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Two Perspectives on Mutations Two Perspectives on Cluster Mutations Dylan Rupel Northeastern University April 20, 2013 Maurice Auslander Distinguished Lectures and International Conference 2013 Woods Hole, MA Dylan Rupel (NEU) Two


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SLIDE 1

Two Perspectives on Mutations

Two Perspectives on Cluster Mutations

Dylan Rupel

Northeastern University

April 20, 2013 Maurice Auslander Distinguished Lectures and International Conference 2013 Woods Hole, MA

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 1 / 21

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SLIDE 2

Two Perspectives on Mutations Quantum Cluster Algebras Initial Data

To get started defining the quantum cluster algebra we need the combinatorial data of a compatible pair (˜ B, Λ). ˜ B - m × n (m ≥ n) exchange matrix B - skew-symmetrizable principal n × n submatrix D - diagonal skew-symmetrizing matrix, i.e. DB is skew-symmetric Λ - m × m commutation matrix

Compatibility Condition:

˜ BtΛ =

  • D
  • Dylan Rupel (NEU)

Two Perspectives on Mutations April 20, 2013 2 / 21

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SLIDE 3

Two Perspectives on Mutations Quantum Cluster Algebras Initial Data

To get started defining the quantum cluster algebra we need the combinatorial data of a compatible pair (˜ B, Λ). ˜ B - m × n (m ≥ n) exchange matrix B - skew-symmetrizable principal n × n submatrix D - diagonal skew-symmetrizing matrix, i.e. DB is skew-symmetric Λ - m × m commutation matrix

Compatibility Condition:

˜ BtΛ =

  • D
  • Dylan Rupel (NEU)

Two Perspectives on Mutations April 20, 2013 2 / 21

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SLIDE 4

Two Perspectives on Mutations Quantum Cluster Algebras Initial Data

To get started defining the quantum cluster algebra we need the combinatorial data of a compatible pair (˜ B, Λ). ˜ B - m × n (m ≥ n) exchange matrix B - skew-symmetrizable principal n × n submatrix D - diagonal skew-symmetrizing matrix, i.e. DB is skew-symmetric Λ - m × m commutation matrix

Compatibility Condition:

˜ BtΛ =

  • D
  • Dylan Rupel (NEU)

Two Perspectives on Mutations April 20, 2013 2 / 21

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SLIDE 5

Two Perspectives on Mutations Quantum Cluster Algebras Initial Data

To get started defining the quantum cluster algebra we need the combinatorial data of a compatible pair (˜ B, Λ). ˜ B - m × n (m ≥ n) exchange matrix B - skew-symmetrizable principal n × n submatrix D - diagonal skew-symmetrizing matrix, i.e. DB is skew-symmetric Λ - m × m commutation matrix

Compatibility Condition:

˜ BtΛ =

  • D
  • Dylan Rupel (NEU)

Two Perspectives on Mutations April 20, 2013 2 / 21

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SLIDE 6

Two Perspectives on Mutations Quantum Cluster Algebras Initial Data

To get started defining the quantum cluster algebra we need the combinatorial data of a compatible pair (˜ B, Λ). ˜ B - m × n (m ≥ n) exchange matrix B - skew-symmetrizable principal n × n submatrix D - diagonal skew-symmetrizing matrix, i.e. DB is skew-symmetric Λ - m × m commutation matrix

Compatibility Condition:

˜ BtΛ =

  • D
  • Dylan Rupel (NEU)

Two Perspectives on Mutations April 20, 2013 2 / 21

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SLIDE 7

Two Perspectives on Mutations Quantum Cluster Algebras Initial Data

To get started defining the quantum cluster algebra we need the combinatorial data of a compatible pair (˜ B, Λ). ˜ B - m × n (m ≥ n) exchange matrix B - skew-symmetrizable principal n × n submatrix D - diagonal skew-symmetrizing matrix, i.e. DB is skew-symmetric Λ - m × m commutation matrix

Compatibility Condition:

˜ BtΛ =

  • D
  • Dylan Rupel (NEU)

Two Perspectives on Mutations April 20, 2013 2 / 21

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SLIDE 8

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Torus

For a parameter q, the commutation matrix Λ determines the quasi-commutation of an m-dimensional quantum torus TΛ,q which will contain the quantum cluster algebra Aq(˜ B, Λ).

Quantum Torus:

TΛ,q = Z[q± 1

2 ]X ±1

1 , . . . , X ±1 m

: XiXj = qλijXjXi The quantum torus has a unique anti-involution (reverses the order of products) called the bar-involution which fixes the generators (Xi = Xi) and sends q to q−1.

Bar Invariant Monomials (X a = X a):

Let α1, . . . , αm be the standard basis vectors of Zm. For a =

m

  • i=1

aiαi ∈ Zm we define bar-invariant monomials X a = q

− 1

2

  • i<j

aiajλij

X a1

1 · · · X am m .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 3 / 21

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SLIDE 9

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Torus

For a parameter q, the commutation matrix Λ determines the quasi-commutation of an m-dimensional quantum torus TΛ,q which will contain the quantum cluster algebra Aq(˜ B, Λ).

Quantum Torus:

TΛ,q = Z[q± 1

2 ]X ±1

1 , . . . , X ±1 m

: XiXj = qλijXjXi The quantum torus has a unique anti-involution (reverses the order of products) called the bar-involution which fixes the generators (Xi = Xi) and sends q to q−1.

Bar Invariant Monomials (X a = X a):

Let α1, . . . , αm be the standard basis vectors of Zm. For a =

m

  • i=1

aiαi ∈ Zm we define bar-invariant monomials X a = q

− 1

2

  • i<j

aiajλij

X a1

1 · · · X am m .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 3 / 21

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SLIDE 10

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Torus

For a parameter q, the commutation matrix Λ determines the quasi-commutation of an m-dimensional quantum torus TΛ,q which will contain the quantum cluster algebra Aq(˜ B, Λ).

Quantum Torus:

TΛ,q = Z[q± 1

2 ]X ±1

1 , . . . , X ±1 m

: XiXj = qλijXjXi The quantum torus has a unique anti-involution (reverses the order of products) called the bar-involution which fixes the generators (Xi = Xi) and sends q to q−1.

Bar Invariant Monomials (X a = X a):

Let α1, . . . , αm be the standard basis vectors of Zm. For a =

m

  • i=1

aiαi ∈ Zm we define bar-invariant monomials X a = q

− 1

2

  • i<j

aiajλij

X a1

1 · · · X am m .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 3 / 21

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SLIDE 11

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Torus

For a parameter q, the commutation matrix Λ determines the quasi-commutation of an m-dimensional quantum torus TΛ,q which will contain the quantum cluster algebra Aq(˜ B, Λ).

Quantum Torus:

TΛ,q = Z[q± 1

2 ]X ±1

1 , . . . , X ±1 m

: XiXj = qλijXjXi The quantum torus has a unique anti-involution (reverses the order of products) called the bar-involution which fixes the generators (Xi = Xi) and sends q to q−1.

Bar Invariant Monomials (X a = X a):

Let α1, . . . , αm be the standard basis vectors of Zm. For a =

m

  • i=1

aiαi ∈ Zm we define bar-invariant monomials X a = q

− 1

2

  • i<j

aiajλij

X a1

1 · · · X am m .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 3 / 21

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SLIDE 12

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seeds and the Mutation Tree

Write X = {X1, . . . , Xm} for the set of generators of the quantum torus TΛ,q and call the collection X the initial cluster.

Initial Quantum Seed:

Σ0 = (X, ˜ B, Λ) Let Tn denote the rooted n-regular tree with root vertex t0. We will label the n edges of Tn emanating from each vertex by the set {1, . . . , n}. We will actually have many quantum seeds Σt, one for each vertex t of Tn, subject to the following conditions: The initial quantum seed is associated to the root: Σt0 = Σ0. If there exists an edge of Tn labeled by k between vertices t and t′, then the quantum seeds Σt and Σt′ are related by the mutation in direction k.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 4 / 21

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Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seeds and the Mutation Tree

Write X = {X1, . . . , Xm} for the set of generators of the quantum torus TΛ,q and call the collection X the initial cluster.

