A tale of dihedral groups, SL(2), and beyond
Or: N0-matrices, my love Daniel Tubbenhauer
t • 1 s
· · · ·
Joint work with Marco Mackaay, Volodymyr Mazorchuk and Vanessa Miemietz
July 2018
LetA(Γ) be the adjacency matrix of a finite, connected, loopless graphΓ. Let Ue+1(X) be the Chebyshev polynomial .
Classification problem (CP).Classify allΓsuch that Ue+1(A(Γ)) = 0.
fore= 2
fore= 4 ADE graphs fore+ 2 being(at most)the Coxeter number.
Type Am: • • • · · · • • • fore=m−1
Type Dm: • • · · · • •
•
•
for e= 2m−4
Type E6:
• • • • •
•
fore= 10
Type E7:
• • • • • •
•
fore= 16
Type E8:
• • • • • • •
•
fore= 28
LetA(Γ) be the adjacency matrix of a finite, connected, loopless graphΓ. Let Ue+1(X) be the Chebyshev polynomial .
Classification problem (CP).Classify allΓsuch that Ue+1(A(Γ)) = 0.
A3= 1 3 2
• • • A(A3) =
0 0 1
0 0 1
1 1 0
SA3={2 cos(π4),0,2 cos(3π4)}
U3(X) = (X−2 cos(π4))X(X−2 cos(3π4))
fore= 2
fore= 4 Smith∼1969. The graphs solutions to (CP) are precisely
ADE graphs fore+ 2 being(at most)the Coxeter number.
Type Am: • • • · · · • • • fore=m−1
Type Dm: • • · · · • •
•
•
for e= 2m−4
Type E6:
• • • • •
•
fore= 10
Type E7:
• • • • • •
•
fore= 16
Type E8:
• • • • • • •
•
fore= 28
LetA(Γ) be the adjacency matrix of a finite, connected, loopless graphΓ. Let Ue+1(X) be the Chebyshev polynomial .
Classification problem (CP).Classify allΓsuch that Ue+1(A(Γ)) = 0.
A3= 1 3 2
• • • A(A3) =
0 0 1
0 0 1
1 1 0
SA3={2 cos(π4),0,2 cos(3π4)}
D4= 1 4 2
3
• •
•
•
A(D4) =
0 0 0 1
0 0 0 1
0 0 0 1
1 1 1 0
SD4={2 cos(π6),02,2 cos(5π6)}
U3(X) = (X−2 cos(π4))X(X−2 cos(3π4))
U5(X) = (X−2 cos(π6))(X−2 cos(2π6))X(X−2 cos(4π6))(X−2 cos(5π6))
fore= 2
fore= 4 ADE graphs fore+ 2 being(at most)the Coxeter number.
Type Am: • • • · · · • • • fore=m−1
Type Dm: • • · · · • •
•
•
for e= 2m−4
Type E6:
• • • • •
•
fore= 10
Type E7:
• • • • • •
•
fore= 16
Type E8:
• • • • • • •
•
fore= 28
LetA(Γ) be the adjacency matrix of a finite, connected, loopless graphΓ. Let Ue+1(X) be the Chebyshev polynomial .
Classification problem (CP).Classify allΓsuch that Ue+1(A(Γ)) = 0.
A3= 1 3 2
• • • A(A3) =
0 0 1
0 0 1
1 1 0
SA3={2 cos(π4),0,2 cos(3π4)}
D4= 1 4 2
3
• •
•
•
A(D4) =
0 0 0 1
0 0 0 1
0 0 0 1
1 1 1 0
SD4={2 cos(π6),02,2 cos(5π6)}
U3(X) = (X−2 cos(π4))X(X−2 cos(3π4))
U5(X) = (X−2 cos(π6))(X−2 cos(2π6))X(X−2 cos(4π6))(X−2 cos(5π6)) fore= 2
fore= 4
Smith∼1969. The graphs solutions to (CP) are precisely ADE graphs fore+ 2 being(at most)the Coxeter number.
Type Am: • • • · · · • • • fore=m−1
Type Dm: • • · · · • •
•
•
for e= 2m−4
Type E6:
• • • • •
•
fore= 10
Type E7:
• • • • • •
•
fore= 16
Type E8:
• • • • • • •
•
fore= 28
LetA(Γ) be the adjacency matrix of a finite, connected, loopless graphΓ. Let Ue+1(X) be the Chebyshev polynomial .
Classification problem (CP).Classify allΓsuch that Ue+1(A(Γ)) = 0.
A3= 1 3 2
• • • A(A3) =
0 0 1
0 0 1
1 1 0
SA3={2 cos(π4),0,2 cos(3π4)}
D4= 1 4 2
3
• •
•
•
A(D4) =
0 0 0 1
0 0 0 1
0 0 0 1
1 1 1 0
SD4={2 cos(π6),02,2 cos(5π6)}
U3(X) = (X−2 cos(π4))X(X−2 cos(3π4))
U5(X) = (X−2 cos(π6))(X−2 cos(2π6))X(X−2 cos(4π6))(X−2 cos(5π6))
fore= 4
Smith∼1969. The graphs solutions to (CP) are precisely ADE graphs fore+ 2 being(at most)the Coxeter number.
