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Dominance phenomena: Mutation, scattering and cluster algebras Nathan Reading arXiv:1802.10107 NC State University Vingt ans d’alg` ebres amass´ ees CIRM, Luminy 21 mars 2018 Dominance phenomena Refinement Ring homomorphisms
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Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Feb 24, 2020

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Page 1: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Dominance phenomena:Mutation, scattering and cluster algebras

Nathan ReadingarXiv:1802.10107

NC State University

Vingt ans d’algebres amasseesCIRM, Luminy21 mars 2018

Dominance phenomena

Refinement

Ring homomorphisms

Page 2: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Section 1. Dominance phenomena

Page 3: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Dominance relations between exchange matrices

B = [bij ] dominates B ′ = [b′ij ] if, for all i , j ,

• bij and b′ij weakly agree in sign (i.e. bijb′ij ≥ 0) and

• |bij | ≥ |b′ij |.

Example. B =

[0 1−2 0

]B ′ =

[0 1−1 0

]

Question: What are the consequences of dominance for structuresthat take an exchange matrix as input?

I’ll address that question by presenting some “dominancephenomena.”

1. Dominance phenomena 1

.

Page 4: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Four phenomena

Suppose B and B ′ are exchange matrices and B dominates B ′.In many cases:

Phenomenon I

The identity map from RB to RB′is mutation-linear.

Phenomenon II

FB refines FB′ . (mutation fans)

Phenomenon III

ScatFan(B) refines ScatFan(B ′). (cluster scattering fans)

Phenomenon IV

There is an injective, g-vector-preserving ring homomorphism fromA•(B ′) to A•(B). (principal coefficients cluster algebras)

1. Dominance phenomena 2

.

Page 5: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Four phenomena

Suppose B and B ′ are exchange matrices and B dominates B ′.In many cases (not the same cases for all four phenomena):

Phenomenon I

The identity map from RB to RB′is mutation-linear.

Phenomenon II

FB refines FB′ . (mutation fans)

Phenomenon III

ScatFan(B) refines ScatFan(B ′). (cluster scattering fans)

Phenomenon IV

There is an injective, g-vector-preserving ring homomorphism fromA•(B ′) to A•(B). (principal coefficients cluster algebras)

1. Dominance phenomena 2

.

Page 6: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Why phenomena?

• There are counterexamples.

• I don’t know necessary and sufficient conditions for thephenomena.

• Yet there are theorems that give compelling and surprisingexamples.

Goal: Establish that something real and nontrivial is happening,with an eye towards two potential benefits:

• Researchers from the various areas will apply their tools tofind more examples, necessary and/or sufficient conditions forthe phenomena, and/or additional dominance phenomena.

• The phenomena will lead to insights in the various areaswhere matrix mutation, scattering diagrams, and clusteralgebras are fundamental.

1. Dominance phenomena 3

.

Page 7: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Phenomenon I

In many cases, the identity map from RB to RB′is mutation-linear.

One way to understand this:

exchange matrix

coefficient rows

B

− − −− − −− − −− − −− − −

specialization−−−−−−−−−−→CA IV, Section 12

B

− − −− − −− − −

A mutation-linear map RB to RB′induces a functor

(geometric cluster algebras for B, specialization)↓

(geometric cluster algebras for B ′, specialization)

1. Dominance phenomena 4

.

Page 8: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Phenomenon I

In many cases, the identity map from RB to RB′is mutation-linear.

One way to understand this:

exchange matrix

coefficient rows

B

− − −− − −− − −− − −− − −

specialization−−−−−−−−−−→

CA IV, Section 12

B

− − −− − −− − −

A mutation-linear map RB to RB′induces a functor

(geometric cluster algebras for B, specialization)↓

(geometric cluster algebras for B ′, specialization)

1. Dominance phenomena 4

.

Page 9: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Phenomenon I

In many cases, the identity map from RB to RB′is mutation-linear.

One way to understand this:

exchange matrix

coefficient rows

B

− − −− − −− − −− − −− − −

specialization−−−−−−−−−−→

CA IV, Section 12

B

− − −− − −− − −

A mutation-linear map RB to RB′induces a functor

(geometric cluster algebras for B, specialization)↓

(geometric cluster algebras for B ′, specialization)1. Dominance phenomena 4

.

Page 10: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Phenomenon I

In many cases, the identity map from RB to RB′is mutation-linear.