Initial Quantum Seed:

Σ0 = (X, ˜ B, Λ) Let Tn denote the rooted n-regular tree with root vertex t0. We will label the n edges of Tn emanating from each vertex by the set {1, . . . , n}. We will actually have many quantum seeds Σt, one for each vertex t of Tn, subject to the following conditions: The initial quantum seed is associated to the root: Σt0 = Σ0. If there exists an edge of Tn labeled by k between vertices t and t′, then the quantum seeds Σt and Σt′ are related by the mutation in direction k.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 4 / 21

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SLIDE 14

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seeds and the Mutation Tree

Write X = {X1, . . . , Xm} for the set of generators of the quantum torus TΛ,q and call the collection X the initial cluster.

Initial Quantum Seed:

Σ0 = (X, ˜ B, Λ) Let Tn denote the rooted n-regular tree with root vertex t0. We will label the n edges of Tn emanating from each vertex by the set {1, . . . , n}. We will actually have many quantum seeds Σt, one for each vertex t of Tn, subject to the following conditions: The initial quantum seed is associated to the root: Σt0 = Σ0. If there exists an edge of Tn labeled by k between vertices t and t′, then the quantum seeds Σt and Σt′ are related by the mutation in direction k.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 4 / 21

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SLIDE 15

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seeds and the Mutation Tree

Write X = {X1, . . . , Xm} for the set of generators of the quantum torus TΛ,q and call the collection X the initial cluster.

Initial Quantum Seed:

Σ0 = (X, ˜ B, Λ) Let Tn denote the rooted n-regular tree with root vertex t0. We will label the n edges of Tn emanating from each vertex by the set {1, . . . , n}. We will actually have many quantum seeds Σt, one for each vertex t of Tn, subject to the following conditions: The initial quantum seed is associated to the root: Σt0 = Σ0. If there exists an edge of Tn labeled by k between vertices t and t′, then the quantum seeds Σt and Σt′ are related by the mutation in direction k.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 4 / 21

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SLIDE 16

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seeds and the Mutation Tree

Write X = {X1, . . . , Xm} for the set of generators of the quantum torus TΛ,q and call the collection X the initial cluster.

Initial Quantum Seed:

Σ0 = (X, ˜ B, Λ) Let Tn denote the rooted n-regular tree with root vertex t0. We will label the n edges of Tn emanating from each vertex by the set {1, . . . , n}. We will actually have many quantum seeds Σt, one for each vertex t of Tn, subject to the following conditions: The initial quantum seed is associated to the root: Σt0 = Σ0. If there exists an edge of Tn labeled by k between vertices t and t′, then the quantum seeds Σt and Σt′ are related by the mutation in direction k.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 4 / 21

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SLIDE 17

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seeds and the Mutation Tree

Write X = {X1, . . . , Xm} for the set of generators of the quantum torus TΛ,q and call the collection X the initial cluster.

Initial Quantum Seed:

Σ0 = (X, ˜ B, Λ) Let Tn denote the rooted n-regular tree with root vertex t0. We will label the n edges of Tn emanating from each vertex by the set {1, . . . , n}. We will actually have many quantum seeds Σt, one for each vertex t of Tn, subject to the following conditions: The initial quantum seed is associated to the root: Σt0 = Σ0. If there exists an edge of Tn labeled by k between vertices t and t′, then the quantum seeds Σt and Σt′ are related by the mutation in direction k.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 4 / 21

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Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seed Mutations

To define the mutation of quantum seeds we need a little more notation. Write bk for the kth column of ˜ B thought of as an element of Zm. Let bk

+ = bik>0

bikαi and bk

− = bk + − bk.

Internal Mutations:

For 1 ≤ k ≤ n, define the mutation µkΣ = (µkX, µk ˜ B, µkΛ) of a seed in direction k as follows: µkX = X \ {Xk} ∪ {X ′

k} where X ′ k = X bk

+−αk + X bk −−αk,

µk ˜ B = Ek ˜ BFk (Fomin-Zelevinsky), µkΛ = EkΛE t

k (Berenstein-Zelevinsky).

Note: cluster variables obtained through iterated mutations will, a priori, be elements of the skew-field of fractions F of TΛ,q.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 5 / 21

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SLIDE 19

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seed Mutations

To define the mutation of quantum seeds we need a little more notation. Write bk for the kth column of ˜ B thought of as an element of Zm. Let bk

+ = bik>0

bikαi and bk

− = bk + − bk.

Internal Mutations:

For 1 ≤ k ≤ n, define the mutation µkΣ = (µkX, µk ˜ B, µkΛ) of a seed in direction k as follows: µkX = X \ {Xk} ∪ {X ′

k} where X ′ k = X bk

+−αk + X bk −−αk,

µk ˜ B = Ek ˜ BFk (Fomin-Zelevinsky), µkΛ = EkΛE t

k (Berenstein-Zelevinsky).

Note: cluster variables obtained through iterated mutations will, a priori, be elements of the skew-field of fractions F of TΛ,q.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 5 / 21

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SLIDE 20

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seed Mutations

To define the mutation of quantum seeds we need a little more notation. Write bk for the kth column of ˜ B thought of as an element of Zm. Let bk

+ = bik>0

bikαi and bk

− = bk + − bk.

Internal Mutations:

For 1 ≤ k ≤ n, define the mutation µkΣ = (µkX, µk ˜ B, µkΛ) of a seed in direction k as follows: µkX = X \ {Xk} ∪ {X ′

k} where X ′ k = X bk

+−αk + X bk −−αk,

µk ˜ B = Ek ˜ BFk (Fomin-Zelevinsky), µkΛ = EkΛE t

k (Berenstein-Zelevinsky).

Note: cluster variables obtained through iterated mutations will, a priori, be elements of the skew-field of fractions F of TΛ,q.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 5 / 21

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SLIDE 21

Two Perspectives on Mutations Quantum Cluster Algebras Quantum Seed Mutations

To define the mutation of quantum seeds we need a little more notation. Write bk for the kth column of ˜ B thought of as an element of Zm. Let bk

+ = bik>0

bikαi and bk

− = bk + − bk.

Internal Mutations:

For 1 ≤ k ≤ n, define the mutation µkΣ = (µkX, µk ˜ B, µkΛ) of a seed in direction k as follows: µkX = X \ {Xk} ∪ {X ′

k} where X ′ k = X bk

+−αk + X bk −−αk,

µk ˜ B = Ek ˜ BFk (Fomin-Zelevinsky), µkΛ = EkΛE t

k (Berenstein-Zelevinsky).

Note: cluster variables obtained through iterated mutations will, a priori, be elements of the skew-field of fractions F of TΛ,q.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 5 / 21

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SLIDE 22

Two Perspectives on Mutations Quantum Cluster Algebras Definition

We are finally ready to define the quantum cluster algebra.

Quantum Cluster Algebra:

Define the quantum cluster algebra Aq(˜ B, Λ) to be the Z[q± 1

2 ]-subalgebra

  • f F generated by all cluster variables from all seeds Σt where t runs over

the vertices of the mutation tree Tn.

Theorem (Quantum Laurent Phenomenon: Berenstein, Zelevinsky)

For any seed Σt = (Xt, ˜ Bt, Λt), the quantum cluster algebra Aq(˜ B, Λ) is a subalgebra of the quantum torus TΛt,q.

Laurent Problem:

Understand the initial cluster Laurent expansion of each cluster variable. Our Goal: Solve this problem when the principal submatrix B is acyclic.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 6 / 21

slide-23
SLIDE 23

Two Perspectives on Mutations Quantum Cluster Algebras Definition

We are finally ready to define the quantum cluster algebra.

Quantum Cluster Algebra:

Define the quantum cluster algebra Aq(˜ B, Λ) to be the Z[q± 1

2 ]-subalgebra

  • f F generated by all cluster variables from all seeds Σt where t runs over

the vertices of the mutation tree Tn.

Theorem (Quantum Laurent Phenomenon: Berenstein, Zelevinsky)

For any seed Σt = (Xt, ˜ Bt, Λt), the quantum cluster algebra Aq(˜ B, Λ) is a subalgebra of the quantum torus TΛt,q.