Type Am: • • • · · · • • • fore=m−1
Type Dm: • • · · · • •
•
•
fore= 2m−4
Type E6:
• • • • •
•
for e= 10
Type E7:
• • • • • •
•
for e= 16
Type E8:
•
for e= 28
1 Dihedral representation theory
A brief primer onN0-representation theory DihedralN0-representation theory
2 Dihedral 2-representation theory A brief primer on 2-representation theory Dihedral 2-representation theory
3 Towards modular representation theory SL(2)
...and beyond
The main example today: dihedral groups
The dihedral groups are of Coxeter type I2(e+ 2):
We+2=hs,t|s2=t2= 1, se+2 =. . .sts
| {z }
e+2
=w0=. . .tst
| {z }
e+2
=te+2i, e.g.: W4=hs,t|s2=t2= 1, tsts=w0=ststi
Example. These are the symmetry groups of regulare+ 2-gons, e.g. fore= 2 the Coxeter complex is:
• H
H
H
H F F
F F
1
I should do the Hecke case, but I will keep it easy.
For the moment: Never mind! Highest cell.
s-cell. t-cell.
The main example today: dihedral groups
The dihedral groups are of Coxeter type I2(e+ 2):
We+2=hs,t|s2=t2= 1, se+2 =. . .sts
| {z }
e+2
=w0=. . .tst
| {z }
e+2
=te+2i, e.g.: W4=hs,t|s2=t2= 1, tsts=w0=ststi
Example. These are the symmetry groups of regulare+ 2-gons, e.g. fore= 2 the Coxeter complex is:
• H
H
H
H F F
F F
1 t s
I should do the Hecke case, but I will keep it easy.
I will explain in a few minutes what cells are. For the moment: Never mind!
Lowest cell. Highest cell.
s-cell. t-cell.
The main example today: dihedral groups
The dihedral groups are of Coxeter type I2(e+ 2):
We+2=hs,t|s2=t2= 1, se+2 =. . .sts
| {z }
e+2
=w0=. . .tst
| {z }
e+2
=te+2i, e.g.: W4=hs,t|s2=t2= 1, tsts=w0=ststi
Example. These are the symmetry groups of regulare+ 2-gons, e.g. fore= 2 the Coxeter complex is:
• H
H
H
H F F
F F
1 t s
ts
st
I will explain in a few minutes what cells are. For the moment: Never mind!
Lowest cell. Highest cell.
s-cell. t-cell.
The main example today: dihedral groups
The dihedral groups are of Coxeter type I2(e+ 2):
We+2=hs,t|s2=t2= 1, se+2 =. . .sts
| {z }
e+2
=w0=. . .tst
| {z }
e+2
=te+2i, e.g.: W4=hs,t|s2=t2= 1, tsts=w0=ststi
Example. These are the symmetry groups of regulare+ 2-gons, e.g. fore= 2 the Coxeter complex is:
• H
H
H
H F F
F F
1 t s
ts
st tst sts
I should do the Hecke case, but I will keep it easy.
I will explain in a few minutes what cells are. For the moment: Never mind!
Lowest cell. Highest cell.
s-cell. t-cell.
The main example today: dihedral groups
The dihedral groups are of Coxeter type I2(e+ 2):
We+2=hs,t|s2=t2= 1, se+2 =. . .sts
| {z }
e+2
=w0=. . .tst
| {z }
e+2
=te+2i, e.g.: W4=hs,t|s2=t2= 1, tsts=w0=ststi
Example. These are the symmetry groups of regulare+ 2-gons, e.g. fore= 2 the Coxeter complex is:
• H
H
H
H F F
F F
1 t s
ts
st tst sts
w0
I will explain in a few minutes what cells are. For the moment: Never mind!
Lowest cell. Highest cell.
s-cell. t-cell.
The main example today: dihedral groups
The dihedral groups are of Coxeter type I2(e+ 2):
We+2=hs,t|s2=t2= 1, se+2 =. . .sts
| {z }
e+2
=w0=. . .tst
| {z }
e+2
=te+2i, e.g.: W4=hs,t|s2=t2= 1, tsts=w0=ststi
Example. These are the symmetry groups of regulare+ 2-gons, e.g. fore= 2 the Coxeter complex is:
• H
H
H
H F F
F F
1 t s
ts
st tst sts
w0
I should do the Hecke case, but I will keep it easy.
I will explain in a few minutes what cells are.
For the moment: Never mind!
Lowest cell.
Highest cell. s-cell. t-cell.
The main example today: dihedral groups
The dihedral groups are of Coxeter type I2(e+ 2):
We+2=hs,t|s2=t2= 1, se+2 =. . .sts
| {z }
e+2
=w0=. . .tst
| {z }
e+2
=te+2i, e.g.: W4=hs,t|s2=t2= 1, tsts=w0=ststi
Example. These are the symmetry groups of regulare+ 2-gons, e.g. fore= 2 the Coxeter complex is:
• H
H
H
H F F
F F
1 t s
ts
st tst sts
w0
I will explain in a few minutes what cells are.
For the moment: Never mind!
Lowest cell.
Highest cell.
s-cell. t-cell.
The main example today: dihedral groups
The dihedral groups are of Coxeter type I2(e+ 2):
We+2=hs,t|s2=t2= 1, se+2 =. . .sts
| {z }
e+2
=w0=. . .tst
| {z }
e+2
=te+2i, e.g.: W4=hs,t|s2=t2= 1, tsts=w0=ststi
Example. These are the symmetry groups of regulare+ 2-gons, e.g. fore= 2 the Coxeter complex is:
• H
H
H
H F F
F F
1 t s
ts
st tst sts
w0
I should do the Hecke case, but I will keep it easy.
