Bourbaki

§ 4. Classification of root systems

1. Finite Coxeter groups

In this section, we are going to determine, up to isomorphism, all root systems, and consequently all crystallographic groups (§ 2, no. 5). More generally, we shall start by determining all finite groups generated by reflections in a finite-dimensional real vector space: this is equivalent (Chap. V, § 4, no. 8) to determining all finite Coxeter groups, or (Chap. V, § 4, no. 8, Th. 2) to determining all Coxeter matrices of finite order such that the associated bilinear form is positive and non-degenerate.

Let M=(mij)i,j∈IM = (m_{ij})_{i,j \in I} be a Coxeter matrix of finite order ll. Put

qij=−cos⁡(π/mij). q_{ij} = -\cos(\pi / m_{ij}).

Recall that qii=1q_{ii} = 1 and that qij=qjiq_{ij} = q_{ji} is zero or ≤−1/2\leq -1/2 for i≠ji \neq j. Put E=RlE = \mathbf{R}^l and let (ei)i∈I(e_i)_{i \in I} be the canonical basis of EE. Denote by (x∣y)(x|y) the bilinear form on EE associated to MM (Chap. V, § 4, no. 1) and qq the quadratic form x↦(x∣x)x \mapsto (x|x) on EE. For x=∑i∈Iξixix = \sum_{i \in I} \xi_i x_i,

∥x∥2=q(x)=∑i,j∈Iqijξiξj. \| x \| ^2 = q(x) = \sum_{i,j \in I} q_{ij} \xi_i \xi_j.

Denote by (X,f)(X, f) the Coxeter graph of MM (Chap. IV, § 1, no. 9). If aa is an edge of XX, f(a)f(a) is called the order of aa.

In the remainder of this number, the Coxeter group W(M)W(M) defined by MM (Chap. V, § 4, no. 3) is assumed to be finite, so that qq is positive and non-degenerate and XX is a forest (Chap. V, § 4, no. 8, Prop. 8). We also assume that XX is connected (in other words that the Coxeter group W(M)W(M) is irreducible), so that XX is a tree.

From the condition that qq is positive and non-degenerate, we shall obtain conditions on the mijm_{ij} that will enable us to list all the possibilities for the corresponding Coxeter graphs; it will only remain to show that these possibilities are actually realised, in other words that the corresponding groups W(M)W(M) are finite.

Lemma 1

For all ii, ∑j≠iqij2<1\sum_{j \neq i} q_{ij}^2 < 1.

Let JJ be the set of j∈Ij \in I such that qij≠0q_{ij} \neq 0, in other words such that {i,j}\{i, j\} is an edge of XX. If j,j′∈Jj, j' \in J and j≠j′j \neq j', {j,j′}\{j, j'\} is not an edge (otherwise i,j,j′i, j, j' would form a circuit), so (ej∣ej′)=0(e_j|e_{j'}) = 0. Let F=∑j∈JRejF = \sum_{j \in J} \mathbf{R} e_j. Then (ej)j∈J(e_j)_{j \in J} is an orthonormal basis of FF. The distance dd from eie_i to FF is given by d2=1−∑j∈J(ei∣ej)2=1−∑j∈Jqij2=1−∑j≠iqij2d^2 = 1 - \sum_{j \in J} (e_i|e_j)^2 = 1 - \sum_{j \in J} q_{ij}^2 = 1 - \sum_{j \neq i} q_{ij}^2, hence the lemma.

Lemma 2

Any vertex of XX belongs to at most 3 edges.

Indeed, if ii is linked to hh other vertices, the relations qij2≥14q_{ij}^2 \geq \frac{1}{4} for these other vertices implies that h4<1\frac{h}{4} < 1 by Lemma 1, so h≤3h \leq 3.

Lemma 3

If ii belongs to 3 edges, these edges are of order 3.

If not, we would have, in view of the relation cos⁡π4=22\cos \frac{\pi}{4} = \frac{\sqrt{2}}{2},

∑j≠iqij2≥14+14+(22)2=1 \sum_{j \neq i} q_{ij}^2 \geq \frac{1}{4} + \frac{1}{4} + (\frac{\sqrt{2}}{2})^2 = 1

which is impossible (Lemma 1).

Lemma 4

If there exists an edge of order ≥6\geq 6, then l=2l = 2.

Indeed, let {i,j}\{i, j\} be such an edge. If l>2l > 2, one of the edges i,ji, j (say ii) would be linked to a third vertex j′j', since XX is connected. In view of the relation cos⁡π6=32\cos \frac{\pi}{6} = \frac{\sqrt{3}}{2} we would have

∑k≠iqik2≥14+(32)2=1 \sum_{k \neq i} q_{ik}^2 \geq \frac{1}{4} + (\frac{\sqrt{3}}{2})^2 = 1

which is impossible (Lemma 1).

Lemma 5

A vertex cannot belong to two distinct edges of order ≥4\geq 4.

Let ii be such a vertex. We would have ∑j≠iqij2≥(22)2+(22)2=1\sum_{j \neq i} q_{ij}^2 \geq (\frac{\sqrt{2}}{2})^2 + (\frac{\sqrt{2}}{2})^2 = 1, which is impossible (Lemma 1).

Let {i,j}\{i, j\} be an edge of XX. We are going to define a new Coxeter graph, which will be obtained from the graph of MM by identifying ii and jj. The set I′I' of its vertices is the quotient of II obtained by identifying ii and jj. Put p={i,j}p = \{i, j\}, which is an element of I′I', and identify the elements of II distinct from ii and jj with their canonical images in I′I'. Let k,k′k, k' be two distinct elements of I′I'. Then, {k,k′}\{k, k'\} is an edge of the new graph in the following cases:

1) kk and k′k' are distinct from pp and {k,k′}\{k, k'\} is an edge of XX: in this case, the order of this edge is defined to be mkk′m_{kk'}:

2) k=pk = p, and one of the sets {i,k′},{j,k′}\{i, k'\}, \{j, k'\} is an edge of XX; the order of {p,k′}\{p, k'\} is defined to be mik′m_{ik'} if {i,k′}\{i, k'\} is an edge of XX, and mjk′m_{jk'} if {j,k′}\{j, k'\} is an edge of XX (these two possibilities are mutually exclusive because XX is a tree).

Let M′=(mij′)i,j∈I′M' = (m'_{ij})_{i,j \in I'} be the new Coxeter matrix thus defined, and put qij′=−cos⁡πmij′q'_{ij} = -\cos \frac{\pi}{m'_{ij}}. Then, for k≠pk \neq p, tpk′=qik+qjkt'_{pk} = q_{ik} + q_{jk}. Thus, if (ξi)∈RI′(\xi_i) \in \mathbf{R}^{I'},

∑k,k′∈I′qkk′′ξkξk′=∑k,k′∈Iqkk′ξkξk′+ξp2−ξi2−ξj2−2qijξiξj(1) \sum_{k, k' \in I'} q'_{kk'} \xi_k \xi_{k'} = \sum_{k, k' \in I} q_{kk'} \xi_k \xi_{k'} + \xi_p^2 - \xi_i^2 - \xi_j^2 - 2q_{ij} \xi_i \xi_j \tag{1}
=∑k,k′∈Iqkk′ξkξk′−(1+2qij)ξp2. = \sum_{k, k' \in I} q_{kk'} \xi_k \xi_{k'} - (1 + 2q_{ij}) \xi_p^2.

Lemma 6

If {i,j}\{i, j\} is of order 3, W(M′)W(M') is a finite Coxeter group.

Indeed, qij=−12q_{ij} = -\frac{1}{2}, so (1) becomes

∑k,k′∈I′qkk′′ξkξk′=∑k,k′∈Iqkk′ξkξk′ \sum_{k,k' \in I'} q'_{kk'} \xi_k \xi_{k'} = \sum_{k,k' \in I} q_{kk'} \xi_k \xi_{k'}

and (ξk)k∈I′↦∑k,k′∈I′qkk′′ξkξk′(\xi_k)_{k \in I'} \mapsto \sum_{k,k' \in I'} q'_{kk'} \xi_k \xi_{k'} is a positive non-degenerate quadratic form. It now suffices to apply Th. 2 of Chap. V. § 4, no. 8.

Lemma 7

We have one of the following:

a) X has a unique ramification point (Chap. IV, Appendix, no. 1). and all the edges of X are of order 3. b) X is a chain and has at most one edge of order ≥4\geq 4.

We argue by induction on l.

a) Assume that X has a ramification point i. Then i belongs to 3 edges of order 3. {i,k1},{i,k2},{i,k3}\{i, k_1\}, \{i, k_2\}, \{i, k_3\} (Lemmas 2 and 3). If l=4l = 4 the lemma is proved. If not, then k1k_1, say, belongs to an edge distinct from those just mentioned since X is connected. Identify i and k1k_1 in the Coxeter graph of M. This gives a new graph to which the induction hypothesis can be applied, in view of Lemma 6. Now the image pp of i is a ramification point of the new graph X′X'. Thus X′X' has no other ramification point and all its edges are of order 3. Thus all the edges of X are of order 3, and i and k1k_1 are its only possible ramification points. But if k1k_1 were a ramification point of X, pp would belong to at least 4 edges in X′X', contrary to Lemma 2.

b) Assume that X has no ramification point. Then X is a chain (Chap. IV, Appendix, no. 3, Prop. 3). Let {i,j}\{i, j\} be an edge of order ≥4\geq 4. If l=2l = 2, the lemma is trivial. If not, then i, say, belongs to an edge {i,k}\{i, k\} with k≠jk \neq j (since X is connected). This edge is of order 3 (Lemma 5). Identify i and k in the Coxeter graph of M. By Lemma 6, the induction hypothesis can be applied. Let pp be the image of i in the new graph X′X'. In X′X', {p,j}\{p, j\} is an edge of order ≥4\geq 4, so X′X' has no other edge of order ≥4\geq 4, and hence {i,j}\{i, j\} is the only edge of order ≥4\geq 4 in X.

Lemma 8

Let i1,i2,…,ipi_1, i_2, \ldots, i_p be vertices of X such that {i1,i2},{i2,i3},…,{ip−1,ip}\{i_1, i_2\}, \{i_2, i_3\}, \ldots, \{i_{p-1}, i_p\} are edges of order 3. Then q(∑r=1preir)=12p(p+1)q(\sum_{r=1}^p r e_{i_r}) = \frac{1}{2} p(p+1).

We have (eir∣eir)=1,(eir∣eir+1)=−12,(eir∣eis)=0(e_{i_r}|e_{i_r}) = 1, (e_{i_r}|e_{i_{r+1}}) = -\frac{1}{2}, (e_{i_r}|e_{i_s}) = 0 if s>r+1s > r + 1. Thus

q(∑r=1preir)=∑r=1pr2−2∑r=1p−112r(r+1)=p2−∑r=1p−1r. q(\sum_{r=1}^p r e_{i_r}) = \sum_{r=1}^p r^2 - 2 \sum_{r=1}^{p-1} \frac{1}{2} r(r+1) = p^2 - \sum_{r=1}^{p-1} r.

By Theory of Sets, Chap. III. § 5, no. 8. Cor. to Prop. 14, this is equal to

p2−12p(p−1)=12p(p+1). p^2 - \frac{1}{2} p(p-1) = \frac{1}{2} p(p+1).

Lemma 9

Assume that X is a chain with vertices 1, 2, ..., l and edges {1, 2}, {2, 3}, ..., {l - 1, l}.