Laurent Problem:

Understand the initial cluster Laurent expansion of each cluster variable. Our Goal: Solve this problem when the principal submatrix B is acyclic.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 6 / 21

slide-24
SLIDE 24

Two Perspectives on Mutations Quantum Cluster Algebras Definition

We are finally ready to define the quantum cluster algebra.

Quantum Cluster Algebra:

Define the quantum cluster algebra Aq(˜ B, Λ) to be the Z[q± 1

2 ]-subalgebra

  • f F generated by all cluster variables from all seeds Σt where t runs over

the vertices of the mutation tree Tn.

Theorem (Quantum Laurent Phenomenon: Berenstein, Zelevinsky)

For any seed Σt = (Xt, ˜ Bt, Λt), the quantum cluster algebra Aq(˜ B, Λ) is a subalgebra of the quantum torus TΛt,q.

Laurent Problem:

Understand the initial cluster Laurent expansion of each cluster variable. Our Goal: Solve this problem when the principal submatrix B is acyclic.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 6 / 21

slide-25
SLIDE 25

Two Perspectives on Mutations Quantum Cluster Algebras Definition

We are finally ready to define the quantum cluster algebra.

Quantum Cluster Algebra:

Define the quantum cluster algebra Aq(˜ B, Λ) to be the Z[q± 1

2 ]-subalgebra

  • f F generated by all cluster variables from all seeds Σt where t runs over

the vertices of the mutation tree Tn.

Theorem (Quantum Laurent Phenomenon: Berenstein, Zelevinsky)

For any seed Σt = (Xt, ˜ Bt, Λt), the quantum cluster algebra Aq(˜ B, Λ) is a subalgebra of the quantum torus TΛt,q.

Laurent Problem:

Understand the initial cluster Laurent expansion of each cluster variable. Our Goal: Solve this problem when the principal submatrix B is acyclic.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 6 / 21

slide-26
SLIDE 26

Two Perspectives on Mutations Quantum Cluster Algebras Definition

We are finally ready to define the quantum cluster algebra.

Quantum Cluster Algebra:

Define the quantum cluster algebra Aq(˜ B, Λ) to be the Z[q± 1

2 ]-subalgebra

  • f F generated by all cluster variables from all seeds Σt where t runs over

the vertices of the mutation tree Tn.

Theorem (Quantum Laurent Phenomenon: Berenstein, Zelevinsky)

For any seed Σt = (Xt, ˜ Bt, Λt), the quantum cluster algebra Aq(˜ B, Λ) is a subalgebra of the quantum torus TΛt,q.

Laurent Problem:

Understand the initial cluster Laurent expansion of each cluster variable. Our Goal: Solve this problem when the principal submatrix B is acyclic.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 6 / 21

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SLIDE 27

Two Perspectives on Mutations Quantum Cluster Algebras Two Views of Mutation

The internal mutation µk in the definition of the quantum cluster algebra should be viewed as a recursive process inside the fixed skew-field F. There is another way to look at mutations, we view the mutation as a change of the initial cluster. We will call this type of mutation an external mutation. To be more precise suppose t and t′ are connected by an edge in Tn labeled by k. By the quantum Laurent phenomenon the quantum cluster algebra Aq(˜ B, Λ) is contained in both TΛt,q ⊂ Ft and TΛt′,q ⊂ Ft′. Write X a

t and X a t′ for the bar-invariant monomials in TΛt,q and TΛt′,q

respectively.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 7 / 21

slide-28
SLIDE 28

Two Perspectives on Mutations Quantum Cluster Algebras Two Views of Mutation

The internal mutation µk in the definition of the quantum cluster algebra should be viewed as a recursive process inside the fixed skew-field F. There is another way to look at mutations, we view the mutation as a change of the initial cluster. We will call this type of mutation an external mutation. To be more precise suppose t and t′ are connected by an edge in Tn labeled by k. By the quantum Laurent phenomenon the quantum cluster algebra Aq(˜ B, Λ) is contained in both TΛt,q ⊂ Ft and TΛt′,q ⊂ Ft′. Write X a

t and X a t′ for the bar-invariant monomials in TΛt,q and TΛt′,q

respectively.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 7 / 21

slide-29
SLIDE 29

Two Perspectives on Mutations Quantum Cluster Algebras Two Views of Mutation

The internal mutation µk in the definition of the quantum cluster algebra should be viewed as a recursive process inside the fixed skew-field F. There is another way to look at mutations, we view the mutation as a change of the initial cluster. We will call this type of mutation an external mutation. To be more precise suppose t and t′ are connected by an edge in Tn labeled by k. By the quantum Laurent phenomenon the quantum cluster algebra Aq(˜ B, Λ) is contained in both TΛt,q ⊂ Ft and TΛt′,q ⊂ Ft′. Write X a

t and X a t′ for the bar-invariant monomials in TΛt,q and TΛt′,q

respectively.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 7 / 21

slide-30
SLIDE 30

Two Perspectives on Mutations Quantum Cluster Algebras Two Views of Mutation

The internal mutation µk in the definition of the quantum cluster algebra should be viewed as a recursive process inside the fixed skew-field F. There is another way to look at mutations, we view the mutation as a change of the initial cluster. We will call this type of mutation an external mutation. To be more precise suppose t and t′ are connected by an edge in Tn labeled by k. By the quantum Laurent phenomenon the quantum cluster algebra Aq(˜ B, Λ) is contained in both TΛt,q ⊂ Ft and TΛt′,q ⊂ Ft′. Write X a

t and X a t′ for the bar-invariant monomials in TΛt,q and TΛt′,q

respectively.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 7 / 21

slide-31
SLIDE 31

Two Perspectives on Mutations Quantum Cluster Algebras Two Views of Mutation

The external mutation ˜ µk takes the form of a bi-rational isomorphism of skew-fields with ˜ µk(Aq(˜ B, Λ)) = Aq(˜ B, Λ):

External Mutations:

˜ µk : Ft Ft′ : ˜ µk Xk X

bk

t′ +−αk

t′

+ X

bk

t′ −−αk

t′

X

bk

t +−αk

t

+ X

bk

t −−αk

t

X ′

k .

With regards to the Laurent problem these two mutations have close connections to the representation theory of valued quivers (species).

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 8 / 21

slide-32
SLIDE 32

Two Perspectives on Mutations Quantum Cluster Algebras Two Views of Mutation

The external mutation ˜ µk takes the form of a bi-rational isomorphism of skew-fields with ˜ µk(Aq(˜ B, Λ)) = Aq(˜ B, Λ):

External Mutations:

˜ µk : Ft Ft′ : ˜ µk Xk X

bk

t′ +−αk

t′

+ X

bk

t′ −−αk

t′

X

bk

t +−αk

t

+ X

bk

t −−αk

t

X ′

k .

With regards to the Laurent problem these two mutations have close connections to the representation theory of valued quivers (species).

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 8 / 21

slide-33
SLIDE 33

Two Perspectives on Mutations Quantum Cluster Algebras Two Views of Mutation

The external mutation ˜ µk takes the form of a bi-rational isomorphism of skew-fields with ˜ µk(Aq(˜ B, Λ)) = Aq(˜ B, Λ):

External Mutations:

˜ µk : Ft Ft′ : ˜ µk Xk X

bk

t′ +−αk

t′

+ X

bk

t′ −−αk

t′

X

bk

t +−αk

t

+ X

bk

t −−αk

t

X ′

k .

With regards to the Laurent problem these two mutations have close connections to the representation theory of valued quivers (species).

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 8 / 21

slide-34
SLIDE 34

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quivers

Our solution to the Laurent problem will involve combinatorial objects called valued quivers.

Valued Quivers:

Q = (Q0, Q1, s, t) - acyclic quiver with vertices Q0 = {1, . . . , n}, arrows Q1, and source and target maps s, t : Q1 → Q0. d : Q0 → Z>0 - valuations on the vertices, d(i) = di. Call the pair (Q, d) an acyclic valued quiver. From a skew-symmetrizable n × n matrix B we can construct a valued quiver (Q, d) as follows: Q has vertices {1, . . . , n} with valuations di = ith diagonal entry of the symmetrizing matrix D, whenever bij > 0, Q has gcd(bij, −bji) arrows i → j.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 9 / 21

slide-35
SLIDE 35

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quivers

Our solution to the Laurent problem will involve combinatorial objects called valued quivers.