I will explain in a few minutes what cells are.
For the moment: Never mind!
Lowest cell.
Highest cell.
s-cell.
t-cell.
The main example today: dihedral groups
The dihedral groups are of Coxeter type I2(e+ 2):
We+2=hs,t|s2=t2= 1, se+2 =. . .sts
| {z }
e+2
=w0=. . .tst
| {z }
e+2
=te+2i, e.g.: W4=hs,t|s2=t2= 1, tsts=w0=ststi
Example. These are the symmetry groups of regulare+ 2-gons, e.g. fore= 2 the Coxeter complex is:
• H
H
H
H F F
F F
1 t s
ts
st tst sts
w0
I will explain in a few minutes what cells are.
For the moment: Never mind!
Lowest cell.
Highest cell.
s-cell.
t-cell.
Dihedral representation theory on one slide
One-dimensional modules. Mλs,λt, λs, λt∈C, θs7→λs, θt7→λt.
e≡0 mod 2 e6≡0 mod 2
M0,0,M2,0, M0,2,M2,2 M0,0,M2,2
Two-dimensional modules. Mz,z ∈C, θs7→(20 0z), θt7→(0 0z2).
e≡0 mod 2 e6≡0 mod 2
Mz,z ∈V±e−{0} Mz,z ∈V±e Ve =roots(Ue+1(X)) andVe± theZ/2Z-orbits under z 7→ −z.
The Bott–Samelson (BS) generatorsθs=s+ 1, θt=t+ 1.
There is also a Kazhdan–Lusztig (KL) bases. Explicit formulas do not matter today.
Proposition (Lusztig?).
The list of one- and two-dimensionalWe+2-modules is a complete, irredundant list of simple modules.
I learned this construction from Mackaay in 2017. Example.
M0,0is the sign representation andM2,2is the trivial representation. In casee is odd, Ue+1(X) has a constant term, soM2,0,M0,2are not representations.
Example.
Mz forz being a root of the Chebyshev polynomial is a representation because the braid relation in terms of BS generators
involves the coefficients of the Chebyshev polynomial. Example.
These representations are indexed byZ/2Z-orbits of the Chebyshev roots:
Dihedral representation theory on one slide
One-dimensional modules. Mλs,λt, λs, λt∈C, θs7→λs, θt7→λt.
e≡0 mod 2 e6≡0 mod 2
M0,0,M2,0, M0,2,M2,2 M0,0,M2,2
Two-dimensional modules. Mz,z ∈C, θs7→(20 0z), θt7→(0 0z2).
e≡0 mod 2 e6≡0 mod 2
Mz,z ∈V±e−{0} Mz,z ∈V±e Ve =roots(Ue+1(X)) andVe± theZ/2Z-orbits under z 7→ −z.
Proposition (Lusztig?).
The list of one- and two-dimensionalWe+2-modules is a complete, irredundant list of simple modules.
I learned this construction from Mackaay in 2017.
Example.
M0,0is the sign representation andM2,2is the trivial representation. In casee is odd, Ue+1(X) has a constant term, soM2,0,M0,2are not representations.
Example.
Mz forz being a root of the Chebyshev polynomial is a representation because the braid relation in terms of BS generators
involves the coefficients of the Chebyshev polynomial.
These representations are indexed byZ/2Z-orbits of the Chebyshev roots:
Dihedral representation theory on one slide
One-dimensional modules. Mλs,λt, λs, λt∈C, θs7→λs, θt7→λt.
e≡0 mod 2 e6≡0 mod 2
M0,0,M2,0, M0,2,M2,2 M0,0,M2,2
Two-dimensional modules. Mz,z ∈C, θs7→(20 0z), θt7→(0 0z2).
e≡0 mod 2 e6≡0 mod 2
Mz,z ∈V±e−{0} Mz,z ∈V±e Ve =roots(Ue+1(X)) andVe± theZ/2Z-orbits under z 7→ −z.
The Bott–Samelson (BS) generatorsθs=s+ 1, θt=t+ 1. There is also a Kazhdan–Lusztig (KL) bases. Explicit formulas do not matter today.
Proposition (Lusztig?).
The list of one- and two-dimensionalWe+2-modules is a complete, irredundant list of simple modules.
I learned this construction from Mackaay in 2017.
Example.
M0,0is the sign representation andM2,2is the trivial representation.
In casee is odd, Ue+1(X) has a constant term, soM2,0,M0,2are not representations.
Example.
Mz forz being a root of the Chebyshev polynomial is a representation because the braid relation in terms of BS generators
involves the coefficients of the Chebyshev polynomial. Example.
These representations are indexed byZ/2Z-orbits of the Chebyshev roots:
Dihedral representation theory on one slide
One-dimensional modules. Mλs,λt, λs, λt∈C, θs7→λs, θt7→λt.
e≡0 mod 2 e6≡0 mod 2
M0,0,M2,0, M0,2,M2,2 M0,0,M2,2
Two-dimensional modules. Mz,z ∈C, θs7→(20 0z), θt7→(0 0z2).
e≡0 mod 2 e6≡0 mod 2
Mz,z ∈V±e−{0} Mz,z ∈V±e Ve =roots(Ue+1(X)) andVe± theZ/2Z-orbits under z 7→ −z.