(i) If one of the edges {2, 3}, {3, 4}, ..., {l - 2, l - 1} is of order ≥4\geq 4, this edge is of order 4 and the graph is the following:

!Graph with 4 nodes connected in a chain

(ii) If the edge {1, 2} is of order 5, the graph is one of the following:

!Graphs with 5 nodes connected in chains

We can assume that l>2l > 2 (Lemma 4). Assume that {i,i+1}\{i, i + 1\} is of order ≥4\geq 4, with 1≤i≤l−11 \leq i \leq l - 1. Put

x=e1+2e2+⋯+iei, y=ei+2el−1+⋯+(l−i)ei+1, and j=l−i. x = e_1 + 2e_2 + \cdots + ie_i,\ y = e_i + 2e_{l-1} + \cdots + (l - i)e_{i+1}, \text{ and } j = l - i.

By Lemma 8, ∥x∥2=12i(i+1)\| x \| ^2 = \frac{1}{2} i(i + 1), ∥y∥2=12j(j+1)\| y \| ^2 = \frac{1}{2} j(j + 1). On the other hand, (x∣y)=ij(ei∣ei+1)=−ijcos⁡πm(x|y) = ij(e_i|e_{i+1}) = -ij \cos \frac{\pi}{m} with m=4m = 4 or 5 (Lemma 4). Now

(x∣y)2<∥x∥2∥y∥2. (x|y)^2 < \| x \| ^2 \| y \| ^2.

which gives

14ij(i+1)(j+1)>i2j2cos⁡2πm \frac{1}{4} ij(i + 1)(j + 1) > i^2 j^2 \cos^2 \frac{\pi}{m}

so

(i+1)(j+1)>4ijcos⁡2πm≥2ij. (i + 1)(j + 1) > 4ij \cos^2 \frac{\pi}{m} \geq 2ij.

This gives, first of all, ij−i−j−1<0ij - i - j - 1 < 0, or (i−1)(j−1)<2(i - 1)(j - 1) < 2. If

1<i<l−1, 1 < i < l - 1,

then 1<j<l−11 < j < l - 1, so i=j=2i = j = 2, and so 1^1

9>16cos⁡2πm, thus cos⁡2πm<cos⁡2π5 9 > 16 \cos^2 \frac{\pi}{m}, \text{ thus } \cos^2 \frac{\pi}{m} < \cos^2 \frac{\pi}{5}

and hence m=4m = 4. This proves (i). If i=1i = 1 and m=5m = 5, then 2j+2>4j3+582j + 2 > 4j \frac{3+\sqrt{5}}{8}, or j5−12<2,j<5+1<4j \frac{\sqrt{5}-1}{2} < 2, j < \sqrt{5} + 1 < 4, and so l=j+1≤4l = j + 1 \leq 4. This proves (ii).

1^1 The 5th roots of 1 distinct from 1 are the solutions of z4+z3+z2+z+1=0z^4 + z^3 + z^2 + z + 1 = 0. Putting x=12(z+1z)x = \frac{1}{2}(z + \frac{1}{z}), this equation becomes (2x)2−2+2x+1=0(2x)^2 - 2 + 2x + 1 = 0, or 4x2+2x−1=04x^2 + 2x - 1 = 0, so x=−1±54x = \frac{-1 \pm \sqrt{5}}{4}. Hence,

2cos⁡2π5−1=cos⁡2π5=5−14,cos⁡4π5=3+58>58>916,cos⁡π5=1+54. 2 \cos^2 \frac{\pi}{5} - 1 = \cos \frac{2\pi}{5} = \frac{\sqrt{5} - 1}{4}, \quad \cos^4 \frac{\pi}{5} = \frac{3 + \sqrt{5}}{8} > \frac{5}{8} > \frac{9}{16}, \quad \cos \frac{\pi}{5} = \frac{1 + \sqrt{5}}{4}.

Lemma 10

If X has a ramification point i, the full subgraph X - {i} is the union of three chains, and if p - 1, q - 1, r - 1 are the lengths of these chains, the triple {p, q, r} is equal, up to a permutation, to one of the triples {1, 2, 2}, {1, 2, 3}, {1, 2, 4}, {1, 1, m} (for some m ≥1\geq 1).

The vertex i belongs to 3 edges (Lemma 2), and there is no other ramification point (Lemma 7), so the full subgraph X - {i} is the sum of 3 chains X_1, X_2, X_3, each of which has a terminal vertex linked to i in X. Let {i_1, i_2}, {i_2, i_3}, ..., {i_{p-1}, i_p} be the edges of X_1, {j_1, j_2}, {j_2, j_3}, ..., {j_{q-1}, j_q} those of X_2, and {k_1, k_2}, {k_2, k_3}, ..., {k_{r-1}, k_r} those of X_3, with i_1, j_1, k_1 linked to i in X. We can assume that p≥q≥r≥1p \geq q \geq r \geq 1. Put

x=eip+2eip−1+⋯+pei1 x = e_{i_p} + 2e_{i_{p-1}} + \cdots + pe_{i_1}
y=ejq+2ejq−1+⋯+qej1 y = e_{j_q} + 2e_{j_{q-1}} + \cdots + qe_{j_1}
z=ekr+2ekr−1+⋯+rek1. z = e_{k_r} + 2e_{k_{r-1}} + \cdots + re_{k_1}.

Since all the edges of X are of order 3 (Lemma 7), Lemma 8 gives ∥x∥2=12p(p+1)\| x \| ^2 = \frac{1}{2} p(p+1), ∥y∥2=12q(q+1)\| y \| ^2 = \frac{1}{2} q(q+1), ∥z∥2=12r(r+1)\| z \| ^2 = \frac{1}{2} r(r+1). On the other hand, eie_i is orthogonal to ei2,ei3,…,eipe_{i_2}, e_{i_3}, \ldots, e_{i_p}, so (ei∣x)=p(ei∣ei1)=−12p(e_i | x) = p(e_i | e_{i_1}) = -\frac{1}{2} p; similarly (ei∣y)=−12q(e_i | y) = -\frac{1}{2} q, (ei∣z)=−12r(e_i | z) = -\frac{1}{2} r. The unit vectors ∥x∥−1x,∥y∥−1y,∥z∥−1z\| x \|^{-1} x, \| y \|^{-1} y, \| z \|^{-1} z are mutually orthogonal, and eie_i does not belong to the subspace F that they generate; the square of the distance from eie_i to F is

1−(ei∣x∥x∥)2−(ei∣y∥y∥)2−(ei∣z∥z∥)2 1 - (e_i | \frac{x}{\| x \|})^2 - (e_i | \frac{y}{\| y \|})^2 - (e_i | \frac{z}{\| z \|})^2
=1−12pp+1−12qq+1−12rr+1 = 1 - \frac{1}{2} \frac{p}{p+1} - \frac{1}{2} \frac{q}{q+1} - \frac{1}{2} \frac{r}{r+1}
=1−12+121p+1−12+121q+1−12+121r+1. = 1 - \frac{1}{2} + \frac{1}{2} \frac{1}{p+1} - \frac{1}{2} + \frac{1}{2} \frac{1}{q+1} - \frac{1}{2} + \frac{1}{2} \frac{1}{r+1}.

Since this quantity is > 0, we have

(p+1)−1+(q+1)−1+(r+1)−1>1. (p+1)^{-1} + (q+1)^{-1} + (r+1)^{-1} > 1.
(4)

Hence 3(r+1)−1>13(r+1)^{-1} > 1, so r<2r < 2 and finally r=1r = 1. Then (4) gives

(p+1)−1+(q+1)−1>12 (p+1)^{-1} + (q+1)^{-1} > \frac{1}{2}
(5)

hence 2(q+1)−1>122(q+1)^{-1} > \frac{1}{2}, so q≤2q \leq 2. Finally, if q=2q = 2, (5) gives

(p+1)−1>16.hence p≤4. (p+1)^{-1} > \frac{1}{6}. \quad \text{hence } p \leq 4.

Theorem 1

The graph of any irreducible finite Coxeter system (W, S) is isomorphic to one of the following:

A_l (l \geq 1\ vertices) B_l (l \geq 2\ vertices) D_l (l \geq 4\ vertices) E_6 E_7 E_8 F_4 4 G_2 6 H_3 5 H_4 5 I_2(p) p (p = 5\ or\ p \geq 7).

No two of these graphs are isomorphic.

Indeed, let W = (m_{ij}) be the Coxeter matrix of (W, S), and let l = Card(S). If one of the m_{ij} is \geq 6, then l = 2 (Lemma 4) and the Coxeter graph of (W, S) is of type G_2 or I_2(p) with p \geq 7. Assume now that all the m_{ij} \leq 5.

a) If the m_{ij} are not all equal to 3, the graph X of (W, S) is a chain and exactly one of the m_{ij} is equal to 4 or 5 (Lemma 7). If one of the m_{ij} is equal to 5, Lemma 9 shows that we have one of the types H_3, H_4 or I_2(5). If one of the m_{ij} is equal to 4, Lemma 9 shows that we have one of the types B_l or F_4.

b) Assume now that all the m_{ij} are equal to 3. If X is a chain, the Coxeter graph is of type A_l. If not, Lemma 10 shows that it is of type E_6, E_7, E_8 or D_l.

The fact that no two of the Coxeter graphs listed are isomorphic is clear.

Conversely:

Theorem 2

The Coxeter groups defined by the Coxeter graphs A_l, B_l, ..., I_2(p) of Th. 1 are finite.

This is clear for I_2(p), the corresponding group being the dihedral group of order 2p (Chap. IV, § 1, no. 9). For H_4 the corresponding quadratic form is

ξ12+ξ22+ξ32+ξ42−ξ1ξ2−ξ2ξ3−2(cos⁡π5)ξ3ξ4 \xi_1^2 + \xi_2^2 + \xi_3^2 + \xi_4^2 - \xi_1 \xi_2 - \xi_2 \xi_3 - 2(\cos \frac{\pi}{5}) \xi_3 \xi_4
=ξ12+ξ22+ξ32+ξ42−ξ1ξ2−ξ2ξ3−1+52ξ3ξ4 = \xi_1^2 + \xi_2^2 + \xi_3^2 + \xi_4^2 - \xi_1 \xi_2 - \xi_2 \xi_3 - \frac{1 + \sqrt{5}}{2} \xi_3 \xi_4
=(ξ2−ξ1+ξ32)2+(ξ4−1+54ξ3)2+34(ξ1−13ξ3)2+7−3524ξ32. = (\xi_2 - \frac{\xi_1 + \xi_3}{2})^2 + (\xi_4 - \frac{1 + \sqrt{5}}{4} \xi_3)^2 + \frac{3}{4} (\xi_1 - \frac{1}{3} \xi_3)^2 + \frac{7 - 3 \sqrt{5}}{24} \xi_3^2.

Since 7−357 - 3 \sqrt{5} is >0> 0, this form is positive non-degenerate, and the corresponding Coxeter group is finite. The same holds for that corresponding to H3H_3, since it is isomorphic to a subgroup of the preceding (Chap. IV, § 1, no. 8).

For the types Al,Bl,…,G2A_l, B_l, \ldots, G_2, we shall construct, in Nos. 5 to 13, root systems having the corresponding groups as Weyl groups. We shall see that these groups are not only finite, but crystallographic (§ 2, no. 5).

2. Dynkin graphs

By abuse of language, we shall call a normed graph a pair (Γ,f)(\Gamma, f) having the following properties:

1) Γ\Gamma is a graph (called the underlying graph of (Γ,f)(\Gamma, f)).

2) If EE denotes the set of pairs (i,j)(i, j) such that {i,j}\{i, j\} is an edge of Γ\Gamma, ff is a map from EE to R\mathbf{R} such that f(i,j)f(j,i)=1f(i, j) f(j, i) = 1 for all (i,j)∈E(i, j) \in E.

There is an obvious notion of isomorphism of normed graphs.