Valued Quivers:

Q = (Q0, Q1, s, t) - acyclic quiver with vertices Q0 = {1, . . . , n}, arrows Q1, and source and target maps s, t : Q1 → Q0. d : Q0 → Z>0 - valuations on the vertices, d(i) = di. Call the pair (Q, d) an acyclic valued quiver. From a skew-symmetrizable n × n matrix B we can construct a valued quiver (Q, d) as follows: Q has vertices {1, . . . , n} with valuations di = ith diagonal entry of the symmetrizing matrix D, whenever bij > 0, Q has gcd(bij, −bji) arrows i → j.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 9 / 21

slide-36
SLIDE 36

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quivers

Our solution to the Laurent problem will involve combinatorial objects called valued quivers.

Valued Quivers:

Q = (Q0, Q1, s, t) - acyclic quiver with vertices Q0 = {1, . . . , n}, arrows Q1, and source and target maps s, t : Q1 → Q0. d : Q0 → Z>0 - valuations on the vertices, d(i) = di. Call the pair (Q, d) an acyclic valued quiver. From a skew-symmetrizable n × n matrix B we can construct a valued quiver (Q, d) as follows: Q has vertices {1, . . . , n} with valuations di = ith diagonal entry of the symmetrizing matrix D, whenever bij > 0, Q has gcd(bij, −bji) arrows i → j.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 9 / 21

slide-37
SLIDE 37

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quivers

Our solution to the Laurent problem will involve combinatorial objects called valued quivers.

Valued Quivers:

Q = (Q0, Q1, s, t) - acyclic quiver with vertices Q0 = {1, . . . , n}, arrows Q1, and source and target maps s, t : Q1 → Q0. d : Q0 → Z>0 - valuations on the vertices, d(i) = di. Call the pair (Q, d) an acyclic valued quiver. From a skew-symmetrizable n × n matrix B we can construct a valued quiver (Q, d) as follows: Q has vertices {1, . . . , n} with valuations di = ith diagonal entry of the symmetrizing matrix D, whenever bij > 0, Q has gcd(bij, −bji) arrows i → j.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 9 / 21

slide-38
SLIDE 38

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quivers

Our solution to the Laurent problem will involve combinatorial objects called valued quivers.

Valued Quivers:

Q = (Q0, Q1, s, t) - acyclic quiver with vertices Q0 = {1, . . . , n}, arrows Q1, and source and target maps s, t : Q1 → Q0. d : Q0 → Z>0 - valuations on the vertices, d(i) = di. Call the pair (Q, d) an acyclic valued quiver. From a skew-symmetrizable n × n matrix B we can construct a valued quiver (Q, d) as follows: Q has vertices {1, . . . , n} with valuations di = ith diagonal entry of the symmetrizing matrix D, whenever bij > 0, Q has gcd(bij, −bji) arrows i → j.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 9 / 21

slide-39
SLIDE 39

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quivers

Our solution to the Laurent problem will involve combinatorial objects called valued quivers.

Valued Quivers:

Q = (Q0, Q1, s, t) - acyclic quiver with vertices Q0 = {1, . . . , n}, arrows Q1, and source and target maps s, t : Q1 → Q0. d : Q0 → Z>0 - valuations on the vertices, d(i) = di. Call the pair (Q, d) an acyclic valued quiver. From a skew-symmetrizable n × n matrix B we can construct a valued quiver (Q, d) as follows: Q has vertices {1, . . . , n} with valuations di = ith diagonal entry of the symmetrizing matrix D, whenever bij > 0, Q has gcd(bij, −bji) arrows i → j.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 9 / 21

slide-40
SLIDE 40

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quivers

Our solution to the Laurent problem will involve combinatorial objects called valued quivers.

Valued Quivers:

Q = (Q0, Q1, s, t) - acyclic quiver with vertices Q0 = {1, . . . , n}, arrows Q1, and source and target maps s, t : Q1 → Q0. d : Q0 → Z>0 - valuations on the vertices, d(i) = di. Call the pair (Q, d) an acyclic valued quiver. From a skew-symmetrizable n × n matrix B we can construct a valued quiver (Q, d) as follows: Q has vertices {1, . . . , n} with valuations di = ith diagonal entry of the symmetrizing matrix D, whenever bij > 0, Q has gcd(bij, −bji) arrows i → j.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 9 / 21

slide-41
SLIDE 41

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quiver Representations

To define representations of a valued quiver we need to introduce some more notation. F - finite field with q elements ¯ F - an algebraic closure of F Fk - degree k extension of F in ¯ F Note: Fk ∩ Fℓ = Fgcd(k,ℓ)

Valued Quiver Representations:

A representation V = ({Vi}i∈Q0, {ϕa}a∈Q1) of (Q, d) consists of an Fdi-vector space Vi for each vertex i and an Fgcd(ds(a),dt(a))-linear map ϕa : Vs(a) → Vt(a) for each arrow a. repF(Q, d) - hereditary, Abelian category of finite dimensional representations of (Q, d) (equivalent to modules over a species)

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 10 / 21

slide-42
SLIDE 42

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quiver Representations

To define representations of a valued quiver we need to introduce some more notation. F - finite field with q elements ¯ F - an algebraic closure of F Fk - degree k extension of F in ¯ F Note: Fk ∩ Fℓ = Fgcd(k,ℓ)

Valued Quiver Representations:

A representation V = ({Vi}i∈Q0, {ϕa}a∈Q1) of (Q, d) consists of an Fdi-vector space Vi for each vertex i and an Fgcd(ds(a),dt(a))-linear map ϕa : Vs(a) → Vt(a) for each arrow a. repF(Q, d) - hereditary, Abelian category of finite dimensional representations of (Q, d) (equivalent to modules over a species)

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 10 / 21

slide-43
SLIDE 43

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quiver Representations

To define representations of a valued quiver we need to introduce some more notation. F - finite field with q elements ¯ F - an algebraic closure of F Fk - degree k extension of F in ¯ F Note: Fk ∩ Fℓ = Fgcd(k,ℓ)

Valued Quiver Representations:

A representation V = ({Vi}i∈Q0, {ϕa}a∈Q1) of (Q, d) consists of an Fdi-vector space Vi for each vertex i and an Fgcd(ds(a),dt(a))-linear map ϕa : Vs(a) → Vt(a) for each arrow a. repF(Q, d) - hereditary, Abelian category of finite dimensional representations of (Q, d) (equivalent to modules over a species)

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 10 / 21

slide-44
SLIDE 44

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quiver Representations

To define representations of a valued quiver we need to introduce some more notation. F - finite field with q elements ¯ F - an algebraic closure of F Fk - degree k extension of F in ¯ F Note: Fk ∩ Fℓ = Fgcd(k,ℓ)

Valued Quiver Representations:

A representation V = ({Vi}i∈Q0, {ϕa}a∈Q1) of (Q, d) consists of an Fdi-vector space Vi for each vertex i and an Fgcd(ds(a),dt(a))-linear map ϕa : Vs(a) → Vt(a) for each arrow a. repF(Q, d) - hereditary, Abelian category of finite dimensional representations of (Q, d) (equivalent to modules over a species)

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 10 / 21

slide-45
SLIDE 45

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quiver Representations

To define representations of a valued quiver we need to introduce some more notation. F - finite field with q elements ¯ F - an algebraic closure of F Fk - degree k extension of F in ¯ F Note: Fk ∩ Fℓ = Fgcd(k,ℓ)

Valued Quiver Representations:

A representation V = ({Vi}i∈Q0, {ϕa}a∈Q1) of (Q, d) consists of an Fdi-vector space Vi for each vertex i and an Fgcd(ds(a),dt(a))-linear map ϕa : Vs(a) → Vt(a) for each arrow a. repF(Q, d) - hereditary, Abelian category of finite dimensional representations of (Q, d) (equivalent to modules over a species)

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 10 / 21

slide-46
SLIDE 46

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quiver Representations

To define representations of a valued quiver we need to introduce some more notation. F - finite field with q elements ¯ F - an algebraic closure of F Fk - degree k extension of F in ¯ F Note: Fk ∩ Fℓ = Fgcd(k,ℓ)