One way to understand this (and I won’t say more here):

exchange matrix

coefficient rows

B

− − −− − −− − −− − −− − −

specialization−−−−−−−−−−→

CA IV, Section 12

B

− − −− − −− − −

A mutation-linear map RB to RB′induces a functor

(geometric cluster algebras for B, specialization)↓

(geometric cluster algebras for B ′, specialization)1. Dominance phenomena 4

.

Page 11: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Phenomena II and III (refinement of fans)

In many cases,• the mutation fan FB refines the mutation fan FB′ .• the cluster scattering fan ScatFan(B) refines the cluster

scattering fan ScatFan(B ′).

Aside: Theorem (R., 2017). A consistent scattering diagram withminimal support cuts space into a fan.

In finite type, both FB and ScatFan(B) coincide with the g-vectorfanT , the normal fan to a generalized associahedron.

Example: cyclohedron and associahedron.

[0 1−2 0

] [0 1−1 0

]1. Dominance phenomena 5

.

Page 12: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

2-cyclohedron & 2-associahedron

[0 1−2 0

] [0 1−1 0

]

Aside: Can we understand this on the level of triangulations?

1. Dominance phenomena 6

.

Page 13: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

2-cyclohedron & 2-associahedron

[0 1−2 0

] [0 1−1 0

]Aside: Can we understand this on the level of triangulations?

1. Dominance phenomena 6

.

Page 14: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

3-cyclohedron & 3-associahedron: B =[

0 1 0−2 0 10 −1 0

]

B ′ =[

0 1 0−1 0 10 −1 0

]

FB (cyclohedron)

1. Dominance phenomena 7

.

Page 15: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

3-cyclohedron & 3-associahedron: B =[

0 1 0−2 0 10 −1 0

]B ′ =

[0 1 0−1 0 10 −1 0

]FB (cyclohedron)

FB′ (associahedron)

1. Dominance phenomena 7

.

Page 16: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

3-cyclohedron & 3-associahedron: B =[

0 1 0−2 0 10 −1 0

]B ′ =

[0 1 0−1 0 10 −1 0

]FB (cyclohedron)

FB′ (associahedron)

1. Dominance phenomena 7

.

Page 17: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

3-cyclohedron & 3-associahedron: B =[

0 1 0−2 0 10 −1 0

]B ′ =

[0 1 0−1 0 10 −1 0

]FB (cyclohedron)

FB′ (associahedron)

General cyclo/associahedra:S. Viel, thesis in progress(surface and orbifold models)

1. Dominance phenomena 7

.

Page 18: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Non-Example: B =[

0 1 −1−1 0 11 −1 0

]B ′ =

[0 1 0−1 0 10 −1 0

]

FB FB′

These are normal fans to two different 3-associahedra.

1. Dominance phenomena 8

.

Page 19: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Phenomenon IV

In many cases, there is an injective, g-vector-preserving ringhomomorphism from A•(B ′) to A•(B) (principal coefficientscluster algebras).

Remarks:

• Phenomenon is known∗ to occur for B acyclic of finite type.

• There is a nice description of the homomorphism (where itsends initial cluster variables and coefficients).

• In some cases, including acyclic finite type, the map sendscluster variables to cluster variables (or “ray theta functions”to ray theta functions).

• Sending cluster variables to cluster variables is suggested byPhenomena II and III (fan refinement).

• Coefficients—and specifically principal ones—are crucial.

1. Dominance phenomena 9

.

Page 20: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Section 2. Refinement

Page 21: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Mutation maps ηBk

Let B be [ Ba ] (i.e. B with an extra row a ∈ Rn ).

For k = kq, kq−1, . . . , k1, define ηBk (a) to be the last row of µk(B).

Example: B =[

0 1−1 0

][

0 1−1 0a1 a2

]µ1−→

[0 −11 0

−a1 ?

]

? =

{a2 if a1 ≤ 0a2 + a1 if a1 ≥ 0

ηB1−→

2. Refinement 10

.

Page 22: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

The mutation fan

Define an equivalence relation ≡B on Rn by setting

a1 ≡B a2 ⇐⇒ sgn(ηBk (a1)) = sgn(ηBk (a2)) ∀k.

sgn(a) is the vector of signs (−1, 0,+1) of the entries of a.

B-classes: equivalence classes of ≡B .B-cones: closures of B-classes.

Right intuition, but not strictly correct:B-cones are common domains of linearity of all mutation maps.

Mutation fan for B:The collection FB of all B-cones and all faces of B-cones.