Let RR be a reduced root system in a real vector space VV. We are going to associate to it a normed graph (X,f)(X, f), called the Dynkin graph of RR. The vertices of XX will be the elements of the set II of orbits of W(R)W(R) in the union of the sets {B}×B\{B\} \times B (where BB is the set of bases of RR). If N=(nij)i,j∈IN = (n_{ij})_{i,j \in I} (resp. M=(mij)i,j∈IM = (m_{ij})_{i,j \in I}) is the canonical Cartan matrix (resp. the Coxeter matrix) of RR (§ 1, no. 5, Remark 7), two vertices ii and jj of XX are linked if and only if nij≠0n_{ij} \neq 0 and we then put

f(i,j)=nijnji. f(i, j) = \frac{n_{ij}}{n_{ji}}.
Since nij=0n_{ij} = 0 implies nji=0n_{ji} = 0, this defines a normed graph (X,f)(X, f).

Let (x∣y)(x|y) be a scalar product on VV, invariant under W(R)W(R), and let B=(αi)i∈IB = (\alpha_i)_{i \in I} be a basis of RR, indexed canonically. Formulas (7) and (9) of § 1, no. 1 show that vertices ii and jj of the graph XX are linked if and only if

(αi∣αj)≠0 (\alpha_i|\alpha_j) \neq 0
and that
f(i,j)=(αi∣αi)(αj∣αj). f(i, j) = \frac{(\alpha_i|\alpha_i)}{(\alpha_j|\alpha_j)}.

In view of the results of § 1, Nos. 3 and 5, the only possibilities are the following, up to interchanging ii and jj:

1) ii and jj are not linked; nij=nji=0;mij=2;n_{ij} = n_{ji} = 0; m_{ij} = 2; 2) f(i,j)=f(j,i)=1;nij=nji=−1;mij=3;f(i, j) = f(j, i) = 1; n_{ij} = n_{ji} = -1; m_{ij} = 3; 3) f(i,j)=2,f(j,i)=1/2;nij=−2,nji=−1;mij=4;f(i, j) = 2, f(j, i) = 1/2; n_{ij} = -2, n_{ji} = -1; m_{ij} = 4; 4) f(i,j)=3,f(j,i)=1/3;nij=−3,nji=−1;mij=6.f(i, j) = 3, f(j, i) = 1/3; n_{ij} = -3, n_{ji} = -1; m_{ij} = 6.

We see from this that the Dynkin graph RR determines the Cartan matrix and the Coxeter matrix of RR, and hence determines RR up to isomorphism. More precisely, the Cor. of Prop. 15 of § 1, no. 5 implies the following result:

Proposition 1

Let R1R_1 and R2R_2 be two reduced root systems in vector spaces V1V_1 and V2V_2. Let B1=(αi)i∈I1B_1 = (\alpha_i)_{i \in I_1} and B2=(αi)i∈I2B_2 = (\alpha_i)_{i \in I_2} be bases of R1R_1 and R2R_2, indexed canonically. Let λ\lambda be an isomorphism from the Dynkin graph of R1R_1 to the Dynkin graph of R2R_2. Then, there exists a unique isomorphism from V1V_1 to V2V_2 transforming R1R_1 into R2R_2 and αi\alpha_i into αλ(i)\alpha_{\lambda(i)} for all i∈I1i \in I_1.

It is clear that an automorphism of RR defines an automorphism of the Dynkin graph of RR, and hence a homomorphism φ\varphi from the group A(R)A(R) to the group of automorphisms of the Dynkin graph of RR.

Corollary

The homomorphism φ\varphi defines by passage to the quotient an isomorphism from the group A(R)/W(R)A(R)/W(R) to the group of automorphisms of the Dynkin graph of RR.

Clearly, φ(g)=Id\varphi(g) = \mathrm{Id} for all g∈W(R)g \in W(R). On the other hand, Prop. 1 shows that there exists an isomorphism ψ\psi from the group of isomorphisms of the Dynkin graph of RR to the subgroup EE of elements of A(R)A(R) leaving fixed a given basis BB of RR, such that φ∘ψ=Id\varphi \circ \psi = \mathrm{Id}. Since A(R)A(R) is the semi-direct product of EE and W(R)W(R) (§ 1, no. 5, Prop. 16), the corollary follows.

In practice, the Dynkin graph (X,f)(X, f) is represented by a diagram composed of nodes and bonds in the following way. The nodes correspond to the vertices of XX; two nodes corresponding to two distinct vertices ii and jj are joined by 0, 1, 2 or 3 bonds in cases 1), 2), 3) and 4) above (up to interchanging ii and jj). Moreover, in cases 3) and 4), that is when f(i,j)>1f(i, j) > 1, or when the roots αi\alpha_i and αj\alpha_j are not orthogonal and not of the same length, an inequality sign >> is placed on the double or triple bond joining the nodes corresponding to ii and jj oriented towards the node corresponding to jj (that is, the shortest root):

∘⟹∘(for f(i,j)=2).∘⇛∘(for f(i,j)=3). \begin{array}{cc} \circ \Longrightarrow \circ & \text{(for } f(i, j) = 2 \text{).} \\ \circ \Rrightarrow \circ & \text{(for } f(i, j) = 3 \text{).} \end{array}

It is clear that the Dynkin graph (X,f)(X, f) can be recovered from this diagram.

We remark that the diagram associated to the Coxeter graph of W(R)W(R) can be obtained from that associated to the Dynkin graph of RR by keeping the nodes and the single bonds and replacing the double (resp. triple) bonds by a bond surmounted by the number 4 (resp. 6). Conversely, given the Coxeter graph of W(R), the diagram associated to the Dynkin graph of R can be recovered using the inverse of this procedure, except for the inequality signs on the double or triple bonds. Th. 1 thus gives immediately the list of possible Dynkin graphs. More precisely:

Theorem 3

If R is an irreducible reduced root system, its Dynkin graph is isomorphic to one of the graphs represented by the following diagrams:

Al∘−⋯−∘(l≥1 vertices )Bl∘−⋯−∘−∘(l≥2 vertices )Cl∘−⋯−∘−∘(l≥3 vertices )Dl∘−⋯−∘−∘−∘(l≥4 vertices )E6∘−⋯−∘E7∘−⋯−∘−∘−∘E8∘−⋯−∘−∘−∘−∘F4∘−∘−∘−∘G2∘−∘−∘ \begin{array}{ll} A_l & \circ-\cdots-\circ \quad (l \geq 1 \text{ vertices }) \\ B_l & \circ-\cdots-\circ-\circ \quad (l \geq 2 \text{ vertices }) \\ C_l & \circ-\cdots-\circ-\circ \quad (l \geq 3 \text{ vertices }) \\ D_l & \circ-\cdots-\circ-\circ-\circ \quad (l \geq 4 \text{ vertices }) \\ E_6 & \circ-\cdots-\circ \\ E_7 & \circ-\cdots-\circ-\circ-\circ \\ E_8 & \circ-\cdots-\circ-\circ-\circ-\circ \\ F_4 & \circ-\circ-\circ-\circ \\ G_2 & \circ-\circ-\circ \end{array}

No two of these graphs are isomorphic and there are irreducible reduced root systems having each of them as their Dynkin graph (up to isomorphism).

The first assertion follows immediately from Th. 1, in view of the preceding remarks, the fact that the Coxeter groups of the graphs H_3, H_4 and I_2(p) (for p = 5 and p \geq 7) are not crystallographic, and the fact that the two possible inequalities for the double (resp. triple) bond of the Dynkin graph associated to the Coxeter graph F_4 (resp. G_2) give isomorphic Dynkin graphs. The second assertion is clear and the third will follow from the explicit construction of an irreducible reduced root system for each type, a construction that will be carried out in Nos. 5 to 13.

Remark 1

The graph A_1 reduces to a single node; we denote it also by B_1 or C_1. The graph B_2 \circ-\circ-\circ-\circ is also denoted by C_2. The graph A_3 \circ-\cdots-\circ is also denoted by D_3. Finally, D_2 denotes the graph consisting of two unconnected nodes. (These conventions are derived from the properties of the corresponding root systems, cf. nos. 5 to 8.)

Remark 2

If (X, f) is the Dynkin graph of a reduced root system R, the Dynkin graph of the inverse system can be identified with (X, f^{-1}). In other words, the diagram associated to the Dynkin graph of R^- can be obtained from that associated to the Dynkin graph of R by reversing the inequality signs. If R is irreducible, we see that R is isomorphic to R^- unless R is of type B_l or C_l, in which case R^- is of type C_l or B_l.

3. Affine Weyl group and completed Dynkin graph

Let R be an irreducible reduced root system and let (X, f) be its Dynkin graph. We are going to define another normed graph (\tilde{X}, \tilde{f}) that we shall call the completed Dynkin graph of R. The set \tilde{I} of vertices of \tilde{X} consists of the set I of vertices of X and a vertex denoted by 0, not belonging to I. To define \tilde{f}, choose a basis B = (\alpha_i)_{i \in I} of R and a scalar product \langle x | y \rangle invariant under W(R). Let \alpha_0 be the negative of the highest root for the order defined by B. Two distinct vertices i, j \in \tilde{I} are linked if and only if \langle \alpha_i | \alpha_j \rangle \neq 0 and we then put

f~(i,j)=⟨αi∣αi⟩⟨αj∣αj⟩. \tilde{f}(i, j) = \frac{\langle \alpha_i | \alpha_i \rangle}{\langle \alpha_j | \alpha_j \rangle}.

It is immediate that the graph \tilde{X} and the map \tilde{f} thus defined do not depend on the choice of B or the scalar product.

If the rank l of R is equal to 1, then I = \{i\} and \alpha_0 = -\alpha_1; hence \tilde{f}(0, i) = 1. If l \geq 2, \alpha_0 is not proportional to any of the \alpha_i and \langle \alpha_0 | \alpha_i \rangle is \leq 0 (§ 1, no. 8, Prop. 25). For any pair (i, j) of distinct elements of \tilde{I}, the only possibilities are those denoted by 1), 2), 3), 4) in the preceding number (putting, for example, n_{0i} = n(\alpha_0, \alpha_i) and m_{0i} = order of s_{\alpha_0} s_{\alpha_i} for all i \in I).

In the case l \geq 2, the completed Dynkin graph is represented by a diagram with the same conventions as in the preceding number, sometimes indicating by dotted lines the bonds joining the vertex 0 to the other vertices. We remark that the inequality sign > on such a bond, if it exists, is always directed towards the vertex distinct from 0, since \alpha_0 is a longest root (§ 1, no. 8, Prop. 25). The graph (X, f) is the subgraph obtained from (\tilde{X}, \tilde{f}) by deleting the vertex 0.

The action of A(R) on (X, f) extends to an action on (\tilde{X}, \tilde{f}), leaving 0 fixed, and W(R) acts trivially on (\tilde{X}, \tilde{f}).