Proposition (Lusztig?).
The list of one- and two-dimensionalWe+2-modules is a complete, irredundant list of simple modules.
I learned this construction from Mackaay in 2017. Example.
M0,0is the sign representation andM2,2is the trivial representation. In casee is odd, Ue+1(X) has a constant term, soM2,0,M0,2are not representations.
Example.
Mz forz being a root of the Chebyshev polynomial is a representation because the braid relation in terms of BS generators
involves the coefficients of the Chebyshev polynomial.
These representations are indexed byZ/2Z-orbits of the Chebyshev roots:
Dihedral representation theory on one slide
One-dimensional modules. Mλs,λt, λs, λt∈C, θs7→λs, θt7→λt.
e≡0 mod 2 e6≡0 mod 2
M0,0,M2,0, M0,2,M2,2 M0,0,M2,2
Two-dimensional modules. Mz,z ∈C, θs7→(20 0z), θt7→(0 0z2).
e≡0 mod 2 e6≡0 mod 2
Mz,z ∈V±e−{0} Mz,z ∈V±e Ve =roots(Ue+1(X)) andVe± theZ/2Z-orbits under z 7→ −z.
The Bott–Samelson (BS) generatorsθs=s+ 1, θt=t+ 1. There is also a Kazhdan–Lusztig (KL) bases. Explicit formulas do not matter today.
Proposition (Lusztig?).
The list of one- and two-dimensionalWe+2-modules is a complete, irredundant list of simple modules.
I learned this construction from Mackaay in 2017. Example.
M0,0is the sign representation andM2,2is the trivial representation. In casee is odd, Ue+1(X) has a constant term, soM2,0,M0,2are not representations.
Example.
Mz forz being a root of the Chebyshev polynomial is a representation because the braid relation in terms of BS generators
involves the coefficients of the Chebyshev polynomial.
Example.
These representations are indexed byZ/2Z-orbits of the Chebyshev roots:
N
0-algebras and their representations
An algebra Pwith a basisBP with 1∈BP is called aN0-algebra if xy∈N0BP (x,y∈BP).
AP-moduleMwith a basisBM is called anN0-module if xm∈N0BM (x∈BP,m∈BM).
These are N0-equivalent if there is aN0-valued change of basis matrix.
Example. N0-algebras andN0-modules arise naturally as the decategorification of 2-categories and 2-modules, andN0-equivalence comes from 2-equivalence upstairs.
Group algebras of finite groups with basis given by group elements areN0-algebras. The regular representation is anN0-module.
Example.
The regular representation of group algebras decomposes overCinto simples. However, this decomposition is almost never anN0-equivalence.
Example.
Hecke algebras of (finite) Coxeter groups with their KL basis areN0-algebras. For the symmetric group a miracle happens: all simples areN0-modules.
N
0-algebras and their representations
An algebra Pwith a basisBP with 1∈BP is called aN0-algebra if xy∈N0BP (x,y∈BP).
AP-moduleMwith a basisBM is called anN0-module if xm∈N0BM (x∈BP,m∈BM).
These are N0-equivalent if there is aN0-valued change of basis matrix.
Example. N0-algebras andN0-modules arise naturally as the decategorification of 2-categories and 2-modules, andN0-equivalence comes from 2-equivalence upstairs.
Example.
Group algebras of finite groups with basis given by group elements areN0-algebras.
The regular representation is anN0-module.
Example.
The regular representation of group algebras decomposes overCinto simples. However, this decomposition is almost never anN0-equivalence.
Example.
Hecke algebras of (finite) Coxeter groups with their KL basis areN0-algebras. For the symmetric group a miracle happens: all simples areN0-modules.
N
0-algebras and their representations
An algebra Pwith a basisBP with 1∈BP is called aN0-algebra if xy∈N0BP (x,y∈BP).
AP-moduleMwith a basisBM is called anN0-module if xm∈N0BM (x∈BP,m∈BM).
These are N0-equivalent if there is aN0-valued change of basis matrix.
Example. N0-algebras andN0-modules arise naturally as the decategorification of 2-categories and 2-modules, andN0-equivalence comes from 2-equivalence upstairs.
Example.
Group algebras of finite groups with basis given by group elements areN0-algebras.
The regular representation is anN0-module.
Example.
The regular representation of group algebras decomposes overCinto simples.
However, this decomposition is almost never anN0-equivalence.
Hecke algebras of (finite) Coxeter groups with their KL basis areN0-algebras. For the symmetric group a miracle happens: all simples areN0-modules.
N
0-algebras and their representations
An algebra Pwith a basisBP with 1∈BP is called aN0-algebra if xy∈N0BP (x,y∈BP).
AP-moduleMwith a basisBM is called anN0-module if xm∈N0BM (x∈BP,m∈BM).
These are N0-equivalent if there is aN0-valued change of basis matrix.
Example. N0-algebras andN0-modules arise naturally as the decategorification of 2-categories and 2-modules, andN0-equivalence comes from 2-equivalence upstairs.
Example.
Group algebras of finite groups with basis given by group elements areN0-algebras.
The regular representation is anN0-module.
Example.
The regular representation of group algebras decomposes overCinto simples.
However, this decomposition is almost never anN0-equivalence.
Example.