Theorem (R., 2011). FB is a complete fan (possibly withinfinitely many cones).

Theorem (R., 2017). ScatFan(B) refines FB .

Conjecture. For rank ≥ 3, they coincide iff B mutation-finite.

2. Refinement 11

.

Page 23: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

The mutation fan

Define an equivalence relation ≡B on Rn by setting

a1 ≡B a2 ⇐⇒ sgn(ηBk (a1)) = sgn(ηBk (a2)) ∀k.

sgn(a) is the vector of signs (−1, 0,+1) of the entries of a.

B-classes: equivalence classes of ≡B .B-cones: closures of B-classes.

Right intuition, but not strictly correct:B-cones are common domains of linearity of all mutation maps.

Mutation fan for B:The collection FB of all B-cones and all faces of B-cones.

Theorem (R., 2011). FB is a complete fan (possibly withinfinitely many cones).

Theorem (R., 2017). ScatFan(B) refines FB .

Conjecture. For rank ≥ 3, they coincide iff B mutation-finite.

2. Refinement 11

.

Page 24: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

The mutation fan

Define an equivalence relation ≡B on Rn by setting

a1 ≡B a2 ⇐⇒ sgn(ηBk (a1)) = sgn(ηBk (a2)) ∀k.

sgn(a) is the vector of signs (−1, 0,+1) of the entries of a.

B-classes: equivalence classes of ≡B .B-cones: closures of B-classes.

Right intuition, but not strictly correct:B-cones are common domains of linearity of all mutation maps.

Mutation fan for B:The collection FB of all B-cones and all faces of B-cones.

Theorem (R., 2011). FB is a complete fan (possibly withinfinitely many cones).

Theorem (R., 2017). ScatFan(B) refines FB .

Conjecture. For rank ≥ 3, they coincide iff B mutation-finite.

2. Refinement 11

.

Page 25: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

The mutation fan

Define an equivalence relation ≡B on Rn by setting

a1 ≡B a2 ⇐⇒ sgn(ηBk (a1)) = sgn(ηBk (a2)) ∀k.

sgn(a) is the vector of signs (−1, 0,+1) of the entries of a.

B-classes: equivalence classes of ≡B .B-cones: closures of B-classes.

Right intuition, but not strictly correct:B-cones are common domains of linearity of all mutation maps.

Mutation fan for B:The collection FB of all B-cones and all faces of B-cones.

Theorem (R., 2011). FB is a complete fan (possibly withinfinitely many cones).

Theorem (R., 2017). ScatFan(B) refines FB .

Conjecture. For rank ≥ 3, they coincide iff B mutation-finite.2. Refinement 11

.

Page 26: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B = [ 0 1−1 0 ]

ηB1−→

↓ ηB2

Each of the 5 maximalcones shown in the top-left picture is a B-cone.

2. Refinement 12

.

Page 27: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B = [ 0 1−1 0 ]

ηB1−→

↓ ηB2

Each of the 5 maximalcones shown in the top-left picture is a B-cone.

2. Refinement 12

.

Page 28: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B = [ 0 1−1 0 ]

ηB1−→

↓ ηB2

Each of the 5 maximalcones shown in the top-left picture is a B-cone.

2. Refinement 12

.

Page 29: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B = [ 0 1−1 0 ]

ηB1−→

↓ ηB2

Each of the 5 maximalcones shown in the top-left picture is a B-cone.

2. Refinement 12

.

Page 30: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 2

2 −2 0

](Markov quiver)

Mutation fans arehard to constructin general, but insome cases, there arecombinatorial models.

We’ll discussPhenomenon II intwo models:Cambrian fans andsurfaces (orbifolds).

2. Refinement 13

.

Page 31: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 2

2 −2 0

](Markov quiver)

Mutation fans arehard to constructin general, but insome cases, there arecombinatorial models.

We’ll discussPhenomenon II intwo models:Cambrian fans andsurfaces (orbifolds).

2. Refinement 13

.

Page 32: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 2

2 −2 0

](Markov quiver)

Mutation fans arehard to constructin general, but insome cases, there arecombinatorial models.

We’ll discussPhenomenon II intwo models:Cambrian fans andsurfaces (orbifolds).

2. Refinement 13

.

Page 33: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Mutation fans in the surfaces model

21 1

3

3

[ 0 2 −2−2 0 22 −2 0

]Maximal cones in themutation fan are givenby triangulations andmore general configu-rations that includeclosed curves.

(Shear coordinates ofquasi-laminations)

2. Refinement 14

.