Valued Quiver Representations:

A representation V = ({Vi}i∈Q0, {ϕa}a∈Q1) of (Q, d) consists of an Fdi-vector space Vi for each vertex i and an Fgcd(ds(a),dt(a))-linear map ϕa : Vs(a) → Vt(a) for each arrow a. repF(Q, d) - hereditary, Abelian category of finite dimensional representations of (Q, d) (equivalent to modules over a species)

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 10 / 21

slide-47
SLIDE 47

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Valued Quiver Representations

To define representations of a valued quiver we need to introduce some more notation. F - finite field with q elements ¯ F - an algebraic closure of F Fk - degree k extension of F in ¯ F Note: Fk ∩ Fℓ = Fgcd(k,ℓ)

Valued Quiver Representations:

A representation V = ({Vi}i∈Q0, {ϕa}a∈Q1) of (Q, d) consists of an Fdi-vector space Vi for each vertex i and an Fgcd(ds(a),dt(a))-linear map ϕa : Vs(a) → Vt(a) for each arrow a. repF(Q, d) - hereditary, Abelian category of finite dimensional representations of (Q, d) (equivalent to modules over a species)

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 10 / 21

slide-48
SLIDE 48

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Character Setup

To introduce the quantum cluster character we need more notation: K(Q, d) - Grothendieck group of repF(Q, d) αi - isomorphism class of the vertex-simple Si Q acyclic = ⇒ K(Q, d) =

i∈Q0 Zαi

Euler-Ringel Form:

Suppose V , W ∈ repF(Q, d). We will need the Euler-Ringel form given by V , W = dimFHom(V , W ) − dimFExt1(V , W ). Note: the Euler-Ringel form only depends on the classes of V and W in K(Q, d). Abbreviate α∨

i := 1 di αi. For e ∈ K(Q, d) define vectors ∗e, e∗ ∈ Zn by ∗e = n i=1α∨ i , eαi, e∗ = n i=1e, α∨ i αi.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 11 / 21

slide-49
SLIDE 49

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Character Setup

To introduce the quantum cluster character we need more notation: K(Q, d) - Grothendieck group of repF(Q, d) αi - isomorphism class of the vertex-simple Si Q acyclic = ⇒ K(Q, d) =

i∈Q0 Zαi

Euler-Ringel Form:

Suppose V , W ∈ repF(Q, d). We will need the Euler-Ringel form given by V , W = dimFHom(V , W ) − dimFExt1(V , W ). Note: the Euler-Ringel form only depends on the classes of V and W in K(Q, d). Abbreviate α∨

i := 1 di αi. For e ∈ K(Q, d) define vectors ∗e, e∗ ∈ Zn by ∗e = n i=1α∨ i , eαi, e∗ = n i=1e, α∨ i αi.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 11 / 21

slide-50
SLIDE 50

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Character Setup

To introduce the quantum cluster character we need more notation: K(Q, d) - Grothendieck group of repF(Q, d) αi - isomorphism class of the vertex-simple Si Q acyclic = ⇒ K(Q, d) =

i∈Q0 Zαi

Euler-Ringel Form:

Suppose V , W ∈ repF(Q, d). We will need the Euler-Ringel form given by V , W = dimFHom(V , W ) − dimFExt1(V , W ). Note: the Euler-Ringel form only depends on the classes of V and W in K(Q, d). Abbreviate α∨

i := 1 di αi. For e ∈ K(Q, d) define vectors ∗e, e∗ ∈ Zn by ∗e = n i=1α∨ i , eαi, e∗ = n i=1e, α∨ i αi.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 11 / 21

slide-51
SLIDE 51

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Character Setup

To introduce the quantum cluster character we need more notation: K(Q, d) - Grothendieck group of repF(Q, d) αi - isomorphism class of the vertex-simple Si Q acyclic = ⇒ K(Q, d) =

i∈Q0 Zαi

Euler-Ringel Form:

Suppose V , W ∈ repF(Q, d). We will need the Euler-Ringel form given by V , W = dimFHom(V , W ) − dimFExt1(V , W ). Note: the Euler-Ringel form only depends on the classes of V and W in K(Q, d). Abbreviate α∨

i := 1 di αi. For e ∈ K(Q, d) define vectors ∗e, e∗ ∈ Zn by ∗e = n i=1α∨ i , eαi, e∗ = n i=1e, α∨ i αi.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 11 / 21

slide-52
SLIDE 52

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Character Setup

To introduce the quantum cluster character we need more notation: K(Q, d) - Grothendieck group of repF(Q, d) αi - isomorphism class of the vertex-simple Si Q acyclic = ⇒ K(Q, d) =

i∈Q0 Zαi

Euler-Ringel Form:

Suppose V , W ∈ repF(Q, d). We will need the Euler-Ringel form given by V , W = dimFHom(V , W ) − dimFExt1(V , W ). Note: the Euler-Ringel form only depends on the classes of V and W in K(Q, d). Abbreviate α∨

i := 1 di αi. For e ∈ K(Q, d) define vectors ∗e, e∗ ∈ Zn by ∗e = n i=1α∨ i , eαi, e∗ = n i=1e, α∨ i αi.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 11 / 21

slide-53
SLIDE 53

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Character Setup

To introduce the quantum cluster character we need more notation: K(Q, d) - Grothendieck group of repF(Q, d) αi - isomorphism class of the vertex-simple Si Q acyclic = ⇒ K(Q, d) =

i∈Q0 Zαi

Euler-Ringel Form:

Suppose V , W ∈ repF(Q, d). We will need the Euler-Ringel form given by V , W = dimFHom(V , W ) − dimFExt1(V , W ). Note: the Euler-Ringel form only depends on the classes of V and W in K(Q, d). Abbreviate α∨

i := 1 di αi. For e ∈ K(Q, d) define vectors ∗e, e∗ ∈ Zn by ∗e = n i=1α∨ i , eαi, e∗ = n i=1e, α∨ i αi.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 11 / 21

slide-54
SLIDE 54

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Character Setup

To introduce the quantum cluster character we need more notation: K(Q, d) - Grothendieck group of repF(Q, d) αi - isomorphism class of the vertex-simple Si Q acyclic = ⇒ K(Q, d) =

i∈Q0 Zαi

Euler-Ringel Form:

Suppose V , W ∈ repF(Q, d). We will need the Euler-Ringel form given by V , W = dimFHom(V , W ) − dimFExt1(V , W ). Note: the Euler-Ringel form only depends on the classes of V and W in K(Q, d). Abbreviate α∨

i := 1 di αi. For e ∈ K(Q, d) define vectors ∗e, e∗ ∈ Zn by ∗e = n i=1α∨ i , eαi, e∗ = n i=1e, α∨ i αi.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 11 / 21

slide-55
SLIDE 55

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Characters

Let V ∈ repF(Q, d) and write v ∈ K(Q, d) for the dimension vector of V .

Quantum Cluster Character:

We define the quantum cluster character V → XV ∈ TΛ,q by XV =

  • e∈K(Q,d)

q− 1

2 e,v−e|Gre(V )|X −e∗−∗(v−e)

where Gre(V ) denotes the Grassmannian of subrepresentations of V with isomorphism class e.

Theorem (R.)

The quantum cluster character V → XV defines a bijection from indecomposable rigid representations V of (Q, d) to non-initial quantum cluster variables of the quantum cluster algebra Aq(˜ B, Λ) ⊂ TΛ,q.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 12 / 21

slide-56
SLIDE 56

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Characters

Let V ∈ repF(Q, d) and write v ∈ K(Q, d) for the dimension vector of V .

Quantum Cluster Character:

We define the quantum cluster character V → XV ∈ TΛ,q by XV =

  • e∈K(Q,d)

q− 1

2 e,v−e|Gre(V )|X −e∗−∗(v−e)

where Gre(V ) denotes the Grassmannian of subrepresentations of V with isomorphism class e.

Theorem (R.)