Hecke algebras of (finite) Coxeter groups with their KL basis areN0-algebras.
For the symmetric group a miracle happens: all simples areN0-modules.
Cells of N
0-algebras and N
0-modules
Kazhdan–Lusztig ∼1979. x≤Lyifxappears inzywith non-zero coefficient for somez∈BP. x∼Lyif x≤Lyandy≤Lx.
∼Lpartitions Pinto cells L. Similarly for right R, two-sided cells J orN0-modules.
AnN0-module Mis transitive if all basis elements belong to the same∼L equivalence class. An apex ofMis a maximal two-sided cell not killing it.
Fact. Each transitiveN0-module has a unique apex.
Example. TransitiveN0-modules arise as decategorifications of simple 2-modules.
Philosophy.
Imagine a graph whose vertices are thex’s or them’s. v1→v2ifv1appears inzv2.
cells = connected components transitive = one connected component
“The basic building blocks ofN0-representation theory”. Group algebras with the group element basis have only one cell,G itself. TransitiveN0-modules areC[G/H] forH being a subgroup. The apex isG.
Example (Kazhdan–Lusztig∼1979). Hecke algebras for the symmetric group with KL basis
have cells coming from the Robinson–Schensted correspondence.
The transitiveN0-modules are the simples
with apex given by elements for the same shape of Young tableaux. Example (Lusztig ≤2003).
Hecke algebras for the dihedral group with KL basis have the following cells:
1
s ts sts tsts ststs
t st tst stst tstst w0
We will see the transitiveN0-modules in a second.
Left cells Right cells Two-sided cells
Cells of N
0-algebras and N
0-modules
Kazhdan–Lusztig ∼1979. x≤Lyifxappears inzywith non-zero coefficient for somez∈BP. x∼Lyif x≤Lyandy≤Lx.
∼Lpartitions Pinto cells L. Similarly for right R, two-sided cells J orN0-modules.
AnN0-module Mis transitive if all basis elements belong to the same∼L equivalence class. An apex ofMis a maximal two-sided cell not killing it.
Fact. Each transitiveN0-module has a unique apex.
Example. TransitiveN0-modules arise as decategorifications of simple 2-modules.
Philosophy.
Imagine a graph whose vertices are thex’s or them’s.
v1→v2ifv1appears inzv2.
x1
x2
x3
x4 m1
m2
m3
m4
cells = connected components transitive = one connected component
“The basic building blocks ofN0-representation theory”.
Example.
Group algebras with the group element basis have only one cell,G itself. TransitiveN0-modules areC[G/H] forH being a subgroup. The apex isG.
Example (Kazhdan–Lusztig∼1979). Hecke algebras for the symmetric group with KL basis
have cells coming from the Robinson–Schensted correspondence.
The transitiveN0-modules are the simples
with apex given by elements for the same shape of Young tableaux. Example (Lusztig ≤2003).
Hecke algebras for the dihedral group with KL basis have the following cells:
1
s ts sts tsts ststs
t st tst stst tstst w0
We will see the transitiveN0-modules in a second.
Left cells Right cells Two-sided cells
Cells of N
0-algebras and N
0-modules
Kazhdan–Lusztig ∼1979. x≤Lyifxappears inzywith non-zero coefficient for somez∈BP. x∼Lyif x≤Lyandy≤Lx.
∼Lpartitions Pinto cells L. Similarly for right R, two-sided cells J orN0-modules.
AnN0-module Mis transitive if all basis elements belong to the same∼L equivalence class. An apex ofMis a maximal two-sided cell not killing it.
Fact. Each transitiveN0-module has a unique apex.
Example. TransitiveN0-modules arise as decategorifications of simple 2-modules.
Philosophy.
Imagine a graph whose vertices are thex’s or them’s.
v1→v2ifv1appears inzv2.
x1
x2
x3
x4 m1
m2
m3
m4
cells = connected components transitive = one connected component
“The basic building blocks ofN0-representation theory”.
Group algebras with the group element basis have only one cell,G itself. TransitiveN0-modules areC[G/H] forH being a subgroup. The apex isG.
Example (Kazhdan–Lusztig∼1979). Hecke algebras for the symmetric group with KL basis
have cells coming from the Robinson–Schensted correspondence.
The transitiveN0-modules are the simples
with apex given by elements for the same shape of Young tableaux. Example (Lusztig ≤2003).
Hecke algebras for the dihedral group with KL basis have the following cells:
1
s ts sts tsts ststs
t st tst stst tstst w0
We will see the transitiveN0-modules in a second.
Left cells Right cells Two-sided cells
Cells of N
0-algebras and N
0-modules
Kazhdan–Lusztig ∼1979. x≤Lyifxappears inzywith non-zero coefficient for somez∈BP. x∼Lyif x≤Lyandy≤Lx.
∼Lpartitions Pinto cells L. Similarly for right R, two-sided cells J orN0-modules.
AnN0-module Mis transitive if all basis elements belong to the same∼L equivalence class. An apex ofMis a maximal two-sided cell not killing it.
Fact. Each transitiveN0-module has a unique apex.
Example. TransitiveN0-modules arise as decategorifications of simple 2-modules.
Philosophy.
Imagine a graph whose vertices are thex’s or them’s.
v1→v2ifv1appears inzv2.
x1
x2
x3
x4 m1
m2
m3
m4
cells = connected components transitive = one connected component
“The basic building blocks ofN0-representation theory”.