Page 34: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Resecting a triangulated surface on an edge

α → α

B B ′

Theorem. (R., 2013) Assuming the Null Tangle Property,B dominates B ′ and FB refines∗ FB′ .

Null Tangle Property: Known for some surfaces, probably truefor many more (or maybe all?).

∗ “rational parts” of these fans.

Orbifold model: Extends surfaces model to cover more generalnon-skew-symmetric cases.

Shira Viel, 2017: Constructs mutation fan for an orbifold.She defines orbifold resection, and proves Phenomenon II.(E.g. cyclohedron fan refines associahedron fan.)

2. Refinement 15

.

Page 35: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Resecting a triangulated surface on an edge

α → α

B B ′

Theorem. (R., 2013) Assuming the Null Tangle Property,B dominates B ′ and FB refines∗ FB′ .

Null Tangle Property: Known for some surfaces, probably truefor many more (or maybe all?).

∗ “rational parts” of these fans.

Orbifold model: Extends surfaces model to cover more generalnon-skew-symmetric cases.

Shira Viel, 2017: Constructs mutation fan for an orbifold.She defines orbifold resection, and proves Phenomenon II.(E.g. cyclohedron fan refines associahedron fan.)

2. Refinement 15

.

Page 36: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Resecting a triangulated surface on an edge

α → α

B B ′

Theorem. (R., 2013) Assuming the Null Tangle Property,B dominates B ′ and FB refines∗ FB′ .

Null Tangle Property: Known for some surfaces, probably truefor many more (or maybe all?).

∗ “rational parts” of these fans.

Orbifold model: Extends surfaces model to cover more generalnon-skew-symmetric cases.

Shira Viel, 2017: Constructs mutation fan for an orbifold.She defines orbifold resection, and proves Phenomenon II.(E.g. cyclohedron fan refines associahedron fan.)

2. Refinement 15

.

Page 37: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example

Resect arc 1 then arc 3.

Torus Annulus Hexagon

21 1

3

3 1

2

3

3

21

[ 0 2 −2−2 0 22 −2 0

] [ 0 1 −1−1 0 21 −2 0

] [ 0 1 −1−1 0 11 −1 0

]

2. Refinement 16

.

Page 38: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]

B ′ =[

0 1 −1−1 0 21 −2 0

]B ′′ =

[0 1 −1−1 0 11 −1 0

]

FB (torus)

2. Refinement 17

.

Page 39: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]

B ′′ =[

0 1 −1−1 0 11 −1 0

]

FB (torus)

FB′ (annulus)

2. Refinement 17

.

Page 40: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]

B ′′ =[

0 1 −1−1 0 11 −1 0

]

FB (torus)

FB′ (annulus)

2. Refinement 17

.

Page 41: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]

B ′′ =[

0 1 −1−1 0 11 −1 0

]

FB (torus)

FB′ (annulus)

2. Refinement 17

.

Page 42: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]

B ′′ =[

0 1 −1−1 0 11 −1 0

]

FB (torus)

FB′ (annulus)

2. Refinement 17

.

Page 43: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]

B ′′ =[

0 1 −1−1 0 11 −1 0

]

FB (torus)

FB′ (annulus)

2. Refinement 17

.

Page 44: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]

B ′′ =[

0 1 −1−1 0 11 −1 0

]

FB′ (annulus)

2. Refinement 17

.

Page 45: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]B ′′ =

[0 1 −1−1 0 11 −1 0

]

FB′ (annulus)

FB′′ (hexagon)

2. Refinement 17

.

Page 46: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]B ′′ =

[0 1 −1−1 0 11 −1 0

]

FB′ (annulus)

FB′′ (hexagon)

2. Refinement 17

.

Page 47: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]B ′′ =

[0 1 −1−1 0 11 −1 0

]

FB′ (annulus)

FB′′ (hexagon)

2. Refinement 17

.

Page 48: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]B ′′ =

[0 1 −1−1 0 11 −1 0

]

FB′ (annulus)

FB′′ (hexagon)

2. Refinement 17

.

Page 49: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]B ′′ =

[0 1 −1−1 0 11 −1 0

]

FB′ (annulus)

FB′′ (hexagon)

2. Refinement 17

.

Page 50: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: B =[

0 2 −2−2 0 22 −2 0

]B ′ =

[0 1 −1−1 0 21 −2 0

]B ′′ =

[0 1 −1−1 0 11 −1 0

]

FB′′ (hexagon)

2. Refinement 17

.