We retain the notations of § 2, Prop. 5 of § 2, no. 2, together with Th. 1 of Chap. V, § 3, no. 2, shows that the Coxeter graph \Sigma of the affine Weyl group W_a(R) can be obtained from (\tilde{X}, \tilde{f}) by the same rules by which the Coxeter graph of W(R) is obtained from (X, f). On the other hand, let G be the normaliser of W_a(R) (§ 2, no. 3). To any g \in G corresponds an automorphism \varphi(g) of \Sigma and \varphi(g) = \mathrm{Id} if g \in W_a(R). Conversely, given an automorphism \lambda of \Sigma there is, by Prop. 11 of Chap. V, § 4, no. 9, a unique element g = \psi(\lambda) preserving a given alcove C and such that \varphi(g) = \lambda. Since G is the semi-direct product of the subgroup G_C of elements preserving C and W_a(R) (§ 2, no. 3), we deduce that \varphi defines by passage to the quotient an isomorphism from G/W_a (or from G_C) to Aut(\Sigma). It is immediate that the composite of this isomorphism with the canonical map from A(R)/W(R) to G/W_a coincides with the homomorphism from A(R)/W(R) to Aut(\Sigma) induced by the homomorphism from A(R)/W(R) to Aut(\tilde{X}, \tilde{f}) defined above. By § 2, no. 3, the group Aut(\Sigma) is isomorphic to the semi-direct product of

A(R)/W(R) by P(R^*)/Q(R^*). and P(R^*)/Q(R^*) is isomorphic to the group IC=GC∩Wa′I_C = G_C \cap W'_a (with the notation of § 2, no. 3): the element of Aut(Σ\Sigma) corresponding to the element γi\gamma_i of ICI_C transforms the vertex 0 to the vertex ii of Σ\Sigma.

Remark

It can be shown that the canonical map

Aut⁡(X~,f~)→Aut⁡(Σ) \operatorname{Aut}(\tilde{X}, \tilde{f}) \to \operatorname{Aut}(\Sigma)
is an isomorphism.

Theorem 4

Let (W, S) be an irreducible Coxeter system with S finite. The associated quadratic form (Chap. V, § 4, no. 1) is positive and degenerate if and only if the Coxeter graph of (W, S) is isomorphic to one of the following:

A~1∘⟶∞A~l(l≥2)∘⟶⋯⟶∘(circuit with l+1 vertices)B~2∘⟶4⟶∘B~l(l≥3)∘⟶⋯⟶∘⟶4(l + 1 vertices)C~l(l≥3)∘⟶4⟶⋯⟶4(l + 1 vertices)D~l(l≥4)∘⟶⋯⟶∘(l + 1 vertices)E~6∘⟶∘⟶∘⟶∘E~7∘⟶∘⟶∘⟶∘⟶∘E~8∘⟶∘⟶∘⟶∘⟶∘⟶∘F~4∘⟶∘⟶4⟶∘G~2∘⟶6⟶∘ \begin{array}{ll} \tilde{A}_1 & \circ \longrightarrow \infty \\ \tilde{A}_l \quad (l \geq 2) & \circ \longrightarrow \cdots \longrightarrow \circ \quad \text{(circuit with } l + 1 \text{ vertices)} \\ \tilde{B}_2 & \circ \longrightarrow 4 \longrightarrow \circ \\ \tilde{B}_l \quad (l \geq 3) & \circ \longrightarrow \cdots \longrightarrow \circ \longrightarrow 4 \quad \text{(l + 1 vertices)} \\ \tilde{C}_l \quad (l \geq 3) & \circ \longrightarrow 4 \longrightarrow \cdots \longrightarrow 4 \quad \text{(l + 1 vertices)} \\ \tilde{D}_l \quad (l \geq 4) & \circ \longrightarrow \cdots \longrightarrow \circ \quad \text{(l + 1 vertices)} \\ \tilde{E}_6 & \circ \longrightarrow \circ \longrightarrow \circ \longrightarrow \circ \\ \tilde{E}_7 & \circ \longrightarrow \circ \longrightarrow \circ \longrightarrow \circ \longrightarrow \circ \\ \tilde{E}_8 & \circ \longrightarrow \circ \longrightarrow \circ \longrightarrow \circ \longrightarrow \circ \longrightarrow \circ \\ \tilde{F}_4 & \circ \longrightarrow \circ \longrightarrow 4 \longrightarrow \circ \\ \tilde{G}_2 & \circ \longrightarrow 6 \longrightarrow \circ \end{array}

No two of these Coxeter graphs are isomorphic.

By Chap. V, § 4, no. 9 and Prop. 8 of § 2, no. 5, the Coxeter systems whose quadratic form is positive and degenerate are those which correspond to the affine Weyl groups of irreducible reduced root systems. The theorem therefore follows from the determination of the completed Dynkin graphs made in nos. 5 to 13 below.

4. Preliminaries to the construction of root systems

Let V be a real vector space of dimension l≥1l \geq 1 equipped with a scalar product (x∣y)(x|y), L a discrete subgroup of V, Λ\Lambda a finite set of numbers > 0, and R the set of α∈L\alpha \in L such that (α∣α)∈Λ(\alpha|\alpha) \in \Lambda. Assume that R generates V and that, for any pair (α,β)(\alpha, \beta) of points of R, the number 2(α∣β)(α∣α)2 \frac{(\alpha|\beta)}{(\alpha|\alpha)} is an integer. Then, R is a root system in V. Indeed, R clearly satisfies (RS_I). Let α∈R\alpha \in R; let sαs_{\alpha} be the orthogonal reflection x↦x−2(x∣α)(α∣α)αx \mapsto x - 2 \frac{(x|\alpha)}{(\alpha|\alpha)} \alpha: then, if β∈R\beta \in R, we have 2(β∣α)(α∣α)∈Z2 \frac{(\beta|\alpha)}{(\alpha|\alpha)} \in \mathbf{Z}, so sα(β)∈Ls_{\alpha}(\beta) \in L, and moreover ∥sα(β)∥=∥β∥\| s_{\alpha}(\beta) \| = \| \beta \|, so sα(β)∈Rs_{\alpha}(\beta) \in R; thus, R satisfies (RS_{II}) and (RS_{III}), and is reduced if Λ\Lambda does not contain two numbers of the form λ\lambda and 4λ4\lambda.

Now let V be a subspace of E=RnE = \mathbf{R}^n. Let (ε1,…,εn)(\varepsilon_1, \ldots, \varepsilon_n) be the canonical basis of E; we equip E with the scalar product for which this basis is orthonormal and identify E∗E^* with E (resp. V∗V^* with V) by means of this scalar product. We define subgroups L0,L1,L2,L3L_0, L_1, L_2, L_3 of E as follows:

1) L0L_0 is the Z\mathbf{Z}-module with basis (εi)(\varepsilon_i). We have (α∣β)∈Z(\alpha|\beta) \in \mathbf{Z} for all α,β∈L0\alpha, \beta \in L_0. The vectors α∈L0\alpha \in L_0 for which (α∣α)=1(\alpha|\alpha) = 1 are the ±εi\pm \varepsilon_i (1≤i≤n1 \leq i \leq n); those for which (α∣α)=2(\alpha|\alpha) = 2 are the ±εi±εj\pm \varepsilon_i \pm \varepsilon_j for i<ji < j (the two signs ±\pm, in ±εi±εj\pm \varepsilon_i \pm \varepsilon_j, are chosen independently of each other; we adopt an analogous convention throughout the remainder of this section).

2) L1L_1 is the Z\mathbf{Z}-submodule of L0L_0 consisting of the x=∑i=1nξiεi∈L0x = \sum_{i=1}^n \xi_i \varepsilon_i \in L_0 such that ∑i=1nξi\sum_{i=1}^n \xi_i is even; since ξi\xi_i and ξi2\xi_i^2 have the same parity, this is equivalent to requiring that (x∣x)(x|x) is even. Let L1′L_1' be the submodule of L1L_1 generated by the εi±εj\varepsilon_i \pm \varepsilon_j; we have ∑i=1nξiεi≡(∑i=1nξi)εn(modL1′)\sum_{i=1}^n \xi_i \varepsilon_i \equiv (\sum_{i=1}^n \xi_i) \varepsilon_n \pmod{L_1'}, and since 2εn=(ε1+εn)−(ε1−εn)∈L1′2\varepsilon_n = (\varepsilon_1 + \varepsilon_n) - (\varepsilon_1 - \varepsilon_n) \in L_1', it follows that L1′=L1L_1' = L_1. Since L0L_0 is generated by L1L_1 and ε1\varepsilon_1, L0/L1L_0/L_1 is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z}.

3) L2=L0+Z(12∑i=1nεi)L_2 = L_0 + \mathbf{Z}(\frac{1}{2} \sum_{i=1}^n \varepsilon_i). It is clear that an element x=∑i=1nξiεix = \sum_{i=1}^n \xi_i \varepsilon_i of V is in L2L_2 if and only if

2ξi∈Z,ξi−ξj∈Z for all i and j. 2\xi_i \in \mathbf{Z}, \quad \xi_i - \xi_j \in \mathbf{Z} \text{ for all } i \text{ and } j.
Since (εk∣12∑i=1nεi)=12(\varepsilon_k | \frac{1}{2} \sum_{i=1}^n \varepsilon_i ) = \frac{1}{2} for all kk, and since ∥12∑i=1nεi∥2=n4\| \frac{1}{2} \sum_{i=1}^n \varepsilon_i \| ^2 = \frac{n}{4}, we have (α∣β)∈12Z(\alpha|\beta) \in \frac{1}{2}\mathbf{Z} for α,β∈L2\alpha, \beta \in L_2 if nn is even. The group L2/L0L_2/L_0 is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z}.

4) L3=L1+Z(12∑i=1nεi)L_3 = L_1 + \mathbf{Z} (\frac{1}{2} \sum_{i=1}^n \varepsilon_i ). If nn is a multiple of 4, L3L_3 is the set of ∑i=1nξiεi\sum_{i=1}^n \xi_i \varepsilon_i satisfying (6) and the condition ∑i=1nξi∈2Z\sum_{i=1}^n \xi_i \in 2\mathbf{Z}: in this case, (α∣β)∈Z(\alpha|\beta) \in \mathbf{Z} for all α,β∈L3\alpha, \beta \in L_3.

It is immediate that the subgroup of E associated to L0L_0 (resp. L1,L2L_1, L_2) is L0L_0 (resp. L2,L1L_2, L_1). The subgroup of E associated to L3L_3 is the set of

x:=∑i=1nξiεi∈L2 x := \sum_{i=1}^n \xi_i \varepsilon_i \in L_2

such that (x∣12∑i=1nεi)∈Z(x| \frac{1}{2} \sum_{i=1}^n \varepsilon_i ) \in \mathbf{Z}, that is, such that ∑i=1nξi∈2Z\sum_{i=1}^n \xi_i \in 2\mathbf{Z}: if n≡0(mod4)n \equiv 0 \pmod{4}, this associated subgroup is therefore L3L_3.

The abelian group L2/L1L_2/L_1 is of order 4, and hence is isomorphic to Z/4Z\mathbf{Z}/4\mathbf{Z} or Z/2Z×Z/2Z\mathbf{Z}/2\mathbf{Z} \times \mathbf{Z}/2\mathbf{Z} (Algebra, Chap. VII, § 4, no. 6, Th. 3). If nn is odd,

p(12∑i=1nεi)∈L1⇔p≡0(mod4) p(\frac{1}{2} \sum_{i=1}^n \varepsilon_i ) \in L_1 \Leftrightarrow p \equiv 0 \pmod{4}

so L2/L1L_2/L_1 is cyclic of order 4. If nn is even,

p(12∑i=1nεi)∈L1⇔p≡0(mod2) p(\frac{1}{2} \sum_{i=1}^n \varepsilon_i ) \in L_1 \Leftrightarrow p \equiv 0 \pmod{2}

so L2/L1L_2/L_1, which contains two distinct elements of order 2, is isomorphic to Z/2Z×Z/2Z\mathbf{Z}/2\mathbf{Z} \times \mathbf{Z}/2\mathbf{Z}.

