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Poincar´e Series of the Weyl Groups of the Elliptic Root Systems A

(1,1)1

, A

(1,1)1

and A

(1,1)2

TADAYOSHI TAKEBAYASHI [email protected]

Department of Mathematical Science, School of Science and Engineering, Waseda University, Ohkubo Shinjuku-ku, Tokyo, 169-8555

Received February 8, 2001; Revised September 10, 2002

Abstract. We calculate the Poincar´e series of the elliptic Weyl groupW(A(1,1)2 ), which is the Weyl group of the elliptic root system of typeA(1,1)2 . The generators and relations ofW(A(1,1)2 ) have been already given by K. Saito and the author.

Keywords: Poincar´e series, elliptic root system, elliptic Weyl group

1. Introduction

Elliptic Weyl groups are the Weyl groups associated to the elliptic root systems intro- duced by K. Saito [5, 6], which are defined by a semi-positive definite inner product with 2-dimensional radical. The generators and their relations of elliptic Weyl groups were de- scribed from the viewpoint of a generalization of Coxeter groups by K. Saito and the author [7, 9]. The Poincar´e seriesW(t) of a groupW with respect to a generator system is defined by

W(t)=

w∈W

tl(w),

wheretis an indeterminate andl(w) is the length of a minimal expression of an elementw inWin terms of the given generator system. IfWis one of the finite or affine Weyl groups, it is known that

w∈W

tl(w)=







 n i=1

1−tmi+1

1−t (W: finite),

1 (1−t)n

n i=1

1−tmi+1

1−t (W: affine),

wheren is the rank and m1, . . . ,mn are the exponents of W [1–4, 8]. The goal of the present article is to calculate the Poincar´e series W(t) of the elliptic Weyl groups W of types A(1,1)1 ,A(1,1)1 andA(1,1)2 . In the cases of types A(1,1)1 and A(1,1)∗1 ,although they have

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been already given by Wakimoto [10], we give a different proof from those and in the similar way we calculate the case of A(1,1)2 . The result forA(1,1)2 is given by Theorem 3.7.

2. Poincar´e series of the Weyl groups of typesA(1,1)1 andA(1,1)1

The generators and their relations of the elliptic Weyl group of type A(11,1)are given as follows [7, 9]:

Generators: wi, wi (i=0,1).

Relations: wi2=wi2=1 (i=0,1), w0w0w1w1 =1.

The relationw0w0w1w1=1 is rewritten as follows:

w0w1=w0w1(⇔w1w0=w1w0). (2.1.1) (It means thatwiwj =wiwj (i = j).) We setT :=w1w0,R:=w1w1 =w0w0, then we easily see the following.

Lemma 2.1 The elements T,R andw1 generate the Weyl group of type A(1,1)1 and their fundamental relations are given by;

TR=RT, w1T =T1w1, w1R=R1w1, w21=1.

From this, we haveW = {RmTnw1, RmTn,m,n ∈Z}. The elementsT andw1generate a subgroup isomorphic to the affine Weyl group of type A1,and all elements of that are classified to the following:

{(I) Tn(n ≥0), (II) Tn(n≥1), (III) Tnw1(n≥0), (IV) Tnw1(n ≥1)}.

We multiply the elements Rm(m ∈ Z) to the above elements from the left, and examine their minimal length in each case by using the following.

Lemma 2.2 Letwbe a minimal expression byw0andw1. Then even if we attachto any letters ofw,the length ofwdoes not decrease.

Proof: This is clear from the fact that a relation inwiholds if and only if the relation in wiobtained by attaching∗also holds.

(I) Tn =(w1w0)n (n≥0)

From the expression Rw1w0 = w1w0 and (2.1.1), we see that RkTn = Rk(w1w0)n = (w11w10)(w21w20)· · ·(wn1wn0), for 0≤k≤2n, wherewi1(resp.wi0) is eitherw1orw1 (resp.w0orw0) for alli, in such a way that∗is attached until thek-th letter. Further for m ≥1, R2n+mTn = Rm(R2nTn)= (w1w1)m(w1w0)n,RmTn = (w1w1)m(w1w0)n, and

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each length is 2n+2m, so we get{RkTn, (n ≥ 0, k∈ Z)|l(RkTn)=2n} =2n+1, and{RkTn, (n ≥0, k∈Z)|l(RkTn)=2n+2m} =2.

The case of (II) is similar to (I).

(III) Tnw1=(w1w0)nw1 (n≥0)

From Rw1 =w1and (2.1.1), for 0≤k ≤2n+1, we have RkTnw1 = Rk(w1w0)nw1 = (w11w10)· · ·(wn1wn0)wn+1,1wherewi1 ∈ {w1, w1}andwi0 ∈ {w0, w0}, so{RkTnw1, (n ≥ 0, k ∈ Z) | l(RkTnw1) = 2n+1} = 2n +2, and{RkTnw1,(n ≥ 0, k ∈ Z) | l(RkTnw1)=2n+1+2m} ={R2n+1+mTnw1, RmTnw1} =2.