Page 51: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Finite acyclic type: Cambrian fans

Each B defines a Cartan matrix A.

E.g. B =[

0 1 0−2 0 10 −1 0

]→ A =

[ 2 −1 0−2 2 −10 −1 2

]Coxeter fan: Defined by the reflecting hyperplanes of the Coxetergroup W associated to A. Maximal cones ↔ elements of W .

Cambrian fan: A certain coarsening of the Coxeter fan.Two ways to look at this:

• Coarsen according to a certain lattice congruence on W .

• Coarsen according to the combinatorics of “sortableelements.”

For Sn, this is the normal fan to the usual associahedron.(In general, generalized associahedron.)

2. Refinement 18

.

Page 52: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Cambrian fans and mutation fans

For B acyclic of finite type, FB is a Cambrian fan. (Key technicalpoint: identify fundamental weights with standard basis vectors.)

Theorem (R., 2013). For B acyclic of finite type, FB refines FB′

if and only if B dominates B ′.

Dominance relations among exchange matrices imply dominancerelations among Cartan matrices. So the theorem is a statementthat refinement relations exist among Cambrian fans when wedecrease edge-labels (or erase edges) on Coxeter diagrams.

Example (carried out incorrectly):

2. Refinement 19

.

Page 53: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Cambrian fans and mutation fans

For B acyclic of finite type, FB is a Cambrian fan. (Key technicalpoint: identify fundamental weights with standard basis vectors.)

Theorem (R., 2013). For B acyclic of finite type, FB refines FB′

if and only if B dominates B ′.

Dominance relations among exchange matrices imply dominancerelations among Cartan matrices. So the theorem is a statementthat refinement relations exist among Cambrian fans when wedecrease edge-labels (or erase edges) on Coxeter diagrams.

Example (carried out incorrectly):

2. Refinement 19

.

Page 54: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Cambrian fans and mutation fans

For B acyclic of finite type, FB is a Cambrian fan. (Key technicalpoint: identify fundamental weights with standard basis vectors.)

Theorem (R., 2013). For B acyclic of finite type, FB refines FB′

if and only if B dominates B ′.

Dominance relations among exchange matrices imply dominancerelations among Cartan matrices. So the theorem is a statementthat refinement relations exist among Cambrian fans when wedecrease edge-labels (or erase edges) on Coxeter diagrams.

Example (carried out correctly):

2. Refinement 19

.

Page 55: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Lattice homomorphisms between Cambrian lattices

The Cambrian lattice CambB is:

• A partial order on maximal cones in the Cambrian fan FB .The fan and the order interact very closely.

• A lattice quotient—and a sublattice—of the weak order onthe finite Coxeter group associated to B.

To prove the refinement of fans:

• Show that there is a surjective lattice homomorphism fromCambB to CambB′ .

• Appeal to general results on lattice homomorphisms and fans.

Theorem (R., 2012). Such a surjective lattice homomorphismexists for all acyclic, finite-type B,B ′ with B dominating B ′.

2. Refinement 20

.

Page 56: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: A3 Tamari is a lattice quotient of B3 Tamari

2. Refinement 21

.

Page 57: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Lattice homomorphisms between weak orders

To find a surjective lattice homomorphism CambB → CambB′ :

Find a surjective lattice homomorphism between the correspondingweak orders.

Theorem (R., 2012). If (W , S) and (W ′, S) are finite Coxetersystems such that W dominates W ′, then the weak order on W ′ isa lattice quotient of the weak order on W .

Dominance here means that the diagram of W ′ is obtained fromthe diagram of W by reducing edge-labels and/or erasing edges.

This theorem is the origin of the study of the dominance relationon exchange matrices.

A research theme: Lattice theory of the weak order on finiteCoxeter groups “knows” a lot of combinatorics and representationtheory.

2. Refinement 22

.

Page 58: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Lattice homomorphisms between weak orders

To find a surjective lattice homomorphism CambB → CambB′ :

Find a surjective lattice homomorphism between the correspondingweak orders.

Theorem (R., 2012). If (W , S) and (W ′, S) are finite Coxetersystems such that W dominates W ′, then the weak order on W ′ isa lattice quotient of the weak order on W .

Dominance here means that the diagram of W ′ is obtained fromthe diagram of W by reducing edge-labels and/or erasing edges.

This theorem is the origin of the study of the dominance relationon exchange matrices.

A research theme: Lattice theory of the weak order on finiteCoxeter groups “knows” a lot of combinatorics and representationtheory.