We shall use this notation throughout the next nine nos. and in the plates. For each type of Dynkin graph in Th. 3, we shall describe explicitly:

(I) A root system R and the number of roots. (II) A basis B of R, and the corresponding positive roots. The basis B will be indexed by the integers 1, ..., l. (III) The Coxeter number h (§ 1, no. 11). (IV) The highest root α~\tilde{\alpha} (for the order defined by B) and the completed Dynkin graph (no. 3). We shall indicate next to each vertex the corresponding root of B. (V) The inverse system R−R^-, the canonical bilinear form and the constant γ(R)\gamma(R) (§ 1, no. 12). (VI) The fundamental weights relative to B (§ 1, no. 10). (VII) The sum of the positive roots. (VIII) The groups P(R), Q(R), P(R)/Q(R) and the connection index (§ 1, no. 9). (IX) The exponents of W(R) (Chap. V, § 6, no. 2, Def. 2). In the cases A_l, B_l, C_l and D_l we determine the symmetric invariants. (X) The order of W(R) (and in some cases its structure).

(XI) The group A(R)/W(R)A(R)/W(R), its action on the Dynkin graph, and the element w0w_0 of W(R)W(R) that transforms BB to −B-B.

(XII) The action of P(R−)/Q(R−)P(R^-)/Q(R^-) on the completed Dynkin graph and the action of A(R)/W(R)A(R)/W(R) on P(R−)/Q(R−)P(R^-)/Q(R^-).

For each Dynkin graph in Th. 3, these data will be collected in Plates I to IX, and ordered in a uniform way as above. We also give:

(XIII) The Cartan matrix, from which the Dynkin graph is derived as described in no. 2.

5. Systems of type BlB_l (l≥2l \geq 2)

(I) We consider the group L0L_0 in V=RlV = \mathbf{R}^l (no. 4). Let RR be the set of α∈L0\alpha \in L_0 such that (α∣α)=1(\alpha|\alpha) = 1 or (α∣α)=2(\alpha|\alpha) = 2, in other words the set of vectors ±εi\pm \varepsilon_i (1≤i≤l1 \leq i \leq l) and ±εi±εj\pm \varepsilon_i \pm \varepsilon_j (1≤i<j≤l1 \leq i < j \leq l). It is clear that RR generates VV and that 2(α∣β)/(α∣α)∈Z2(\alpha|\beta)/(\alpha|\alpha) \in \mathbf{Z} for all α,β∈R\alpha, \beta \in R. Thus RR is a reduced root system in VV (no. 4). The number of roots is n=2l+4l(l−1)/2=2l2n = 2l + 4^{l(l-1)/2} = 2l^2.

(II) Put

α1=ε1−ε2, α2=ε2−ε3,…,αl−1=εl−1−ε1, αl=εl. \alpha_1 = \varepsilon_1 - \varepsilon_2,\ \alpha_2 = \varepsilon_2 - \varepsilon_3,\ldots,\alpha_{l-1} = \varepsilon_{l-1} - \varepsilon_1,\ \alpha_l = \varepsilon_l.

Then

εi=αi+αi+1+⋯+αl(1≤i≤l) \varepsilon_i = \alpha_i + \alpha_{i+1} + \cdots + \alpha_l \quad (1 \leq i \leq l)
εi+εj=(αi+αi+1+⋯+αl)+(αj+αj+1+⋯+αl)(1≤i<j≤l) \varepsilon_i + \varepsilon_j = (\alpha_i + \alpha_{i+1} + \cdots + \alpha_l) + (\alpha_j + \alpha_{j+1} + \cdots + \alpha_l) \quad (1 \leq i < j \leq l)
εi−εj=αi+αi+1+⋯+αj−1(1≤i<j≤l). \varepsilon_i - \varepsilon_j = \alpha_i + \alpha_{i+1} + \cdots + \alpha_{j-1} \quad (1 \leq i < j \leq l).

Thus (α1,α2,…,αl)(\alpha_1, \alpha_2, \ldots, \alpha_l) is a basis of RR (§ 1, no. 7, Cor. 3 of Prop. 20). Moreover, ∥αi∥2=2\| \alpha_i \|^2 = 2 for i<li < l, ∥αl∥2=1\| \alpha_l \|^2 = 1, (αi∣αi+1)=−1(\alpha_i|\alpha_{i+1}) = -1 for 1≤i≤l−11 \leq i \leq l-1, (αi∣αj)=0(\alpha_i|\alpha_j) = 0 for j>i+1j > i + 1: the Dynkin graph of RR is thus of type BlB_l, which shows that RR is irreducible. The positive roots are the εi\varepsilon_i and the εi±εj\varepsilon_i \pm \varepsilon_j (i<ji < j).

(III) By Th. 1 (ii) of Chap. V, § 6, no. 2,

h=n/l=2l. h = n/l = 2l.

(IV) Let α~=ε1+ε2=α1+2α2+2α3+⋯+2αl\tilde{\alpha} = \varepsilon_1 + \varepsilon_2 = \alpha_1 + 2\alpha_2 + 2\alpha_3 + \cdots + 2\alpha_l, which is a root. The sum of its coordinates relative to the basis (αi)(\alpha_i) is 2l−1=h−12l - 1 = h - 1. In view of Prop. 31 of § 1, no. 11, α~\tilde{\alpha} is the highest root of RR. We have (α~∣αi)=0(\tilde{\alpha}|\alpha_i) = 0 for i≠2i \neq 2 and (α~∣α2)=1(\tilde{\alpha}|\alpha_2) = 1. Since α2\alpha_2 is of length 1 (resp. 2\sqrt{2}) when l=2l = 2 (resp. l≥3l \geq 3), the completed Dynkin graph of RR is as follows:

for l=2l = 2

α2α1 \begin{array}{c} \alpha_2 \\ \alpha_1 \end{array}

for l≥3l \geq 3

α1α2α3⋯αl−1αl \begin{array}{cccccc} \alpha_1 & & & & & \\ & \alpha_2 & \alpha_3 & \cdots & \alpha_{l-1} & \alpha_l \end{array}

(V) The formula α−=2α(α∣α)\alpha^- = \frac{2\alpha}{(\alpha|\alpha)} gives for R−R^- the set of vectors ±2εi\pm 2\varepsilon_i (1≤i≤l1 \leq i \leq l), ±εi±εj\pm \varepsilon_i \pm \varepsilon_j (1≤i<j≤l1 \leq i < j \leq l). The Dynkin graph of R−R^- is obtained from that of RR by the procedure explained in no. 2, and we see that R−R^- is of type ClC_l.

There are 4l−24l - 2 roots not orthogonal to β=ε1\beta = \varepsilon_1, namely ±ε1\pm \varepsilon_1 and ±ε1±εj\pm \varepsilon_1 \pm \varepsilon_j for 2≤j≤l2 \leq j \leq l; for each such root α\alpha, n(α,β)=±2n(\alpha, \beta) = \pm 2. Formula (17) of § 1, no. 12 shows that, for ΦR\Phi_R, the square of the length of β\beta is (4l−2)−1(4l - 2)^{-1}: hence ΦR(x,y)=(x∣y)/(4l−2)\Phi_R(x, y) = (x|y)/(4l - 2). Apply formula (18) of § 1, no. 12 with x=y=βx = y = \beta. This gives

2+14(4l−4)=γ(R)14l−2 2 + \frac{1}{4}(4l - 4) = \gamma(R) \frac{1}{4l - 2}
and so γ(R)=(l+1)(4l−2)\gamma(R) = (l + 1)(4l - 2).

(VI) The fundamental weights ωi\omega_i (1≤i≤l1 \leq i \leq l) such that (ωi∣αj)=δij(\omega_i|\alpha_j) = \delta_{ij} are easily calculated, and we find that

ωi=ε1+ε2+⋯+εi=α1+2α2+⋯+(i−1)αi−1+i(α1+αi+1+⋯+αl)(i<l)ωl=12(ε1+ε2+⋯+εl)=12(α1+2α2+⋯+lαl). \begin{align*} \omega_i &= \varepsilon_1 + \varepsilon_2 + \cdots + \varepsilon_i \\ &= \alpha_1 + 2\alpha_2 + \cdots + (i - 1)\alpha_{i-1} + i(\alpha_1 + \alpha_{i+1} + \cdots + \alpha_l) \quad (i < l) \\ \omega_l &= \frac{1}{2}(\varepsilon_1 + \varepsilon_2 + \cdots + \varepsilon_l) = \frac{1}{2}(\alpha_1 + 2\alpha_2 + \cdots + l\alpha_l). \end{align*}

(VII) The sum of the positive roots is

2ρ=(2l−1)ε1+(2l−3)ε2+⋯+3εl−1+εl=(2l−1)α1+2(2l−2)α2+⋯+i(2l−i)αi+⋯+l2αl. \begin{align*} 2\rho &= (2l - 1)\varepsilon_1 + (2l - 3)\varepsilon_2 + \cdots + 3\varepsilon_{l-1} + \varepsilon_l \\ &= (2l - 1)\alpha_1 + 2(2l - 2)\alpha_2 + \cdots + i(2l - i)\alpha_i + \cdots + l^2\alpha_l. \end{align*}

(VIII) We have Q(R)=L0Q(R) = L_0 (no. 4), and P(R)P(R) is generated by Q(R)Q(R) and ωl\omega_l, hence is equal to L2L_2 (no. 4). Hence, P(R)/Q(R)P(R)/Q(R) is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z}, and the connection index is equal to 2.

(IX) and (X) In Rl\mathbf{R}^l, the orthogonal reflection sεi,−εjs_{\varepsilon_i, -\varepsilon_j} (i≠ji \neq j) interchanges εi\varepsilon_i and εj\varepsilon_j and leaves εk\varepsilon_k invariant when the index kk is distinct from ii and jj. The sεi,−εis_{\varepsilon_i, -\varepsilon_i} generate a group G1G_1 isomorphic to the symmetric group SlS_l. The orthogonal reflection sεis_{\varepsilon_i} transforms εi\varepsilon_i to −εi-\varepsilon_i and leaves invariant the εk\varepsilon_k when the index kk is distinct from ii. The sεis_{\varepsilon_i} generate a group G2G_2 isomorphic to (Z/2Z)l(\mathbf{Z}/2\mathbf{Z})^l. The Weyl group W(R)W(R) is generated by G1G_1 and G2G_2, and G2G_2 is normal in W(R)W(R), so W(R)W(R) is isomorphic to the semi-direct product of GlG_l by (Z/2Z)l(\mathbf{Z}/2\mathbf{Z})^l. Its order is therefore 2l.l!2^l.l!.

The symmetric algebra S(Rl)S(\mathbf{R}^l) can be identified canonically with the algebra of polynomial functions P(ξ1,…,ξl)P(\xi_1, \ldots, \xi_l) on Rl\mathbf{R}^l. For such a polynomial to be invariant under W(R)W(R), it is first of all necessary that

P(ξ1,ξ2,…,ξl)=P(±ξ1,±ξ2,…,±ξl) P(\xi_1, \xi_2, \ldots, \xi_l) = P(\pm \xi_1, \pm \xi_2, \ldots, \pm \xi_l)
for all choices of the signs on the right-hand side, so that
P(ξ1,…,ξl)=Q(ξ12,…,ξl2) P(\xi_1, \ldots, \xi_l) = Q(\xi_1^2, \ldots, \xi_l^2)

where Q is a polynomial, and further that Q is a symmetric polynomial; and these conditions are sufficient. Consequently (Algebra. Chap. V, App. I), S(Rl)W(R)S(\mathbf{R}^l)^{W(R)} is the algebra generated by the l polynomial functions

ti=∑τ∈Slξτ(1)2ξτ(2)2⋯ξτ(l)2(1≤i≤l). t_i = \sum_{\tau \in S_l} \xi_{\tau(1)}^2 \xi_{\tau(2)}^2 \cdots \xi_{\tau(l)}^2 \quad (1 \leq i \leq l).