Example.
Group algebras with the group element basis have only one cell,G itself. TransitiveN0-modules areC[G/H] forH being a subgroup. The apex isG.
Example (Kazhdan–Lusztig∼1979). Hecke algebras for the symmetric group with KL basis
have cells coming from the Robinson–Schensted correspondence.
The transitiveN0-modules are the simples
with apex given by elements for the same shape of Young tableaux. Example (Lusztig ≤2003).
Hecke algebras for the dihedral group with KL basis have the following cells:
1
s ts sts tsts ststs
t st tst stst tstst w0
We will see the transitiveN0-modules in a second.
Left cells Right cells Two-sided cells
Cells of N
0-algebras and N
0-modules
Kazhdan–Lusztig ∼1979. x≤Lyifxappears inzywith non-zero coefficient for somez∈BP. x∼Lyif x≤Lyandy≤Lx.
∼Lpartitions Pinto cells L. Similarly for right R, two-sided cells J orN0-modules.
AnN0-module Mis transitive if all basis elements belong to the same∼L equivalence class. An apex ofMis a maximal two-sided cell not killing it.
Fact. Each transitiveN0-module has a unique apex.
Example. TransitiveN0-modules arise as decategorifications of simple 2-modules.
Imagine a graph whose vertices are thex’s or them’s. v1→v2ifv1appears inzv2.
cells = connected components transitive = one connected component
“The basic building blocks ofN0-representation theory”.
Example.
Group algebras with the group element basis have only one cell,G itself.
TransitiveN0-modules areC[G/H] forH being a subgroup. The apex isG.
Example (Kazhdan–Lusztig∼1979). Hecke algebras for the symmetric group with KL basis
have cells coming from the Robinson–Schensted correspondence.
The transitiveN0-modules are the simples
with apex given by elements for the same shape of Young tableaux. Example (Lusztig ≤2003).
Hecke algebras for the dihedral group with KL basis have the following cells:
1
s ts sts tsts ststs
t st tst stst tstst w0
We will see the transitiveN0-modules in a second.
Left cells Right cells Two-sided cells
Cells of N
0-algebras and N
0-modules
Kazhdan–Lusztig ∼1979. x≤Lyifxappears inzywith non-zero coefficient for somez∈BP. x∼Lyif x≤Lyandy≤Lx.
∼Lpartitions Pinto cells L. Similarly for right R, two-sided cells J orN0-modules.
AnN0-module Mis transitive if all basis elements belong to the same∼L equivalence class. An apex ofMis a maximal two-sided cell not killing it.
Fact. Each transitiveN0-module has a unique apex.
Example. TransitiveN0-modules arise as decategorifications of simple 2-modules.
Philosophy.
Imagine a graph whose vertices are thex’s or them’s. v1→v2ifv1appears inzv2.
cells = connected components transitive = one connected component
“The basic building blocks ofN0-representation theory”.
Example.
Group algebras with the group element basis have only one cell,G itself.
TransitiveN0-modules areC[G/H] forH being a subgroup. The apex isG.
Example (Kazhdan–Lusztig∼1979).
Hecke algebras for the symmetric group with KL basis
have cells coming from the Robinson–Schensted correspondence.
The transitiveN0-modules are the simples
with apex given by elements for the same shape of Young tableaux.
Example (Lusztig ≤2003).
Hecke algebras for the dihedral group with KL basis have the following cells:
1
s ts sts tsts ststs
t st tst stst tstst w0
We will see the transitiveN0-modules in a second.
Left cells Right cells Two-sided cells
Cells of N
0-algebras and N
0-modules
Kazhdan–Lusztig ∼1979. x≤Lyifxappears inzywith non-zero coefficient for somez∈BP. x∼Lyif x≤Lyandy≤Lx.
∼Lpartitions Pinto cells L. Similarly for right R, two-sided cells J orN0-modules.
AnN0-module Mis transitive if all basis elements belong to the same∼L equivalence class. An apex ofMis a maximal two-sided cell not killing it.
Fact. Each transitiveN0-module has a unique apex.
Example. TransitiveN0-modules arise as decategorifications of simple 2-modules.
Imagine a graph whose vertices are thex’s or them’s. v1→v2ifv1appears inzv2.
cells = connected components transitive = one connected component
“The basic building blocks ofN0-representation theory”.
Example.
Group algebras with the group element basis have only one cell,G itself.
TransitiveN0-modules areC[G/H] forH being a subgroup. The apex isG.
Example (Kazhdan–Lusztig∼1979).
Hecke algebras for the symmetric group with KL basis
have cells coming from the Robinson–Schensted correspondence.
The transitiveN0-modules are the simples
with apex given by elements for the same shape of Young tableaux.
Example (Lusztig ≤2003).
Hecke algebras for the dihedral group with KL basis have the following cells:
1
s ts sts tsts ststs w
Left cells
Right cells Two-sided cells
Cells of N
0-algebras and N
0-modules
Kazhdan–Lusztig ∼1979. x≤Lyifxappears inzywith non-zero coefficient for somez∈BP. x∼Lyif x≤Lyandy≤Lx.
∼Lpartitions Pinto cells L. Similarly for right R, two-sided cells J orN0-modules.
AnN0-module Mis transitive if all basis elements belong to the same∼L equivalence class. An apex ofMis a maximal two-sided cell not killing it.