(IV) Tnw1=(w0w1)n−1w0 (n ≥1)

FromR1w0 =w0, (2.1.1), and that form≥1,R(2n1)mTnw1=Rm(w0w1)n1w0 = (w0w0)m(w0w1)n1w0,RmTnw1=(w0w0)m(w0w1)n1w0, we see that {RkTnw1, (n ≥ 1, k ∈ Z) | l(RkTnw1) = 2n −1} = 2n, and {RkTnw1, (n ≥ 1, k ∈ Z) | l(RkTnw1)=2n+2m−1} =2.

In the case of typeA(1,1)∗1 , the generators and their relations are given as follows:

Generators: w0, w1, w1.

Relations: w20=w12=w12 =(w0w1w1)2=1.

This Weyl group is obtained from the Weyl group of typeA(11,1)by removing one generator w0, so we examine the case of typeA(11,1)similarly to the case of typeA(11,1).

(I) Tn =(w1w0)n (n≥0)

From Rw1 =w1, we haveRnTn =(w1w0)n, and form≥1, Rn+mTn = Rm(w1w0)n = (w1w1)m(w1w0)n and RmTn =(w1w1)m(w1w0)n, so we get{RkTn,(n ≥ 0,k ∈ Z) | l(RkTn)=2n} =n+1, and{RkTn,(n ≥0,k∈Z)|l(RkTn)=2n+2m} =2.

The case of (II) is similar to (I).

(III) Tnw1=(w1w0)nw1 (n≥0)

From Rw1=w1, andRn+1(w1w0)nw1=(w1w0)nw1, we see that{RkTnw1,(n≥0,k∈ Z)|l(RkTnw1)=2n+1} =n+2, and{RkTnw1,k∈Z|l(RkTnw1)=2n+1+2m} = {Rn+1+mTnw1,RmTnw1} =2.

(IV) Tnw1=(w0w1)n1w0 (n ≥1)

From R−1(w0w1)=w0w1 and R−(n−1)(w0w1)n−1w0=(w0w1)n−1w0, we see that {RkTnw1, (n ≥ 1, k ∈ Z) | l(RkTnw1) = 2n −1} = n, and{RkTnw1, k ∈ Z|l(RkTnw1)=2n−1+2m} ={Rn+1−mTnw1, RmTnw1} =2.

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From the above argument, we obtain the following.

A(11,1) l(w) (n1,m1) A(11,1) l(w) (n1,m1)

I 0 1 I 0 1

2n 2n+1 2n n+1

2m, 2(n+m) 2 2m, 2(n+m) 2

II 2n 2n+1 II 2n n+1

2(n+m) 2 2(n+m) 2

III 2n1 2n III 2n1 n+1

2(n+m)1 2 2(n+m)1 2

IV 2n1 2n IV 2n1 n

2(n+m)1 2 2(n+m)1 2

Further from this, we obtain the following.

Proposition 2.3([10])

(i) The number of the elements of W(A(1,1)1 )and W(A(1,1)∗1 )of length n is given by;

W

A(1,1)1 : {wW |l(w)=0} =1, {w∈W |l(w)=n, (n≥1)} =4n, W

A(11,1) : {wW |l(w)=0} =1, {wW |l(w)=n, (n≥1)} =3n. (ii) The Poincar´e series of W(A(1,1)1 )and W(A(1,1)∗1 )are given by;

w∈W(A(1,1)1 )

tl(w)= (1+t)2

(1−t)2,

w∈W(A(1.1)∗1 )

tl(w)= 1−t3 (1−t)3.

Proof: (i) For an integerk ≥2,the number of pairs (m,n) satisfyingk=m+n(m ≥ 1,n ≥ 1) is equal tok−1,so in the case of type A(1,1)1 , {wW | l(w) = 2n} = (2n +1)×2+2+2×(n −1)×2 = 8n, and {wW | l(w) = 2n −1} = 2n×2+2×(n−1)×2=8n−4,so we get the result. The case of typeA(1,1)∗1 is calculated similarly. Then (ii) is easily obtained from (i).

3. Poincar´e series of the Weyl group of type A(1,1)2

The elliptic Weyl groupW of typeA(12,1)is presented as follows [7, 9].

Generators: wi, wi (i =0,1,2).

Relations: wi2=w∗2i =1 (i=0,1,2), for i= j

wiwjwi =wjwiwj, wiwjwi =wjwiwj, wiwjwi =wjwiwj =wiwjwi =wjwiwj, and w0w0w1w1w2w2 =1.