The quantum cluster character V → XV defines a bijection from indecomposable rigid representations V of (Q, d) to non-initial quantum cluster variables of the quantum cluster algebra Aq(˜ B, Λ) ⊂ TΛ,q.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 12 / 21

slide-57
SLIDE 57

Two Perspectives on Mutations Solution to Laurent Problem (acyclic case) Quantum Cluster Characters

Let V ∈ repF(Q, d) and write v ∈ K(Q, d) for the dimension vector of V .

Quantum Cluster Character:

We define the quantum cluster character V → XV ∈ TΛ,q by XV =

  • e∈K(Q,d)

q− 1

2 e,v−e|Gre(V )|X −e∗−∗(v−e)

where Gre(V ) denotes the Grassmannian of subrepresentations of V with isomorphism class e.

Theorem (R.)

The quantum cluster character V → XV defines a bijection from indecomposable rigid representations V of (Q, d) to non-initial quantum cluster variables of the quantum cluster algebra Aq(˜ B, Λ) ⊂ TΛ,q.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 12 / 21

slide-58
SLIDE 58

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

repF(Q, d)k - full subcategory of repF(Q, d) of objects without indecomposable summands isomorphic to the simple Sk µkQ - quiver obtained from Q by reversing all arrows incident on vertex k Σ±

k : repF(Q, d)k → repF(µkQ, d)k - Dlab-Ringel reflection

functors at a sink or source vertex k (we usually drop the ± from the notation)

  • riginally defined in terms of modules over an associated F-species

Theorem (R.)

For V ∈ repF(Q, d)k the external mutation at a sink or source vertex k can be computed via the reflection functor Σk by ˜ µk(XV ) = XΣkV .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 13 / 21

slide-59
SLIDE 59

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

repF(Q, d)k - full subcategory of repF(Q, d) of objects without indecomposable summands isomorphic to the simple Sk µkQ - quiver obtained from Q by reversing all arrows incident on vertex k Σ±

k : repF(Q, d)k → repF(µkQ, d)k - Dlab-Ringel reflection

functors at a sink or source vertex k (we usually drop the ± from the notation)

  • riginally defined in terms of modules over an associated F-species

Theorem (R.)

For V ∈ repF(Q, d)k the external mutation at a sink or source vertex k can be computed via the reflection functor Σk by ˜ µk(XV ) = XΣkV .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 13 / 21

slide-60
SLIDE 60

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

repF(Q, d)k - full subcategory of repF(Q, d) of objects without indecomposable summands isomorphic to the simple Sk µkQ - quiver obtained from Q by reversing all arrows incident on vertex k Σ±

k : repF(Q, d)k → repF(µkQ, d)k - Dlab-Ringel reflection

functors at a sink or source vertex k (we usually drop the ± from the notation)

  • riginally defined in terms of modules over an associated F-species

Theorem (R.)

For V ∈ repF(Q, d)k the external mutation at a sink or source vertex k can be computed via the reflection functor Σk by ˜ µk(XV ) = XΣkV .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 13 / 21

slide-61
SLIDE 61

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

repF(Q, d)k - full subcategory of repF(Q, d) of objects without indecomposable summands isomorphic to the simple Sk µkQ - quiver obtained from Q by reversing all arrows incident on vertex k Σ±

k : repF(Q, d)k → repF(µkQ, d)k - Dlab-Ringel reflection

functors at a sink or source vertex k (we usually drop the ± from the notation)

  • riginally defined in terms of modules over an associated F-species

Theorem (R.)

For V ∈ repF(Q, d)k the external mutation at a sink or source vertex k can be computed via the reflection functor Σk by ˜ µk(XV ) = XΣkV .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 13 / 21

slide-62
SLIDE 62

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

repF(Q, d)k - full subcategory of repF(Q, d) of objects without indecomposable summands isomorphic to the simple Sk µkQ - quiver obtained from Q by reversing all arrows incident on vertex k Σ±

k : repF(Q, d)k → repF(µkQ, d)k - Dlab-Ringel reflection

functors at a sink or source vertex k (we usually drop the ± from the notation)

  • riginally defined in terms of modules over an associated F-species

Theorem (R.)

For V ∈ repF(Q, d)k the external mutation at a sink or source vertex k can be computed via the reflection functor Σk by ˜ µk(XV ) = XΣkV .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 13 / 21

slide-63
SLIDE 63

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

repF(Q, d)k - full subcategory of repF(Q, d) of objects without indecomposable summands isomorphic to the simple Sk µkQ - quiver obtained from Q by reversing all arrows incident on vertex k Σ±

k : repF(Q, d)k → repF(µkQ, d)k - Dlab-Ringel reflection

functors at a sink or source vertex k (we usually drop the ± from the notation)

  • riginally defined in terms of modules over an associated F-species

Theorem (R.)

For V ∈ repF(Q, d)k the external mutation at a sink or source vertex k can be computed via the reflection functor Σk by ˜ µk(XV ) = XΣkV .

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 13 / 21

slide-64
SLIDE 64

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

Lemma

For any vertex k, the cluster variable obtained from the initial cluster by mutating in direction k is given by the quantum cluster character XSk. A cluster (X′, ˜ B′, Λ′) is called almost acyclic if there exists a vertex k so that (µkX′, µk ˜ B′, µkΛ′) is acyclic.

Corollary

Any cluster variable of Aq(˜ B, Λ) in an almost acyclic cluster is given by XV for some representation V which can be obtained via reflection functors from a simple representation. Open Question: What about non-sink/non-source mutations? ...Ask Daniel Labardini-Fragoso...there appear to be obstructions...

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 14 / 21

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SLIDE 65

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

Lemma

For any vertex k, the cluster variable obtained from the initial cluster by mutating in direction k is given by the quantum cluster character XSk. A cluster (X′, ˜ B′, Λ′) is called almost acyclic if there exists a vertex k so that (µkX′, µk ˜ B′, µkΛ′) is acyclic.

Corollary

Any cluster variable of Aq(˜ B, Λ) in an almost acyclic cluster is given by XV for some representation V which can be obtained via reflection functors from a simple representation. Open Question: What about non-sink/non-source mutations? ...Ask Daniel Labardini-Fragoso...there appear to be obstructions...

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 14 / 21

slide-66
SLIDE 66

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

Lemma

For any vertex k, the cluster variable obtained from the initial cluster by mutating in direction k is given by the quantum cluster character XSk. A cluster (X′, ˜ B′, Λ′) is called almost acyclic if there exists a vertex k so that (µkX′, µk ˜ B′, µkΛ′) is acyclic.

Corollary

Any cluster variable of Aq(˜ B, Λ) in an almost acyclic cluster is given by XV for some representation V which can be obtained via reflection functors from a simple representation. Open Question: What about non-sink/non-source mutations? ...Ask Daniel Labardini-Fragoso...there appear to be obstructions...

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 14 / 21

slide-67
SLIDE 67

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

Lemma

For any vertex k, the cluster variable obtained from the initial cluster by mutating in direction k is given by the quantum cluster character XSk. A cluster (X′, ˜ B′, Λ′) is called almost acyclic if there exists a vertex k so that (µkX′, µk ˜ B′, µkΛ′) is acyclic.

Corollary

Any cluster variable of Aq(˜ B, Λ) in an almost acyclic cluster is given by XV for some representation V which can be obtained via reflection functors from a simple representation. Open Question: What about non-sink/non-source mutations? ...Ask Daniel Labardini-Fragoso...there appear to be obstructions...

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 14 / 21

slide-68
SLIDE 68

Two Perspectives on Mutations External Mutations Reflection Functors and Quantum Cluster Characters

Lemma

For any vertex k, the cluster variable obtained from the initial cluster by mutating in direction k is given by the quantum cluster character XSk. A cluster (X′, ˜ B′, Λ′) is called almost acyclic if there exists a vertex k so that (µkX′, µk ˜ B′, µkΛ′) is acyclic.

Corollary

Any cluster variable of Aq(˜ B, Λ) in an almost acyclic cluster is given by XV for some representation V which can be obtained via reflection functors from a simple representation. Open Question: What about non-sink/non-source mutations? ...Ask Daniel Labardini-Fragoso...there appear to be obstructions...