Fact. Each transitiveN0-module has a unique apex.
Example. TransitiveN0-modules arise as decategorifications of simple 2-modules.
Philosophy.
Imagine a graph whose vertices are thex’s or them’s. v1→v2ifv1appears inzv2.
cells = connected components transitive = one connected component
“The basic building blocks ofN0-representation theory”.
Example.
Group algebras with the group element basis have only one cell,G itself.
TransitiveN0-modules areC[G/H] forH being a subgroup. The apex isG.
Example (Kazhdan–Lusztig∼1979).
Hecke algebras for the symmetric group with KL basis
have cells coming from the Robinson–Schensted correspondence.
The transitiveN0-modules are the simples
with apex given by elements for the same shape of Young tableaux.
Example (Lusztig ≤2003).
Hecke algebras for the dihedral group with KL basis have the following cells:
1
s ts sts tsts ststs w0
Left cells
Right cells
Two-sided cells
Cells of N
0-algebras and N
0-modules
Kazhdan–Lusztig ∼1979. x≤Lyifxappears inzywith non-zero coefficient for somez∈BP. x∼Lyif x≤Lyandy≤Lx.
∼Lpartitions Pinto cells L. Similarly for right R, two-sided cells J orN0-modules.
AnN0-module Mis transitive if all basis elements belong to the same∼L equivalence class. An apex ofMis a maximal two-sided cell not killing it.
Fact. Each transitiveN0-module has a unique apex.
Example. TransitiveN0-modules arise as decategorifications of simple 2-modules.
Imagine a graph whose vertices are thex’s or them’s. v1→v2ifv1appears inzv2.
cells = connected components transitive = one connected component
“The basic building blocks ofN0-representation theory”.
Example.
Group algebras with the group element basis have only one cell,G itself.
TransitiveN0-modules areC[G/H] forH being a subgroup. The apex isG.
Example (Kazhdan–Lusztig∼1979).
Hecke algebras for the symmetric group with KL basis
have cells coming from the Robinson–Schensted correspondence.
The transitiveN0-modules are the simples
with apex given by elements for the same shape of Young tableaux.
Example (Lusztig ≤2003).
Hecke algebras for the dihedral group with KL basis have the following cells:
1
s ts sts tsts ststs w
Left cells Right cells
Two-sided cells
N
0-modules via graphs
Construct aW∞-moduleMassociated to a bipartite graphΓ:
M=Ch1,2,3,4,5i
1 3 2 4 5
H F H
F
F
θs Ms=
2 0 1 0 0 0 2 1 1 1 0 0 0 0 0
, θt Mt=
0 0 0 0 0 0 0 0 0 0 1 1 2 0 0
The adjacency matrixA(Γ) ofΓis
A(Γ) =
0 0 1 0 0 0 0 1 1 1 1 1 0 0 0 0 1 0 0 0 0 1 0 0 0
These areWe+2-modules for somee
only ifA(Γ) is killed by the Chebyshev polynomial Ue+1(X). Morally speaking: These are constructed as the simples but with integral matrices having the Chebyshev-roots as eigenvalues.
It is not hard to see that the Chebyshev–braid-like relation can not hold otherwise.
Hence, by Smith’s (CP) and Lusztig: We get a representation ofWe+2
ifΓis a ADE Dynkin diagram fore+ 2 being the Coxeter number. That these areN0-modules follows from categorification.
‘Smaller solutions’ are neverN0-modules.
Classification.
Complete , irredundant list of transitiveN0-modules ofWe+2:
Apex 1 cell s – t cell w0 cell
N0-reps. M0,0 MADE+bicoleringfor e+ 2 = Cox. num. M2,2
I learned this from/with Kildetoft–Mackaay–Mazorchuk–Zimmermann∼2016.
N
0-modules via graphs
Construct aW∞-moduleMassociated to a bipartite graphΓ:
M=Ch1,2,3,4,5i
1 3 2 4 5
θs
action
H F H
F
F
2 0 1 0 0 0 2 1 1 1
0 0 0 0 0 0 0 0 0 0
A(Γ) =
0 0 1 0 0 0 0 1 1 1 1 1 0 0 0 0 1 0 0 0 0 1 0 0 0
These areWe+2-modules for somee
only ifA(Γ) is killed by the Chebyshev polynomial Ue+1(X). Morally speaking: These are constructed as the simples but with integral matrices having the Chebyshev-roots as eigenvalues.
It is not hard to see that the Chebyshev–braid-like relation can not hold otherwise.
Hence, by Smith’s (CP) and Lusztig: We get a representation ofWe+2
ifΓis a ADE Dynkin diagram fore+ 2 being the Coxeter number. That these areN0-modules follows from categorification.
‘Smaller solutions’ are neverN0-modules.
Classification.
Complete , irredundant list of transitiveN0-modules ofWe+2:
Apex 1 cell s – t cell w0 cell
N0-reps. M0,0 MADE+bicoleringfor e+ 2 = Cox. num. M2,2
I learned this from/with Kildetoft–Mackaay–Mazorchuk–Zimmermann∼2016.