2. Refinement 22

.

Page 59: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Example: A3 as a lattice quotient of B3

2. Refinement 23

.

Page 60: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Section 3. Ring homomorphisms

Page 61: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Ring homomorphisms of cluster algebras (finite type)

Rays of the mutation fan FB are in bijection with cluster variables.

If FB refines FB′ , there is an inclusion

{rays of FB′} ↪−→ {rays of FB}

3. Ring homomorphisms 24

.

Page 62: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Ring homomorphisms of cluster algebras (finite type)

Rays of the mutation fan FB are in bijection with cluster variables.

If FB refines FB′ , there is an inclusion

{rays of FB′} ↪−→ {rays of FB}

Let’s look at a picture...

3. Ring homomorphisms 24

.

Page 63: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Ring homomorphisms of cluster algebras (finite type)

3. Ring homomorphisms 24

.

Page 64: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Ring homomorphisms of cluster algebras (finite type)

3. Ring homomorphisms 24

.

Page 65: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Ring homomorphisms of cluster algebras (finite type)

3. Ring homomorphisms 24

.

Page 66: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Ring homomorphisms of cluster algebras (finite type)

Rays of the mutation fan FB are in bijection with cluster variables.

If FB refines FB′ , there is an inclusion

{rays of FB′} ↪−→ {rays of FB}

3. Ring homomorphisms 24

.

Page 67: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Ring homomorphisms of cluster algebras (finite type)

Rays of the mutation fan FB are in bijection with cluster variables.

If FB refines FB′ , there is an inclusion

{rays of FB′} ↪−→ {rays of FB}

Therefore there is a natural injective map on cluster variables.

Theorem∗ (Reading 2017, Viel, thesis in progress). This injectionextends to a g-vector-preserving injective homomorphism fromA•(B ′) to A•(B). The map sends initial cluster variables to initialcluster variables and on the tropical (coefficient) variables, it is

y ′k 7→ ykzk

where zk is the cluster monomial whose g-vector is the kth columnof B minus the kth column of B ′.

3. Ring homomorphisms 24

.

Page 68: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Ring homomorphisms of cluster algebras (finite type)

Rays of the mutation fan FB are in bijection with cluster variables.

If FB refines FB′ , there is an inclusion

{rays of FB′} ↪−→ {rays of FB}

Therefore there is a natural injective map on cluster variables.

Theorem∗ (Reading 2017, Viel, thesis in progress). This injectionextends to a g-vector-preserving injective homomorphism fromA•(B ′) to A•(B). The map sends initial cluster variables to initialcluster variables and on the tropical (coefficient) variables, it is

y ′k 7→ ykzk

where zk is the cluster monomial whose g-vector is the kth columnof B minus the kth column of B ′.

3. Ring homomorphisms 24

.

Page 69: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Remarks on ring homomorphisms (finite type)

• Structure-preserving maps (ring structure and g-vectors).

• Close algebraic relationships between cluster algebras withdifferent exchange matrices of the same rank were notpreviously known.

• The homomorphism sends y ′k to where it needs to go topreserve g-vectors.

• Proof idea: the map defined on the initial cluster variables isobviously a homomorphism to something, and is injective(check the Jacobian matrix). Check that it sends clustervariables to cluster variables.

• Equivalently, the map sends y ′k to yk times the F -polynomialof zk and we check that it sends F -polynomials of clustervariables to F -polynomials of cluster variables.

3. Ring homomorphisms 25

.

Page 70: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B → [ 0 00 0 ]

x1 1

x−12 1 + y2x−11 1 + y1x2 1

3. Ring homomorphisms 26

.

Page 71: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B → [ 0 00 0 ]

[0 −11 0

]x1 1 1

x1x−12 1 + y2

x−12 1 + y2 1 + y2 + y1y2x−11 1 + y1 1 + y1x2 1 1

3. Ring homomorphisms 26

.

Page 72: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B → [ 0 00 0 ]

[0 −11 0

]x1 1 1

x1x−12 1 + y2

x−12 1 + y2 1 + y2 + y1y2x−11 1 + y1 1 + y1x2 1 1

y1 7→ y1y2 7→ y2(1 + y1)

3. Ring homomorphisms 26

.

Page 73: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B → [ 0 00 0 ]

[0 −11 0

]x1 1 1

x1x−12 1 + y2

x−12 1 + y2 1 + y2 + y1y2x−11 1 + y1 1 + y1x2 1 1

3. Ring homomorphisms 26

.