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 14 / 21

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SLIDE 69

Two Perspectives on Mutations Internal Mutations Local Tilting Representations

Let V ∈ repF(Q, d). V is rigid if Ext1(V , V ) = 0. V is basic if each indecomposable summand appears with multiplicity

  • ne.

The support of V is the set supp(V ) = {i ∈ Q0 : Vi = 0}. V is sincere if supp(V ) = Q0.

Local Tilting Representations:

We will call a representation T ∈ repF(Q, d) local tilting if T is basic, rigid, and the number of indecomposable summands is equal to the number of vertices in its support. Important: the zero representation is local tilting.

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SLIDE 70

Two Perspectives on Mutations Internal Mutations Local Tilting Representations

Let V ∈ repF(Q, d). V is rigid if Ext1(V , V ) = 0. V is basic if each indecomposable summand appears with multiplicity

  • ne.

The support of V is the set supp(V ) = {i ∈ Q0 : Vi = 0}. V is sincere if supp(V ) = Q0.

Local Tilting Representations:

We will call a representation T ∈ repF(Q, d) local tilting if T is basic, rigid, and the number of indecomposable summands is equal to the number of vertices in its support. Important: the zero representation is local tilting.

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SLIDE 71

Two Perspectives on Mutations Internal Mutations Local Tilting Representations

Let V ∈ repF(Q, d). V is rigid if Ext1(V , V ) = 0. V is basic if each indecomposable summand appears with multiplicity

  • ne.

The support of V is the set supp(V ) = {i ∈ Q0 : Vi = 0}. V is sincere if supp(V ) = Q0.

Local Tilting Representations:

We will call a representation T ∈ repF(Q, d) local tilting if T is basic, rigid, and the number of indecomposable summands is equal to the number of vertices in its support. Important: the zero representation is local tilting.

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SLIDE 72

Two Perspectives on Mutations Internal Mutations Local Tilting Representations

Let V ∈ repF(Q, d). V is rigid if Ext1(V , V ) = 0. V is basic if each indecomposable summand appears with multiplicity

  • ne.

The support of V is the set supp(V ) = {i ∈ Q0 : Vi = 0}. V is sincere if supp(V ) = Q0.

Local Tilting Representations:

We will call a representation T ∈ repF(Q, d) local tilting if T is basic, rigid, and the number of indecomposable summands is equal to the number of vertices in its support. Important: the zero representation is local tilting.

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SLIDE 73

Two Perspectives on Mutations Internal Mutations Local Tilting Representations

Let V ∈ repF(Q, d). V is rigid if Ext1(V , V ) = 0. V is basic if each indecomposable summand appears with multiplicity

  • ne.

The support of V is the set supp(V ) = {i ∈ Q0 : Vi = 0}. V is sincere if supp(V ) = Q0.

Local Tilting Representations:

We will call a representation T ∈ repF(Q, d) local tilting if T is basic, rigid, and the number of indecomposable summands is equal to the number of vertices in its support. Important: the zero representation is local tilting.

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SLIDE 74

Two Perspectives on Mutations Internal Mutations Local Tilting Representations

Let V ∈ repF(Q, d). V is rigid if Ext1(V , V ) = 0. V is basic if each indecomposable summand appears with multiplicity

  • ne.

The support of V is the set supp(V ) = {i ∈ Q0 : Vi = 0}. V is sincere if supp(V ) = Q0.

Local Tilting Representations:

We will call a representation T ∈ repF(Q, d) local tilting if T is basic, rigid, and the number of indecomposable summands is equal to the number of vertices in its support. Important: the zero representation is local tilting.

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SLIDE 75

Two Perspectives on Mutations Internal Mutations Local Tilting Representations

Let V ∈ repF(Q, d). V is rigid if Ext1(V , V ) = 0. V is basic if each indecomposable summand appears with multiplicity

  • ne.

The support of V is the set supp(V ) = {i ∈ Q0 : Vi = 0}. V is sincere if supp(V ) = Q0.

Local Tilting Representations:

We will call a representation T ∈ repF(Q, d) local tilting if T is basic, rigid, and the number of indecomposable summands is equal to the number of vertices in its support. Important: the zero representation is local tilting.

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SLIDE 76

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Main Idea (Hubery): local tilting representations are in bijection with seeds To make this precise we will need to recall two classical theorems on tilting in hereditary categories:

Theorem (Happel, Ringel)

Suppose T is basic and rigid. Then T is a tilting representation if and

  • nly if T has as many non-isomorphic indecomposable summands as the

number of simple representations. This allows us to restrict a local tilting representation T to the full subquiver of (Q, d) on the vertices supp(T) where it becomes a tilting representation.

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SLIDE 77

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Main Idea (Hubery): local tilting representations are in bijection with seeds To make this precise we will need to recall two classical theorems on tilting in hereditary categories:

Theorem (Happel, Ringel)

Suppose T is basic and rigid. Then T is a tilting representation if and

  • nly if T has as many non-isomorphic indecomposable summands as the

number of simple representations. This allows us to restrict a local tilting representation T to the full subquiver of (Q, d) on the vertices supp(T) where it becomes a tilting representation.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 16 / 21

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SLIDE 78

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Main Idea (Hubery): local tilting representations are in bijection with seeds To make this precise we will need to recall two classical theorems on tilting in hereditary categories:

Theorem (Happel, Ringel)

Suppose T is basic and rigid. Then T is a tilting representation if and

  • nly if T has as many non-isomorphic indecomposable summands as the

number of simple representations. This allows us to restrict a local tilting representation T to the full subquiver of (Q, d) on the vertices supp(T) where it becomes a tilting representation.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 16 / 21

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SLIDE 79

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Main Idea (Hubery): local tilting representations are in bijection with seeds To make this precise we will need to recall two classical theorems on tilting in hereditary categories:

Theorem (Happel, Ringel)

Suppose T is basic and rigid. Then T is a tilting representation if and

  • nly if T has as many non-isomorphic indecomposable summands as the

number of simple representations. This allows us to restrict a local tilting representation T to the full subquiver of (Q, d) on the vertices supp(T) where it becomes a tilting representation.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 16 / 21

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SLIDE 80

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

T ∈ repF(Q, d) is called almost complete tilting if it contains one less than the required number of indecomposable summands.

Theorem (Happel, Unger)

Let T be an almost complete tilting representation. If T is sincere, then there exist exactly two non-isomorphic complements to T, otherwise there is a unique complement. We can combine this with the previous theorem to get a mutation

  • peration for local tilting representations which will parallel the mutations

in a quantum cluster algebra.

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SLIDE 81

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

T ∈ repF(Q, d) is called almost complete tilting if it contains one less than the required number of indecomposable summands.

Theorem (Happel, Unger)

Let T be an almost complete tilting representation. If T is sincere, then there exist exactly two non-isomorphic complements to T, otherwise there is a unique complement. We can combine this with the previous theorem to get a mutation

  • peration for local tilting representations which will parallel the mutations

in a quantum cluster algebra.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 17 / 21

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SLIDE 82

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

T ∈ repF(Q, d) is called almost complete tilting if it contains one less than the required number of indecomposable summands.

Theorem (Happel, Unger)

Let T be an almost complete tilting representation. If T is sincere, then there exist exactly two non-isomorphic complements to T, otherwise there is a unique complement. We can combine this with the previous theorem to get a mutation

  • peration for local tilting representations which will parallel the mutations

in a quantum cluster algebra.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 17 / 21

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SLIDE 83

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Mutation of Local Tilting Representations:

Define the mutation µk(T) = T ′ in direction k as follows:

1 If vertex k /

∈ supp(T), then there exists a unique complement T ′

k so

that T ′ = T ′

k ⊕ T is a local tilting representation containing k in its

support.

2 If vertex k ∈ supp(T), then write T = T/Tk. 1

If T is a local tilting representation, i.e. k / ∈ supp(T), let T ′ = T.

2

Otherwise supp(T) = supp(T) and there exists a unique compliment T ′

k ∼

= Tk so that T ′ = T ′

k ⊕ T is a local tilting representation.

It follows from results of [BMRRT] that every local tilting representation can be obtained from the zero representation by a sequence of mutations.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 18 / 21

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SLIDE 84

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Mutation of Local Tilting Representations:

Define the mutation µk(T) = T ′ in direction k as follows:

1 If vertex k /

∈ supp(T), then there exists a unique complement T ′

k so

that T ′ = T ′

k ⊕ T is a local tilting representation containing k in its

support.