N
0-modules via graphs
Construct aW∞-moduleMassociated to a bipartite graphΓ:
M=Ch1,2,3,4,5i
1 3 2 4 5
θs
action
H F H
F
F
θs Ms=
2 0 1 0 0 0 2 1 1 1 0 0 0 0 0
, θt Mt=
0 0 0 0 0 0 0 0 0 0 1 1 2 0 0
The adjacency matrixA(Γ) ofΓis
A(Γ) =
0 0 1 0 0 0 0 1 1 1 1 1 0 0 0 0 1 0 0 0 0 1 0 0 0
These areWe+2-modules for somee
only ifA(Γ) is killed by the Chebyshev polynomial Ue+1(X). Morally speaking: These are constructed as the simples but with integral matrices having the Chebyshev-roots as eigenvalues.
It is not hard to see that the Chebyshev–braid-like relation can not hold otherwise.
Hence, by Smith’s (CP) and Lusztig: We get a representation ofWe+2
ifΓis a ADE Dynkin diagram fore+ 2 being the Coxeter number. That these areN0-modules follows from categorification.
‘Smaller solutions’ are neverN0-modules.
Classification.
Complete , irredundant list of transitiveN0-modules ofWe+2:
Apex 1 cell s – t cell w0 cell
N0-reps. M0,0 MADE+bicoleringfor e+ 2 = Cox. num. M2,2
I learned this from/with Kildetoft–Mackaay–Mazorchuk–Zimmermann∼2016.
N
0-modules via graphs
Construct aW∞-moduleMassociated to a bipartite graphΓ:
M=Ch1,2,3,4,5i
1 3 2 4 5
θs
action
H F H
F
F
2 0 1 0 0 0 2 1 1 1
0 0 0 0 0 0 0 0 0 0
A(Γ) =
0 0 1 0 0 0 0 1 1 1 1 1 0 0 0 0 1 0 0 0 0 1 0 0 0
These areWe+2-modules for somee
only ifA(Γ) is killed by the Chebyshev polynomial Ue+1(X). Morally speaking: These are constructed as the simples but with integral matrices having the Chebyshev-roots as eigenvalues.
It is not hard to see that the Chebyshev–braid-like relation can not hold otherwise.
Hence, by Smith’s (CP) and Lusztig: We get a representation ofWe+2
ifΓis a ADE Dynkin diagram fore+ 2 being the Coxeter number. That these areN0-modules follows from categorification.
‘Smaller solutions’ are neverN0-modules.
Classification.
Complete , irredundant list of transitiveN0-modules ofWe+2:
Apex 1 cell s – t cell w0 cell
N0-reps. M0,0 MADE+bicoleringfor e+ 2 = Cox. num. M2,2
I learned this from/with Kildetoft–Mackaay–Mazorchuk–Zimmermann∼2016.
N
0-modules via graphs
Construct aW∞-moduleMassociated to a bipartite graphΓ:
M=Ch1,2,3,4,5i
1 3 2 4 5
θs
action
H F H
F
F
θs Ms=
2 0 1 0 0 0 2 1 1 1 0 0 0 0 0
, θt Mt=
0 0 0 0 0 0 0 0 0 0 1 1 2 0 0
The adjacency matrixA(Γ) ofΓis
A(Γ) =
0 0 1 0 0 0 0 1 1 1 1 1 0 0 0 0 1 0 0 0 0 1 0 0 0
These areWe+2-modules for somee
only ifA(Γ) is killed by the Chebyshev polynomial Ue+1(X). Morally speaking: These are constructed as the simples but with integral matrices having the Chebyshev-roots as eigenvalues.
It is not hard to see that the Chebyshev–braid-like relation can not hold otherwise.
Hence, by Smith’s (CP) and Lusztig: We get a representation ofWe+2
ifΓis a ADE Dynkin diagram fore+ 2 being the Coxeter number. That these areN0-modules follows from categorification.
‘Smaller solutions’ are neverN0-modules.
Classification.
Complete , irredundant list of transitiveN0-modules ofWe+2:
Apex 1 cell s – t cell w0 cell
N0-reps. M0,0 MADE+bicoleringfor e+ 2 = Cox. num. M2,2
I learned this from/with Kildetoft–Mackaay–Mazorchuk–Zimmermann∼2016.
N
0-modules via graphs
Construct aW∞-moduleMassociated to a bipartite graphΓ:
M=Ch1,2,3,4,5i
1 3 2 4 5
θs
action
H F H
F
F
2 0 1 0 0 0 2 1 1 1
0 0 0 0 0 0 0 0 0 0
A(Γ) =
0 0 1 0 0 0 0 1 1 1 1 1 0 0 0 0 1 0 0 0 0 1 0 0 0
These areWe+2-modules for somee
only ifA(Γ) is killed by the Chebyshev polynomial Ue+1(X). Morally speaking: These are constructed as the simples but with integral matrices having the Chebyshev-roots as eigenvalues.
It is not hard to see that the Chebyshev–braid-like relation can not hold otherwise.
Hence, by Smith’s (CP) and Lusztig: We get a representation ofWe+2
ifΓis a ADE Dynkin diagram fore+ 2 being the Coxeter number. That these areN0-modules follows from categorification.
‘Smaller solutions’ are neverN0-modules.
Classification.
Complete , irredundant list of transitiveN0-modules ofWe+2:
Apex 1 cell s – t cell w0 cell
N0-reps. M0,0 MADE+bicoleringfor e+ 2 = Cox. num. M2,2
I learned this from/with Kildetoft–Mackaay–Mazorchuk–Zimmermann∼2016.