Page 74: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B → [ 0 00 0 ]

[0 −11 0

] [0 −21 0

]x1 1 1 1

x21x−12 1 + y2

x1x−12 1 + y2 1 + y2 + y1y2

x−12 1 + y2 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2x−11 1 + y1 1 + y1 1 + y1x2 1 1 1

3. Ring homomorphisms 26

.

Page 75: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B → [ 0 00 0 ]

[0 −11 0

] [0 −21 0

]x1 1 1 1

x21x−12 1 + y2

x1x−12 1 + y2 1 + y2 + y1y2

x−12 1 + y2 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2x−11 1 + y1 1 + y1 1 + y1x2 1 1 1

y1 7→ y1y2 7→ y2(1 + y1)

3. Ring homomorphisms 26

.

Page 76: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B → [ 0 00 0 ]

[0 −11 0

] [0 −21 0

]x1 1 1 1

x21x−12 1 + y2

x1x−12 1 + y2 1 + y2 + y1y2

x−12 1 + y2 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2x−11 1 + y1 1 + y1 1 + y1x2 1 1 1

3. Ring homomorphisms 26

.

Page 77: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B → [ 0 00 0 ]

[0 −11 0

] [0 −21 0

] [0 −31 0

]x1 1 1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1 1 + y1 1 + y1x2 1 1 1 1

3. Ring homomorphisms 26

.

Page 78: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B →[0 −11 0

] [0 −21 0

] [0 −31 0

]x1 1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1 1 + y1x2 1 1 1

3. Ring homomorphisms 26

.

Page 79: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

3. Ring homomorphisms 26

.

Page 80: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

y1 7→ y1y2 7→ y2(1 + y1)

3. Ring homomorphisms 26

.

Page 81: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.

3. Ring homomorphisms 26

.

Page 82: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.

3. Ring homomorphisms 26

.

Page 83: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.

3. Ring homomorphisms 26

.

Page 84: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.

3. Ring homomorphisms 26

.

Page 85: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.

3. Ring homomorphisms 26

.

Page 86: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples↓ g B →

[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.

3. Ring homomorphisms 26

.

Page 87: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.

3. Ring homomorphisms 26

.

Page 88: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.3. Ring homomorphisms 26

.

Page 89: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples↓ g B →

[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.3. Ring homomorphisms 26

.

Page 90: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Rank-2 examples

↓ g B →[0 −21 0

] [0 −31 0

]x1 1 1

x31x−12 1 + y2

x21x−12 1 + y2 1 + y2 + y1y2

x31x−22 1 + 2y2 + y22 + 3y1 y2 + 3y1 y

22 + 3y21 y

22 + y31 y

22

x1x−12 1 + y2 + y1y2 1 + y2 + 2y1y2 + y21 y2

x−12 1 + y2 + 2y1y2 + y21 y2 1 + y2 + 3y1y2 + 3y21 y2 + y31 y2x−11 1 + y1 1 + y1x2 1 1

Summary of what I know in rank-2:There are g-vector preserving homomorphisms whenever

• B is of finite or affine type, or

• B ′ is of finite type.

In these cases, cluster variables are sent to cluster variables (or“ray theta functions”) unless B =

[0 ba 0

]and B ′ =

[0 dc 0

]with

cd = −3 and 1 6∈ {|a|, |b|}.

Homomorphisms may exist in additional cases.3. Ring homomorphisms 26

.

Page 91: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

The proof in the surfaces case (finite type)

Cluster variables ←→ (tagged) arcsCoefficient variables ←→ “elementary laminations”

Strategy: Consider

• A homomorphism ν sending initial cluster variables to initialcluster variables and sending coefficients to coefficients timescluster monomials (as before).

• A map χ sending each cluster variable to the cluster variablewith the same g-vector and treating coefficients like ν.

ν and χ agree on initial cluster variables and coefficients.

Thus, if we show that χ sends each exchange relation to a validrelation, we can conclude that χ is the restriction of ν (which inparticular maps to the cluster algebra).

3. Ring homomorphisms 27

.

Page 92: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

The proof in the surfaces case (continued)

χ sends each cluster variable to the cluster variable with the sameg-vector, sends coefficients to coefficients times cluster monomials.

Want: χ sends each exchange relation to a valid relation.

Example:

α

δ=

µLα +

ν

χ ↓ χ ↓ χ ↓

α

δ′ =µ

Lα +

ν

3. Ring homomorphisms 28

.

