 / 23

Page 118: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 119: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gon

To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 120: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gon

To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 121: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gon

←→

To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 122: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gon

←→

To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 123: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gon

←→

To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 124: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gon

←→

To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 125: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gonsquare moves ←→ flips of triangulations

←→

To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 126: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gonsquare moves ←→ flips of triangulations

←→

To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 127: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gonsquare moves ←→ flips of triangulations

←→

Plabic graphs (Postnikov) give positivity tests for (Grk,n)>0, just astriangulations give positivity tests for (Gr2,n)>0.To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 128: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gonsquare moves ←→ flips of triangulations

←→

Plabic graphs (Postnikov) give positivity tests for (Grk,n)>0, just astriangulations give positivity tests for (Gr2,n)>0.Recall that the associahedron encodes positivity tests for (Gr2,n)>0. Whatis the analogue for (Grk,n)>0? To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 129: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

Second generalization: triangulation plabic graph

(2, n)-planar bicolored graphs ←→ triangulations of a convex n-gonsquare moves ←→ flips of triangulations

←→

Plabic graphs (Postnikov) give positivity tests for (Grk,n)>0, just astriangulations give positivity tests for (Gr2,n)>0.Recall that the associahedron encodes positivity tests for (Gr2,n)>0. Whatis the analogue for (Grk,n)>0? To be continued in afternoon lecture.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 21 / 23

Page 130: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

BREAK

Lauren K. Williams (Harvard) Cluster Algebras October 2019 22 / 23

Page 131: Cluster Algebras - Harvard CMSAPoisson geometry triangulations of surface and Teichmu¨ller theory mathematical physics: wall-crossing phenomena, quiver gauge theories, scattering

References

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

2 3

4

56

1

P13P24

= P12P34

+ P14P23

P15P

46= P14P

56+ P16P

45

ReferencesFomin and Zelevinsky, Cluster algebras I: Foundations, Journal of the AMS 15 (2002),497–529.

Fomin and Zelevinsky, Y-systems and generalized associahedra, Annals of Mathematics158 (2003), 977–1018.

Fomin and Zelevinsky, Cluster algebras II: Finite type classification, InventionesMathematicae 154 (2003), 63–121.

Williams, Cluster algebras: an introduction, Bulletin of the AMS 51 (2014), 1–26.

Fomin, Williams, and Zelevinsky, Introduction to Cluster Algebras, book in progress,arXiv:1608.05735, arXiv:1707.07190.

Lauren K. Williams (Harvard) Cluster Algebras October 2019 23 / 23


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