Moreover, the transcendence degree over R\mathbf{R} of the field of fractions of S(Rl)W(R)S(\mathbf{R}^l)^{W(R)} is l, so the tit_i are algebraically independent. Since the tit_i have degree 2, 4, ..., 2l, we conclude that the exponents of W(R) (Chap. V. § 6, no. 3, Prop. 3) are:

1,3,5,…,2l−1. 1, 3, 5, \ldots, 2l - 1.

(XI) The only automorphism of the Dynkin graph is the identity element. Thus, A(R)=W(R)A(R) = W(R) and −1∈W(R)-1 \in W(R). Since −1-1 transforms B to −B-B, we conclude that w0=−1w_0 = -1.

(XII) The group P(R−)/Q(R−)P(R^-)/Q(R^-) is dual to P(R)/Q(R)P(R)/Q(R), and hence is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z}. Its non-trivial element permutes the vertices corresponding to α0\alpha_0 and α1\alpha_1 and leaves the others fixed.

6. Systems of type ClC_l (l≥2l \geq 2)

(I) The existence of root systems of type ClC_l has been proved in no. 5, since we have seen that the inverse system of a system of type BlB_l is of type ClC_l. A root system of type ClC_l is thus obtained by taking in R′\mathbf{R}' the vectors ±2εi\pm 2\varepsilon_i (1≤i≤l1 \leq i \leq l), and ±εi±εj\pm \varepsilon_i \pm \varepsilon_j (1≤i<j≤l1 \leq i < j \leq l). The number of roots is 2l22l^2.

(II) A basis of R can be obtained by taking the image under the map α↦2α(α∣α)\alpha \mapsto \frac{2\alpha}{(\alpha|\alpha)} of the basis of the system considered in no. 5. We obtain:

α1=ε1−ε2,α2=ε2−ε3,…,αl−1=εl−1−εl,αl=2εl. \alpha_1 = \varepsilon_1 - \varepsilon_2, \quad \alpha_2 = \varepsilon_2 - \varepsilon_3, \ldots, \quad \alpha_{l-1} = \varepsilon_{l-1} - \varepsilon_l, \quad \alpha_l = 2\varepsilon_l.

The positive roots are the 2εi2\varepsilon_i and the εi±εj\varepsilon_i \pm \varepsilon_j (i<ji < j).

(III) The Coxeter number is the same as for the inverse system: h=2lh = 2l.

(IV) Let α~=2ε1=2α1+2α2+⋯+2αl−1+αl\tilde{\alpha} = 2\varepsilon_1 = 2\alpha_1 + 2\alpha_2 + \cdots + 2\alpha_{l-1} + \alpha_l, which is a root. The sum of its coordinates relative to (αi)(\alpha_i) is 2l−1=h−12l - 1 = h - 1. Hence, α~\tilde{\alpha} is the highest root. We have (α~∣αi)=0(\tilde{\alpha}|\alpha_i) = 0 for i≠li \neq l, (α~∣αl)=2(\tilde{\alpha}|\alpha_l) = 2. Thus, the completed Dynkin graph is

!Dynkin graph for C_l

(V) We have already determined R−R^-, which is of type BlB_l. By formula (19) of § 1, no. 12 and by no. 5 (V), the square of the length of 2εi2\varepsilon_i for ΦR\Phi_R is

((l+1)(4l−2))−1((4l−2)−1)−1=(l+1)−1; ((l+1)(4l-2))^{-1} ((4l-2)^{-1})^{-1} = (l+1)^{-1};

thus, ΦR(x,y)=(x∣y)/4(l+1)\Phi_R(x, y) = (x|y)/4(l+1).

We have γ(R)=γ(R−)=(l+1)(4l−2)\gamma(R) = \gamma(R^-) = (l+1)(4l-2).

(VI) The fundamental weights are easily found:

ωi=ε1+ε2+⋯+εi \omega_i = \varepsilon_1 + \varepsilon_2 + \cdots + \varepsilon_i
=α1+2α2+⋯+(i−1)αi−1+i(αi+αi+1+⋯+12αl)(i≤l). = \alpha_1 + 2\alpha_2 + \cdots + (i-1)\alpha_{i-1} + i(\alpha_i + \alpha_{i+1} + \cdots + \frac{1}{2}\alpha_l) \quad (i \leq l).

(VII) The sum of the positive roots is

2ρ=2lε1+(2l−2)ε2+⋯+4εl−1+2εl 2\rho = 2l\varepsilon_1 + (2l-2)\varepsilon_2 + \cdots + 4\varepsilon_{l-1} + 2\varepsilon_l
=2lα1+2(2l−1)α3+⋯+i(2l−i+1)αi+⋯ = 2l\alpha_1 + 2(2l-1)\alpha_3 + \cdots + i(2l-i+1)\alpha_i + \cdots
⋯+(l−1)(l+2)αl−1+12l(l+1)αl. \cdots + (l-1)(l+2)\alpha_{l-1} + \frac{1}{2}l(l+1)\alpha_l.

(VIII) By no. 4 and no. 5 (VIII), Q(R)=L1,P(R)=L0;P(R)/Q(R)Q(R) = L_1, P(R) = L_0; P(R)/Q(R) is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z}, and the connection index is 2.

(IX) and (X) These data depend only on W(R)W(R), and so are the same as for type BlB_l.

(XI) The same argument as in no. 5 shows that A(R)=W(R)A(R) = W(R) and w0=−1w_0 = -1.

(XII) The single non-identity element of P(R−)/Q(R−)P(R^-)/Q(R^-) defines the unique non-trivial automorphism of the completed Dynkin graph: it interchanges the vertices corresponding to αj\alpha_j and αl−j\alpha_{l-j} for 0≤j≤l0 \leq j \leq l.

7. Systems of type AlA_l (l≥1l \geq 1)

(I) and (II) Let VV be the hyperplane in E=Rl+1E = \mathbf{R}^{l+1} with equation ∑i=1l+1ξi=0\sum_{i=1}^{l+1} \xi_i = 0. Replacing ll by l+1l+1 in no. 5, we obtain a system R′R' of type Bl+1B_{l+1} in EE with basis

α1=ε1−ε2, α2=ε2−ε3,…,αl=εl−εl+1, αl+1=εl+1. \alpha_1 = \varepsilon_1 - \varepsilon_2,\ \alpha_2 = \varepsilon_2 - \varepsilon_3, \ldots, \alpha_l = \varepsilon_l - \varepsilon_{l+1},\ \alpha_{l+1} = \varepsilon_{l+1}.
Since α1,…,αl\alpha_1, \ldots, \alpha_l generate VV, R=R′∩VR = R' \cap V is a root system in VV with basis (α1,…,αl)(\alpha_1, \ldots, \alpha_l) (§ 1, no. 7, Cor. 4 of Prop. 20). By the calculation of the scalar products in no. 5, it is immediate that RR is of type AlA_l. The elements of RR are the εi−εj\varepsilon_i - \varepsilon_j (i≠j,1≤i≤l+1,1≤j≤l+1i \neq j, 1 \leq i \leq l+1, 1 \leq j \leq l+1). There are n=l(l+1)n = l(l+1) roots. The positive roots are the εi−εj\varepsilon_i - \varepsilon_j where i<ji < j.

(III) We have h=n/l=l+1h = n/l = l+1.

(IV) Let α~=ε1−εl+1=α1+α2+⋯+αl\tilde{\alpha} = \varepsilon_1 - \varepsilon_{l+1} = \alpha_1 + \alpha_2 + \cdots + \alpha_l, which is a root. The sum of its coordinates relative to (αi)(\alpha_i) is l=h−1l = h-1. Hence α~\tilde{\alpha} is the highest root. For l=1l = 1, α~=α1\tilde{\alpha} = \alpha_1 so (α~∣α1)=2(\tilde{\alpha}|\alpha_1) = 2; the Coxeter graph of the group Wa(R)W_a(R) is

∞α1 \begin{array}{c} \infty \\ \alpha_1 \end{array}

For l≥2l \geq 2. (α~∣αi)=0(\tilde{\alpha}|\alpha_i) = 0 for 0<i<l0 < i < l and (α~∣α1)=(α~∣αl)=1(\tilde{\alpha}|\alpha_1) = (\tilde{\alpha}|\alpha_l) = 1. Hence the completed Dynkin graph is:

!Dynkin graph

(V) Identifying V with its dual using the scalar product, we have α~=2α(α∣α)=α\tilde{\alpha} = \frac{2\alpha}{(\alpha|\alpha)} = \alpha for all α∈R\alpha \in \mathbf{R}, so R∗=RR^* = R.

For the form ΦR\Phi_R, the length of the roots is h−1/2=(l+1)−1/2h^{-1/2} = (l+1)^{-1/2} (§ 1, no. 12); so Φr(x,y)=(x∣y)/2(l+1)\Phi_r(x, y) = (x|y)/2(l+1).

We have γ(R)=(l+1)2\gamma(R) = (l+1)^2 (§ 1, no. 12, formula (20)).

(VI) Let (ωi)1≤i≤l(\omega_i)_{1 \leq i \leq l} be the family of fundamental weights. Put

ωi=∑j=1l+1ξijεj.with ξij∈R. \omega_i = \sum_{j=1}^{l+1} \xi_{ij} \varepsilon_j. \quad \text{with } \xi_{ij} \in \mathbf{R}.

The conditions (ωi∣αj)=δij(\omega_i|\alpha_j) = \delta_{ij} and ωi∈V\omega_i \in V give

ξii−ξi,i+1=1,ξij−ξi,j+1=0 for j≠i.∑j=1l+1ξij=0, \xi_{ii} - \xi_{i,i+1} = 1, \quad \xi_{ij} - \xi_{i,j+1} = 0 \text{ for } j \neq i. \quad \sum_{j=1}^{l+1} \xi_{ij} = 0,

which easily lead to

ωi=ε1+⋯+εi−il+1(ε1+⋯+εl+1)=1l+1((l−i+1)(α1+2α2+⋯+(i−1)αi−1)+i((l−i+1)αi+(l−i)αi+1+⋯+αl)). \begin{align*} \omega_i &= \varepsilon_1 + \cdots + \varepsilon_i - \frac{i}{l+1}(\varepsilon_1 + \cdots + \varepsilon_{l+1}) \\ &= \frac{1}{l+1}((l-i+1)(\alpha_1 + 2\alpha_2 + \cdots + (i-1)\alpha_{i-1}) \\ &\qquad + i((l-i+1)\alpha_i + (l-i)\alpha_{i+1} + \cdots + \alpha_l)). \end{align*}

(VII) The sum of the positive roots is

2ρ=lε1+(l−2)ε2+(l−4)ε3+⋯−(l−2)εl−lεl+1=lα1+2(l−1)α2+⋯+i(l−i+1)αi+⋯+lαl. \begin{align*} 2\rho &= l\varepsilon_1 + (l-2)\varepsilon_2 + (l-4)\varepsilon_3 + \cdots - (l-2)\varepsilon_l - l\varepsilon_{l+1} \\ &= l\alpha_1 + 2(l-1)\alpha_2 + \cdots + i(l-i+1)\alpha_i + \cdots + l\alpha_l. \end{align*}

(VIII) Introduce in E=Rl+1E = \mathbf{R}^{l+1} the subgroup L0L_0 of no. 4. Let pp be the orthogonal projection of EE onto VV. By § 1, no. 10, Prop. 28, we have

Q(R)=Q(R′)∩V⊄L0∩V,andP(R)=p(P(R′)); Q(R) = Q(R') \cap V \not\subset L_0 \cap V, \quad \text{and} \quad P(R) = p(P(R'));

in view of the fact that the last fundamental weight of R′R' is orthogonal to VV, we have P(R)=p(Q(R′))=p(L0)P(R) = p(Q(R')) = p(L_0). Thus, P(R)P(R) is the group generated by the εi−εj\varepsilon_i - \varepsilon_j and by p(ε1)=ε1−(l+1)−1∑i=1l+1εip(\varepsilon_1) = \varepsilon_1 - (l+1)^{-1} \sum_{i=1}^{l+1} \varepsilon_i, so

P(R)=Q(R)+Z(ε1−(l+1)−1∑i=1l+1εi). P(R) = Q(R) + \mathbf{Z}(\varepsilon_1 - (l+1)^{-1} \sum_{i=1}^{l+1} \varepsilon_i).