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We setT1:=w0w2w0w1,T2:=w0w1w0w2,R1:=w1w1, andR2:=w2w2, then we have the following.

Lemma 3.1

(i) W is generated byw1, w2,T1,T2,R1,R2,and they satisfy the following fundamental relations:









wiTi =Ti1wi

wiRi=R−1i wi

wiTj =TiTjwi (i = j) wiRj =RiRjwi (i = j).

(ii) W = {R1nRm2T1kT2lw, (n,m,k,l ∈Z)|w=id, w1, w2, w1w2, w2w1, w1w2w1}.

Proof: Letbe the elliptic root system of typeA(1,1)2 , then one has the expression [5]

= {±(ij)+nb+ma|1≤i < j ≤3, n,m∈Z}, with an inner product,, which is a symmetric bilinear form given by

i, j =δi j, i,a = i,b = a,b = a,a = b,b =0, (1≤i, j≤3).

LetF =

1i<j3R(ij)⊕Rb⊕Rabe a real vector space. Letwαbe the reflection corresponding to the rootαdefined bywα(x)=x−<x, α > α, ∀x ∈ F withα =

α,α . We setα0:=31+b, α1:=12, α2:=23andαi:=αi+a(i=0,1,2).

Thenwi=wαi, wi =wαi. We see that all reflections act onRb⊕Raas identity, and





w1(1)=2

w1(2)=1

w1(3)=3





w2(1)=1

w2(2)=3

w2(3)=2





w0(1)=3+b w0(2)=2

w0(3)=1b





w1(1)=2a w1(2)=1+a w1(3)=3





w2(1)=1

w2(2)=3a w2(3)=2+a





w0(1)=3+a w0(2)=2

w0(3)=1a From these, we have the following:



T1(1)=1b T1(2)=2+b T1(3)=3



T2(1)=1

T2(2)=2b T2(3)=3+b



R1(1)=1a R1(2)=2+a R1(3)=3



R2(1)=1

R2(2)=2a R2(3)=3+a From these actions, we have

w0=T1T2w1w2w1, w0=R1R2T1T2w1w2w1, w1=w1R1, w2=w2R2, and from this, (i) is easily checked. (ii) follows from (i).

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We first consider minimal expressions of the elements T1nT2m generated by T1 = w0w2w0w1,andT2=w0w1w0w2, then by noting the following minimal expressions;

T1T2=w0w1w2w1, T1T2−1=(w2w0w1)2, T1T22=(w0w1w2)2,

we haveT1nT2n+i =(0121)n(0102)i=(012)2(0121)n−1(0102)i−1, and from this we obtain

T1nT2n+i(n≥1,i ≥1)=

T1nT2n+i =(012)2i(0121)ni (1≤i <n,n ≥2) T1nT22n+i =(0102)i(012)2n (i ≥0,n ≥1)

where for brevity, we use 0,1,2,0,1,2forw0,w1,w2,w0,w1,w2, respectively. Further by considering minimal expressions ofT1nT2mw(w =w1, w2, w1w2, w2w1, w1w2w1), we classifyT1nT2m(n,m∈Z) as follows.

T1nT2m(n,m∈Z)=































T1nT2n+i =(012)2i(0121)ni (1≤i <n, n≥2) (1↔2) T1nT2ni=(210)2i(1210)ni (1≤in, n≥1) (1↔2) T1nT22n+i=(0102)i(012)2n (i ≥0, n ≥1) (1↔2) T1nT2−2ni =(210)2n(2010)i (i ≥1, n≥0) (1↔2) T1niT2n=(1020)i(102)2n (i ≥0, n ≥1) (1↔2) T1n+iT2n=(201)2n(0201)i (i ≥1, n ≥0) (1↔2) T1nT2n=(0121)n (n≥1)

T1nT2n=(1210)n (n ≥0),

(3.1.1) where (1↔2) means that we consider the element obtained by exchangingT1andT2.

Similarly to the case of type A(1,1)1 , we use the following.

Lemma 3.2 Letwbe a minimal expression byw0, w1andw2.Then even if we attachto any letters ofw,the length of that does not decrease.