2 If vertex k ∈ supp(T), then write T = T/Tk. 1

If T is a local tilting representation, i.e. k / ∈ supp(T), let T ′ = T.

2

Otherwise supp(T) = supp(T) and there exists a unique compliment T ′

k ∼

= Tk so that T ′ = T ′

k ⊕ T is a local tilting representation.

It follows from results of [BMRRT] that every local tilting representation can be obtained from the zero representation by a sequence of mutations.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 18 / 21

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SLIDE 85

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Mutation of Local Tilting Representations:

Define the mutation µk(T) = T ′ in direction k as follows:

1 If vertex k /

∈ supp(T), then there exists a unique complement T ′

k so

that T ′ = T ′

k ⊕ T is a local tilting representation containing k in its

support.

2 If vertex k ∈ supp(T), then write T = T/Tk. 1

If T is a local tilting representation, i.e. k / ∈ supp(T), let T ′ = T.

2

Otherwise supp(T) = supp(T) and there exists a unique compliment T ′

k ∼

= Tk so that T ′ = T ′

k ⊕ T is a local tilting representation.

It follows from results of [BMRRT] that every local tilting representation can be obtained from the zero representation by a sequence of mutations.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 18 / 21

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SLIDE 86

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Mutation of Local Tilting Representations:

Define the mutation µk(T) = T ′ in direction k as follows:

1 If vertex k /

∈ supp(T), then there exists a unique complement T ′

k so

that T ′ = T ′

k ⊕ T is a local tilting representation containing k in its

support.

2 If vertex k ∈ supp(T), then write T = T/Tk. 1

If T is a local tilting representation, i.e. k / ∈ supp(T), let T ′ = T.

2

Otherwise supp(T) = supp(T) and there exists a unique compliment T ′

k ∼

= Tk so that T ′ = T ′

k ⊕ T is a local tilting representation.

It follows from results of [BMRRT] that every local tilting representation can be obtained from the zero representation by a sequence of mutations.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 18 / 21

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SLIDE 87

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Mutation of Local Tilting Representations:

Define the mutation µk(T) = T ′ in direction k as follows:

1 If vertex k /

∈ supp(T), then there exists a unique complement T ′

k so

that T ′ = T ′

k ⊕ T is a local tilting representation containing k in its

support.

2 If vertex k ∈ supp(T), then write T = T/Tk. 1

If T is a local tilting representation, i.e. k / ∈ supp(T), let T ′ = T.

2

Otherwise supp(T) = supp(T) and there exists a unique compliment T ′

k ∼

= Tk so that T ′ = T ′

k ⊕ T is a local tilting representation.

It follows from results of [BMRRT] that every local tilting representation can be obtained from the zero representation by a sequence of mutations.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 18 / 21

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SLIDE 88

Two Perspectives on Mutations Internal Mutations Mutations of Local Tilting Representations

Mutation of Local Tilting Representations:

Define the mutation µk(T) = T ′ in direction k as follows:

1 If vertex k /

∈ supp(T), then there exists a unique complement T ′

k so

that T ′ = T ′

k ⊕ T is a local tilting representation containing k in its

support.

2 If vertex k ∈ supp(T), then write T = T/Tk. 1

If T is a local tilting representation, i.e. k / ∈ supp(T), let T ′ = T.

2

Otherwise supp(T) = supp(T) and there exists a unique compliment T ′

k ∼

= Tk so that T ′ = T ′

k ⊕ T is a local tilting representation.

It follows from results of [BMRRT] that every local tilting representation can be obtained from the zero representation by a sequence of mutations.

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 18 / 21

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SLIDE 89

Two Perspectives on Mutations Internal Mutations Relationship to Quantum Cluster Algebras

We assign a quantum seed ΣT = (XT, ˜ BT, ΛT) to each local tilting representation T as follows: XT = (X ′

1, . . . , X ′ m) is given by

X ′

k =

  • Xk

if k / ∈ supp(T); XTk if k ∈ supp(T); The kth column of the exchange matrix ˜ BT is defined homologically in terms of T and T ∗

k (Hubery);

ΛT records the quasi-commutation of XT (explicitly given by formulas involving the Euler-Ringel form and Λ).

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 19 / 21

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SLIDE 90

Two Perspectives on Mutations Internal Mutations Relationship to Quantum Cluster Algebras

We assign a quantum seed ΣT = (XT, ˜ BT, ΛT) to each local tilting representation T as follows: XT = (X ′

1, . . . , X ′ m) is given by

X ′

k =

  • Xk

if k / ∈ supp(T); XTk if k ∈ supp(T); The kth column of the exchange matrix ˜ BT is defined homologically in terms of T and T ∗

k (Hubery);

ΛT records the quasi-commutation of XT (explicitly given by formulas involving the Euler-Ringel form and Λ).

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 19 / 21

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SLIDE 91

Two Perspectives on Mutations Internal Mutations Relationship to Quantum Cluster Algebras

We assign a quantum seed ΣT = (XT, ˜ BT, ΛT) to each local tilting representation T as follows: XT = (X ′

1, . . . , X ′ m) is given by

X ′

k =

  • Xk

if k / ∈ supp(T); XTk if k ∈ supp(T); The kth column of the exchange matrix ˜ BT is defined homologically in terms of T and T ∗

k (Hubery);

ΛT records the quasi-commutation of XT (explicitly given by formulas involving the Euler-Ringel form and Λ).

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 19 / 21

slide-92
SLIDE 92

Two Perspectives on Mutations Internal Mutations Relationship to Quantum Cluster Algebras

We assign a quantum seed ΣT = (XT, ˜ BT, ΛT) to each local tilting representation T as follows: XT = (X ′

1, . . . , X ′ m) is given by

X ′

k =

  • Xk

if k / ∈ supp(T); XTk if k ∈ supp(T); The kth column of the exchange matrix ˜ BT is defined homologically in terms of T and T ∗

k (Hubery);

ΛT records the quasi-commutation of XT (explicitly given by formulas involving the Euler-Ringel form and Λ).

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 19 / 21

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SLIDE 93

Two Perspectives on Mutations Internal Mutations Relationship to Quantum Cluster Algebras

Theorem (R.)

Suppose µk(T) = T ′. Then ΣT and ΣT ′ are related by Berenstein-Zelevinsky quantum seed mutation in direction k.

Lemma

The quantum seed associated to the zero representation is exactly the initial quantum seed (X, ˜ B, Λ).

Corollary (R.)

The quantum cluster character V → XV defines a bijection from indecomposable rigid representations of (Q, d) to non-initial quantum cluster variables of the quantum cluster algebra Aq(˜ B, Λ).

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 20 / 21

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SLIDE 94

Two Perspectives on Mutations Internal Mutations Relationship to Quantum Cluster Algebras

Theorem (R.)

Suppose µk(T) = T ′. Then ΣT and ΣT ′ are related by Berenstein-Zelevinsky quantum seed mutation in direction k.

Lemma

The quantum seed associated to the zero representation is exactly the initial quantum seed (X, ˜ B, Λ).

Corollary (R.)

The quantum cluster character V → XV defines a bijection from indecomposable rigid representations of (Q, d) to non-initial quantum cluster variables of the quantum cluster algebra Aq(˜ B, Λ).

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 20 / 21

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SLIDE 95

Two Perspectives on Mutations Internal Mutations Relationship to Quantum Cluster Algebras

Theorem (R.)

Suppose µk(T) = T ′. Then ΣT and ΣT ′ are related by Berenstein-Zelevinsky quantum seed mutation in direction k.

Lemma

The quantum seed associated to the zero representation is exactly the initial quantum seed (X, ˜ B, Λ).

Corollary (R.)

The quantum cluster character V → XV defines a bijection from indecomposable rigid representations of (Q, d) to non-initial quantum cluster variables of the quantum cluster algebra Aq(˜ B, Λ).

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SLIDE 96

Two Perspectives on Mutations End

Thank you!

Dylan Rupel (NEU) Two Perspectives on Mutations April 20, 2013 21 / 21