Now l+1l + 1 is the smallest integer m>0m > 0 such that mp(ε1)∈Q(R)mp(\varepsilon_1) \in Q(R). Thus P(R)/Q(R)P(R)/Q(R) is isomorphic to Z/(l+1)Z\mathbf{Z}/(l+1)\mathbf{Z} and the connection index is l+1l + 1.

(IX) and (X) For any automorphism gg of VV, let φ(g)\varphi(g) be the automorphism of EE that extends gg and leaves ε1+ε2+⋯+εl\varepsilon_1 + \varepsilon_2 + \cdots + \varepsilon_l invariant. If gg is the orthogonal reflection sεi−εj∣Vs_{\varepsilon_i - \varepsilon_j}|V, φ(g)\varphi(g) is equal to sεi−εjs_{\varepsilon_i - \varepsilon_j}, which interchanges εi\varepsilon_i and εj\varepsilon_j and leaves fixed the εk\varepsilon_k with kk distinct from ii and jj. Let

X={ε1,ε2,…,εl+1}. X = \{\varepsilon_1, \varepsilon_2, \ldots, \varepsilon_{l+1}\}.

Then g↦φ(g)∣Xg \mapsto \varphi(g)|X is an isomorphism from W(R)W(R) to the symmetric group of XX. Thus, W(R)W(R) is isomorphic to the symmetric group Sl+1S_{l+1}, and so is of order (l+1)!(l+1)!.

The symmetric algebra S(E)S(E) can be identified canonically with the algebra of polynomial functions P(ξ1,ξ2,…,ξl+1)P(\xi_1, \xi_2, \ldots, \xi_{l+1}) on EE. Let G=φ(W(R))G = \varphi(W(R)). By the preceding paragraph, the set S(E)GS(E)^G of elements of S(E)S(E) invariant under GG is the set of symmetric polynomials (Algebra, Chap. V, App. I), and consequently (\emph{ibid.}) is the algebra generated by the functions

si′=∑τ∈Sl+1ξτ(1)ξτ(2)⋯ξτ(i)(1≤i≤l+1). s'_i = \sum_{\tau \in S_{l+1}} \xi_{\tau(1)} \xi_{\tau(2)} \cdots \xi_{\tau(i)} \quad (1 \leq i \leq l+1).

The algebra S(V)S(V) can be identified with the restrictions to VV of the polynomial functions on EE. If P∈S(E)GP \in S(E)^G, the restriction of PP to VV is clearly invariant under W(R)W(R). Conversely, if Q∈S(V)W(R)Q \in S(V)^{W(R)}, there exists P∈S(E)P \in S(E) extending QQ; replacing PP by ((l+1)!)−1∑g∈Gg(P)((l+1)!)^{-1} \sum_{g \in G} g(P), which has the same restriction as PP to VV, we can assume that P∈S(E)GP \in S(E)^G. Thus, S(V)W(R)S(V)^{W(R)} is generated by the si=si′∣Vs_i = s'_i|V. Now s1=0s_1 = 0. Moreover, the transcendence degree over R\mathbf{R} of the field of fractions of S(V)W(R)S(V)^{W(R)} is ll, so the sis_i (2≤i≤l+12 \leq i \leq l+1) are algebraically independent. Since the sis_i are of degrees 2,3,…,l+12, 3, \ldots, l+1, the exponents of W(R)W(R) are

1,2,3,…,l. 1, 2, 3, \ldots, l.

(XI) For l=1l = 1, A(R)=W(R)=Z/2ZA(R) = W(R) = \mathbf{Z}/2\mathbf{Z} and w0=−1w_0 = -1.

For l≥2l \geq 2, let ε∈A(R)\varepsilon \in A(R) be the automorphism that transforms αi\alpha_i to αl+1−i\alpha_{l+1-i}. It is clear that the automorphism induced by ε\varepsilon is the unique non-trivial automorphism of the Dynkin graph. The group A(R)/W(R)A(R)/W(R) is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z}. Since −1-1 is an element of A(R)A(R) which does not belong to W(R)W(R) by (IX) and (X), we see that A(R)A(R) is isomorphic to W(R)×Z/2ZW(R) \times \mathbf{Z}/2\mathbf{Z}. We have w0=−εw_0 = -\varepsilon.

(XII) The group P(R−)/Q(R−)P(R^-)/Q(R^-) is cyclic of order l+1l+1 and acts on the completed Dynkin graph by circular permutations. If l≥2l \geq 2, the unique non-identity element of A(R)/W(R)A(R)/W(R) acts on P(R−)/Q(R−)P(R^-)/Q(R^-) by the automorphism x↦−xx \mapsto -x.

8. Systems of type DlD_l (l≥3l \geq 3)

(I) Consider in V=R′V = \mathbf{R}' the group L0L_0 (no. 4). The set RR of α∈L0\alpha \in L_0 such that (α∣α)=2(\alpha|\alpha) = 2 consists of the vectors ±εi±εj\pm \varepsilon_i \pm \varepsilon_j (1≤i<j≤l1 \leq i < j \leq l). It is clear that RR generates VV and that 2(α∣β)/(α∣α)∈Z2(\alpha|\beta)/(\alpha|\alpha) \in \mathbf{Z} for all α,β∈R\alpha, \beta \in R. Thus RR is a reduced root system in VV (no. 4). The number of roots is n=2l(l−1)n = 2l(l-1).

(II) Put

α1=ε1−ε2, α2=ε2−ε3……αl−1=εl−1−εl, αl=εl−1+εl. \alpha_1 = \varepsilon_1 - \varepsilon_2,\ \alpha_2 = \varepsilon_2 - \varepsilon_3 \ldots \ldots \alpha_{l-1} = \varepsilon_{l-1} - \varepsilon_l,\ \alpha_l = \varepsilon_{l-1} + \varepsilon_l.

The following formulas are immediate:

εi−εj=αi+αi+1+⋯+αj−1(i<j) \varepsilon_i - \varepsilon_j = \alpha_i + \alpha_{i+1} + \cdots + \alpha_{j-1}\quad (i < j)
εi+εj=αi+αi+1+⋯+αj−1+2αj+2αj+1+⋯ \varepsilon_i + \varepsilon_j = \alpha_i + \alpha_{i+1} + \cdots + \alpha_{j-1} + 2\alpha_j + 2\alpha_{j+1} + \cdots
⋯+2αl−2+αl−1+αl(i<j≤l−2) \cdots + 2\alpha_{l-2} + \alpha_{l-1} + \alpha_l\quad (i < j \leq l-2)
εi+εl−1=αi+αi+1+⋯+αl(i<l−1) \varepsilon_i + \varepsilon_{l-1} = \alpha_i + \alpha_{i+1} + \cdots + \alpha_l\quad (i < l-1)
εi+εl=αi+αi+1+⋯+αl−2+αl(i<l−1) \varepsilon_i + \varepsilon_l = \alpha_i + \alpha_{i+1} + \cdots + \alpha_{l-2} + \alpha_l\quad (i < l-1)
εl−1+εl=αl. \varepsilon_{l-1} + \varepsilon_l = \alpha_l.

so (α1,…,αl)(\alpha_1, \ldots, \alpha_l) is a basis if RR (§ 1, no. 2, Cor. 3 of Prop. 20). Further, ∥αi∥2=2\| \alpha_i \| ^2 = 2 for all ii. (αi∣αj)=0(\alpha_i|\alpha_j) = 0 for i+1<ji + 1 < j except for i=l−2,j=li = l-2, j = l in which case (αl−2∣αl)=−1(\alpha_{l-2}|\alpha_l) = -1, (αi∣αi+1)=−1(\alpha_i|\alpha_{i+1}) = -1 for i≤l−2i \leq l-2, and finally (αl−1∣αl)=−1(\alpha_{l-1}|\alpha_l) = -1; the Dynkin graph of RR is thus of type DlD_l. The positive roots are the εi±εj\varepsilon_i \pm \varepsilon_j for i<ji < j.

(III) We have h=n/l=2(l−1)h = n/l = 2(l-1).

(IV) Let α~=ε1+ε2=α1+2α2+⋯+2αl−2+αl−1+αl\tilde{\alpha} = \varepsilon_1 + \varepsilon_2 = \alpha_1 + 2\alpha_2 + \cdots + 2\alpha_{l-2} + \alpha_{l-1} + \alpha_l, which is a root. The sum of its coordinates relative to (αi)(\alpha_i) is

2l−3=h−1. 2l-3 = h-1.

Hence α~\tilde{\alpha} is the highest root.

If l=3l = 3, we have

(α~∣α1)=0,(α~∣α2)=(α~∣α3)=1. (\tilde{\alpha}|\alpha_1) = 0,\quad (\tilde{\alpha}|\alpha_2) = (\tilde{\alpha}|\alpha_3) = 1.

If l≥4l \geq 4, we have (α~∣αi)=0(\tilde{\alpha}|\alpha_i) = 0 for i≠2i \neq 2 and (α~∣α2)=1(\tilde{\alpha}|\alpha_2) = 1. Hence the completed Dynkin graph is:

!Dynkin graph for D_l

(V) Since (α∣α)=2(\alpha|\alpha) = 2 for all α∉R\alpha \notin R, we have R−=RR^- = R. The length of the roots for ΦL′\Phi_{L'} is h−1/2=(2l−2)−1/2h^{-1/2} = (2l-2)^{-1/2}. Hence

ΦR(x,y)=(x∣y)/(4l−4)andγ(R)=4(l−1)2. \Phi_R(x, y) = (x|y)/(4l-4)\quad \text{and}\quad \gamma(R) = 4(l-1)^2.

(VI) A calculation analogous to that in no. 7 gives the fundamental weights:

ωi=ε1+ε2+⋯+εi=α1+2α2+⋯+(i−1)αi−1+i(αi+αi+1+⋯+αl−2)+12i(αl−1+αl) \omega_i = \varepsilon_1 + \varepsilon_2 + \cdots + \varepsilon_i \\ = \alpha_1 + 2\alpha_2 + \cdots + (i-1)\alpha_{i-1} + i(\alpha_i + \alpha_{i+1} + \cdots + \alpha_{l-2}) \\ \quad + \frac{1}{2}i(\alpha_{l-1} + \alpha_l)

for i<l−1i < l - 1,

ωl−1=12(ε1+ε2+⋯+εl−2+εl−1−εl)=12(α1+2α2+⋯+(l−2)αl−2+12lαl−1+12(l−2)αl), \omega_{l-1} = \frac{1}{2}(\varepsilon_1 + \varepsilon_2 + \cdots + \varepsilon_{l-2} + \varepsilon_{l-1} - \varepsilon_l) \\ = \frac{1}{2}(\alpha_1 + 2\alpha_2 + \cdots + (l-2)\alpha_{l-2} + \frac{1}{2}l\alpha_{l-1} + \frac{1}{2}(l-2)\alpha_l),
ωl=12(ε1+ε2+⋯+εl−2+εl−1+εl)=12(α1+2α2+⋯+(l−2)αl−2+12(l−2)αl−1+12lαl). \omega_l = \frac{1}{2}(\varepsilon_1 + \varepsilon_2 + \cdots + \varepsilon_{l-2} + \varepsilon_{l-1} + \varepsilon_l) \\ = \frac{1}{2}(\alpha_1 + 2\alpha_2 + \cdots + (l-2)\alpha_{l-2} + \frac{1}{2}(l-2)\alpha_{l-1} + \frac{1}{2}l\alpha_l).