Page 93: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Aside: Dominance on Cartan matrices

A Cartan matrix A = [aij ] dominates a Cartan matrix A′ = [a′ij ]

|aij | ≥ |a′ij | for all i , j .

Theorem (R., 2018) If A dominates A′ then Φ(A′) ⊆ Φ(A).

α1

α2

α1

α2

α1

α2

α1

α2

[ 2 00 2 ]

[2 −1−1 2

] [2 −2−1 2

] [2 −3−1 2

]

. . . but only if you do it right.

• Same simple roots in both root systems

• Include imaginary roots

Proof: Kac-Moody Lie algebras (Serre relations)

4. Dominance on Cartan matrices 29

.

Page 94: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Aside: Dominance on Cartan matrices

A Cartan matrix A = [aij ] dominates a Cartan matrix A′ = [a′ij ]

|aij | ≥ |a′ij | for all i , j .

Theorem (R., 2018) If A dominates A′ then Φ(A′) ⊆ Φ(A).

α1

α2

α1

α2

α1

α2

α1

α2

[ 2 00 2 ]

[2 −1−1 2

] [2 −2−1 2

] [2 −3−1 2

]. . . but only if you do it right.

• Same simple roots in both root systems

• Include imaginary roots

Proof: Kac-Moody Lie algebras (Serre relations)

4. Dominance on Cartan matrices 29

.

Page 95: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Aside: Dominance on Cartan matrices

A Cartan matrix A = [aij ] dominates a Cartan matrix A′ = [a′ij ]

|aij | ≥ |a′ij | for all i , j .

Theorem (R., 2018) If A dominates A′ then Φ(A′) ⊆ Φ(A).

α1

α2

α1

α2

α1

α2

α1

α2

[ 2 00 2 ]

[2 −1−1 2

] [2 −2−1 2

] [2 −3−1 2

]. . . but only if you do it right.

• Same simple roots in both root systems

• Include imaginary roots

Proof: Kac-Moody Lie algebras (Serre relations)

4. Dominance on Cartan matrices 29

.

Page 96: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Aside: Dominance on Cartan matrices

A Cartan matrix A = [aij ] dominates a Cartan matrix A′ = [a′ij ]

|aij | ≥ |a′ij | for all i , j .

Theorem (R., 2018) If A dominates A′ then Φ(A′) ⊆ Φ(A).

α1

α2

α1

α2

α1

α2

α1

α2

[ 2 00 2 ]

[2 −1−1 2

] [2 −2−1 2

] [2 −3−1 2

]. . . but only if you do it right.

• Same simple roots in both root systems

• Include imaginary roots

Proof: Kac-Moody Lie algebras (Serre relations)

4. Dominance on Cartan matrices 29

.

Page 97: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Aside: Dominance on Cartan matrices

A Cartan matrix A = [aij ] dominates a Cartan matrix A′ = [a′ij ]

|aij | ≥ |a′ij | for all i , j .

Theorem (R., 2018) If A dominates A′ then Φ(A′) ⊆ Φ(A).

α1

α2

α1

α2

α1

α2

α1

α2

[ 2 00 2 ]

[2 −1−1 2

] [2 −2−1 2

] [2 −3−1 2

]. . . but only if you do it right.

• Same simple roots in both root systems

• Include imaginary roots

Proof: Kac-Moody Lie algebras (Serre relations)

4. Dominance on Cartan matrices 29

.

Page 98: Dominance phenomena: Mutation, scattering and cluster algebras · The mutation fan De ne an equivalence relation B on Rn by setting a 1 B a 2 sgn( B k (a 1)) = sgn( Bk(a 2)) 8k: sgn(a)

Dominance phenomena scorecard (B dominates B ′)

Phenomenon Cases where it is knownI & II • acyclic finite type (& affine soon with Stella?)(µ-linearity • resection of surfaces (Q versions)and mutation • erasing arrows to disconnect the quiverfan refinement) • fully characterized in rank 2 (occurs and fails)

III • acyclic finite type (& affine soon with Stella?)(scattering • finite type surfaces (& more soon with Muller?)fan refinement) • occurs always∗ in rank 2

IV • acyclic finite type(g-vector- • rank 2, B finite or affine typepreserving ring • rank 2, B ′ finite typehomomorphisms) • some non-acyclic surfaces of finite type

arXiv:1802.10107

Thanks for listening.

4. Dominance on Cartan matrices 30

.