In each case we multiply Rk1Rl2 from the left, and examine their minimal length. For 1≤i <n, T1nT2n+i =(012)2i(0121)ni, by noting the expressions:



















012012=(R1R2) 012012 012012=R2012012 012012=(R1R2) 012012 012012=R2012012 012012=(R1R2) 012012 012012=R2012012









0121=(R1R2) 0121 0121=R20121 0121=(R1R2) 0121 0121=R10121,

we consider how manyR1,R2andR1R2can be contained in (012)2i(0121)niby attaching

∗to arbitrary letters. From the above, (012)2can contain 3×R1R2and 3×R2, and 0121

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can contain 2×R1R2,R1,R2, so by the relation, (012)2Rj =Rj(012)2(j =1,2), we see that (012)2i(0121)nican contain (n−iR1,(n+2i)×R2and (2n+iR1R2. Lemma 3.3 For1≤i <n

Rk1Rl2(R1R2)mT1nT2n+i

= Rk1Rl2(R1R2)m(012)2i(0121)ni

= (w10w11w12)· · ·(w2i,0w2i,1w2i,2)(w10 w11 w12 w11)

· · ·(wni,0wni,1wni,2wni,1)

wherewi j,andwi j=wj, wj(j=0,1,2)andwi1 =w1, w1, for any0≤kni,0≤ ln+2i,0≤m≤2n+i.

We count the number

R1kR2lT1nT2n+i,(1≤i<n,n≥2,k,l∈Z)l

R1kRl2T1nT2n+i

= l

T1nT2n+i =4n+2i .

For the purpose we use the following figure:

R2

R1

ni+1

n+2i+1

n+2i+1

2n+i+1

2n+i+1 ni+1

n+2i+1

then the number is equal to the number of the vertices of the lattices, where ni+1,n+2i+1, and 2n+i+1 are the number of vertices on each edge.

Then we use the following.

Lemma 3.4

a+1 b+1

c+1

c+1 a+1

b+1

In the left figure, the number of the vertices of the lattices is ab+bc+ca+a+b+c+1.

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(For example, the case ofa=1,b=2,c=3)

{all vertices} =1·2+2·3+3·1+1+2+3+1=18.

By multiplyingR±11, R±21,and (R1R2)±1,(R1 =w1w1,R2 =w2w2,R1R2 =w0w0), we obtain the elements whose length are 4n+2i+2, and actually we have only to multiply to the boundary in the figure, and iterating this procedure we get the following.

Lemma 3.5

R1mR2lT1nT2n+i, (1≤i <n, n≥2, m,l ∈Z)l

R1mR2lT1nT2n+i

=4n+2i+2k, (k≥1)

=8n+4i+6k. Proof:

a+2 b+2

c+2

c+2 b+2

a+1 c+1

b+1 a+2

The number of the vertices of the boundary of the outside is

2(a+1+b+1+c+1)=2(a+b+c)+6

={the boundary of the figure of the previous element} +6.

Next we consider the elementsT1nT2n+iw, forw=w1, w2, w1w2, w2w1,andw1w2w1, then we have the following:





















T1nT2n+i =(012)2i(0121)ni T1nT2n+i1=(012)2i(0121)ni1012 T1nT2n+i2=(012)2i(0121)ni−1021 T1nT2n+i12=(012)2i(0121)ni−101 T1nT2n+i21=(012)2i(0121)ni−102 T1nT2n+i121=(012)2i(0121)ni10.

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In the similar method to the case ofT1nT2n+i, in this case and for other cases we count how many R1±1,R±12 and (R1R2)±1 can be contained in a minimal expression. By the figure of the number of R1±1,R±12 and (R1R2)±1,we count the number of a minimal expression of the elements of the Weyl group and that of increasing length by 2, which is equal to (the boundary of the figure of the previous element)+6. In the sequal, we examine the number of the vertices on each edge of the figure in a minimal expression, first we have



















210210=R21210210 210210=(R1R2)−1210210 210210=R−12 210210 210210=(R1R2)1210210 210210=R−12 210210 210210=(R1R2)−1210210









1210=R−11 1210 1210=(R1R2)11210 1210=R−12 1210 1210 =(R1R2)−11210









0102=(R1R2) 0102 0102=R20102 0102=R−11 0102 0102=R20102









2010=R−12 2010 2010=R12010 2010=R212010 2010 =(R1R2)−12010









1020=R111020 1020=R21020 1020=R−11 1020 1020=(R1R2)11020



















102102=R1−1102102 102102=R2102102 102102=R11102102 102102=R2102102 102102=R1−1102102 102102 =R2102102

From these and (3.1.1), we obtain the following eight tables.

(I) Tn1Tn2+i=(012)2i(0121)ni (1i<n,n2)

(012)2i(0121)n−iw R1±1 R2±1 (R1R2)±1

(012)2i(0121)ni ni n+2i 2n+i

(012)2i(0121)ni1012 ni1 n+2i 2n+i (012)2i(0121)ni1021 ni n+2i1 2n+i (012)2i(0121)ni101 ni1 n+2i 2n+i1 (012)2i(0121)n−i−102 ni n+2i1 2n+i1 (012)2i(0121)ni10 ni1 n+2i1 2n+i1

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