(VII) The sum of the positive roots is

2ρ=2(l−1)ε1+2(l−2)ε2+⋯+2εl−1=∑i=1l−22(i(l−i(i+1)2))αi+l(l−1)2(αl−1+αl). 2\rho = 2(l-1)\varepsilon_1 + 2(l-2)\varepsilon_2 + \cdots + 2\varepsilon_{l-1} \\ = \sum_{i=1}^{l-2} 2(i(l-\frac{i(i+1)}{2}))\alpha_i + \frac{l(l-1)}{2}(\alpha_{l-1} + \alpha_l).

(VIII) The ±εi±εj\pm \varepsilon_i \pm \varepsilon_j generate L1L_1 (no. 4), so Q(R)=L1Q(R) = L_1. Hence Q(R∗)=L1Q(R^*) = L_1 and consequently P(R)=L2P(R) = L_2 (no. 4). By no. 4, P(R)/Q(R)P(R)/Q(R) is isomorphic to Z/4Z\mathbf{Z}/4\mathbf{Z} for ll odd, and to Z/2Z×Z/2Z\mathbf{Z}/2\mathbf{Z} \times \mathbf{Z}/2\mathbf{Z} for ll even. In the first case, P(R)/Q(R)P(R)/Q(R) is generated by the canonical image of ωl\omega_l (and also by that of ωl−1\omega_{l-1}). In the second case, P(R)/Q(R)P(R)/Q(R) is generated by the canonical images of ωl−1\omega_{l-1} and ωl\omega_l. In both cases the connection index is 4.

(IX) and (X) In Rl\mathbf{R}^l, the orthogonal reflection sεi,−εjs_{\varepsilon_i, -\varepsilon_j} (i≠ji \neq j) interchanges εi\varepsilon_i and εj\varepsilon_j and leaves invariant the εk\varepsilon_k with kk distinct from ii and jj. The sεi,−εjs_{\varepsilon_i, -\varepsilon_j} generate a group G1G_1 isomorphic to the symmetric group SlS_l. On the other hand, sij=sεi,−εjsεi,+εjs_{ij} = s_{\varepsilon_i, -\varepsilon_j} s_{\varepsilon_i, +\varepsilon_j} transforms εi\varepsilon_i to −εi-\varepsilon_i, εj\varepsilon_j to −εj-\varepsilon_j and leaves invariant the εk\varepsilon_k with kk distinct from ii and jj. The sijs_{ij} generate a group G2G_2, the set of automorphisms uu of the vector space Rl\mathbf{R}^l such that u(εi)=(−1)νiεiu(\varepsilon_i) = (-1)^{\nu_i} \varepsilon_i with ∏i=1l(−1)νi=1\prod_{i=1}^l (-1)^{\nu_i} = 1. The group G2G_2 is isomorphic to (Z/2Z)l−1(\mathbf{Z}/2\mathbf{Z})^{l-1}, and G2G_2 is normal in W(R)W(R), so W(R)W(R) is isomorphic to the semi-direct product of SlS_l by (Z/2Z)l−1(\mathbf{Z}/2\mathbf{Z})^{l-1}. Consequently, its order is 2l−1l!2^{l-1} l!.

The polynomial functions tit_i of no. 5 are invariant under W(R)W(R), and so is t=ξ1ξ2…ξlt = \xi_1 \xi_2 \ldots \xi_l; moreover, tl=t2t_l = t^2. Let P(ξ1,…,ξl)P(\xi_1, \ldots, \xi_l) be a polynomial invariant under W(R)W(R). Let ξ1ν1ξ2ν2…ξlνl\xi_1^{\nu_1} \xi_2^{\nu_2} \ldots \xi_l^{\nu_l} be a monomial featuring in PP such that νi\nu_i is odd; then νj\nu_j is odd for all jj because the monomial (−1)νi+νjξ1ν1ξ2ν2…ξlνl(-1)^{\nu_i + \nu_j} \xi_1^{\nu_1} \xi_2^{\nu_2} \ldots \xi_l^{\nu_l} features in sij(P)s_{ij}(P), so νi+νj≡0(mod2)\nu_i + \nu_j \equiv 0 \pmod{2} and νj≡1(mod2)\nu_j \equiv 1 \pmod{2}. Thus

P = P_1 + tP_2, where all the monomials featuring in P_1 and P_2 have only even exponents. Since P is invariant under the permutations of the ξi\xi_i, P_1 and P_2 have the same property, and so can be written as polynomials in t1,t2,…,tlt_1, t_2, \ldots, t_l. This proves that the algebra S(Rl)W(R)S(\mathbf{R}^l)^{W(R)} is generated by t1,t2,…,tl−1,tt_1, t_2, \ldots, t_{l-1}, t. Moreover, the transcendence degree of the field of fractions of S(Rl)W(R)S(\mathbf{R}^l)^{W(R)} is l, so t1,t2,…,tl−1,tt_1, t_2, \ldots, t_{l-1}, t are algebraically independent. We conclude that the sequence of exponents, suitably ordered, is:

1,3,5,…,2l−5,2l−3,l−1. 1, 3, 5, \ldots, 2l - 5, 2l - 3, l - 1.

Note that l−1l - 1 appears twice if ll is even, and once if ll is odd.

(XI) The automorphisms of the Dynkin graph are those of the underlying graph. Thus: 1) If l=3l = 3, A(R)/W(R)A(R)/W(R) is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z}. 2) If l=4l = 4, every permutation of the terminal vertices defines an automorphism of the graph, so A(R)/W(R)A(R)/W(R) is isomorphic to S3\mathfrak{S}_3. 3) If l≥5l \geq 5, the chains starting at the ramification point have length 1, 1, and l−3≥2l - 3 \geq 2. The only automorphism of the graph distinct from the identity thus corresponds to the automorphism ε∈A(R)\varepsilon \in A(R) which interchanges αl−1\alpha_{l-1} and αl\alpha_l and leaves fixed the αi\alpha_i for 1≤i≤l−21 \leq i \leq l - 2. Thus A(R)/W(R)A(R)/W(R) is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z}; moreover, A(R)A(R) is the semi-direct product of the group G1≅SlG_1 \cong \mathfrak{S}_l defined in (IX) by the group G3G_3 consisting of the automorphisms uu of Rl\mathbf{R}^l such that u(εi)=±εiu(\varepsilon_i) = \pm \varepsilon_i for all ii.

If ll is even, −1∈W(R)-1 \in W(R), so w0=−1w_0 = -1. If ll is odd, −1∉W(R)-1 \notin W(R), so A(R)=W(R)×{1,−1}A(R) = W(R) \times \{1, -1\} and w0=−εw_0 = -\varepsilon.

(XII) For ll even, P(R−)/Q(R−)P(R^-)/Q(R^-) has three elements of order 2, namely ω1,ωl−1\omega_1, \omega_{l-1} and ωl\omega_l. Since ωl\omega_l (resp. ωl−1\omega_{l-1}) interchanges the vertices corresponding to α0\alpha_0 and αl\alpha_l (resp. αl−1\alpha_{l-1}), it interchanges those corresponding to α1\alpha_1 and αl−1\alpha_{l-1} (resp. αl\alpha_l) and also those corresponding to αj\alpha_j and αl−j\alpha_{l-j} for

2≤j≤l−2. 2 \leq j \leq l - 2.

We have ω1=ωlωl−1\omega_1 = \omega_l \omega_{l-1}.

For ll odd, P(R−)/Q(R−)P(R^-)/Q(R^-) has two elements of order 4, namely ωl−1\omega_{l-1} and ωl\omega_l, and one element of order 2, equal to ω1\omega_1. Indeed, ω1\omega_1 interchanges the vertices corresponding to α0\alpha_0 and α1\alpha_1, so it leaves fixed the vertices corresponding to αj\alpha_j for 2≤j≤l−22 \leq j \leq l - 2 and is necessarily of order 2. Consequently ωl\omega_l is of order 4 and transforms the vertex corresponding to α0\alpha_0 (resp. αl\alpha_l, resp. α1\alpha_1, resp. αl−1\alpha_{l-1}) to that corresponding to αl\alpha_l (resp. α1\alpha_1, resp. αl−1\alpha_{l-1}, resp. α0\alpha_0), and interchanges the vertices corresponding to αj\alpha_j and αl−j\alpha_{l-j} for 2≤j≤l−22 \leq j \leq l - 2. We have ω1=ωl2\omega_1 = \omega_l^2 and ωl−1=ωl3\omega_{l-1} = \omega_l^3.

For l≠4l \neq 4, the non-identity element of A(R)/W(R)A(R)/W(R) interchanges the vertices corresponding to αl−1\alpha_{l-1} and αl\alpha_l, and consequently interchanges the elements ωl−1\omega_{l-1} and ωl\omega_l of P(R−)/Q(R−)P(R^-)/Q(R^-). For ll odd, the automorphism of P(R−)/Q(R−)P(R^-)/Q(R^-) thus obtained is the map x↦−xx \mapsto -x.

For l=4l = 4, A(R)/W(R)A(R)/W(R) can be identified with the group of permutations of {1,3,4}\{1, 3, 4\} and acts by permutations of the indices on {ω1,ω3,ω4}\{\omega_1, \omega_3, \omega_4\}.

9. System of type F4F_4

(I) Consider the group L2L_2 (no. 4) in R4\mathbf{R}^4. Let RR be the set of α∈L2\alpha \in L_2 such that (α∣α)=1(\alpha|\alpha) = 1 or (α∣α)=2(\alpha|\alpha) = 2; it contains the vectors

±εi,±εi±εj (i<j),12(±ε1±ε2±ε3±ε4). \pm \varepsilon_i,\quad \pm \varepsilon_i \pm \varepsilon_j\ (i < j),\quad \frac{1}{2}(\pm \varepsilon_1 \pm \varepsilon_2 \pm \varepsilon_3 \pm \varepsilon_4).
Conversely, if α∈R\alpha \in R, the coordinates of α\alpha can only take the values 0,±12,±10, \pm \frac{1}{2}, \pm 1 (since (32)2>2(\frac{3}{2})^2 > 2); either these coordinates are all integers, giving the vectors ±εi,±εi±εj\pm \varepsilon_i, \pm \varepsilon_i \pm \varepsilon_j, or they are all equal to ±12\pm \frac{1}{2}, giving the vectors 12(±ε1±ε2±ε3±ε4)\frac{1}{2}(\pm \varepsilon_1 \pm \varepsilon_2 \pm \varepsilon_3 \pm \varepsilon_4).

We show that, for α,β∈R\alpha, \beta \in R, we have 2(α∣β)/(∣α∣α)∈Z2(\alpha|\beta)/(|\alpha|\alpha) \in \mathbf{Z}. If α=±εi\alpha = \pm \varepsilon_i or α=12(±ε1±ε2±ε3±ε4)\alpha = \frac{1}{2}(\pm \varepsilon_1 \pm \varepsilon_2 \pm \varepsilon_3 \pm \varepsilon_4), then (α∣α)=1(\alpha|\alpha) = 1 and we have seen in no. 4 that (α∣β)∈12Z(\alpha|\beta) \in \frac{1}{2}\mathbf{Z} since α,β∈L2\alpha, \beta \in L_2. If α=±εi±εj\alpha = \pm \varepsilon_i \pm \varepsilon_j, then (α∣α)=2(\alpha|\alpha) = 2 and we have seen in no. 4 that (α∣β)∈Z(\alpha|\beta) \in \mathbf{Z} since α∈L1\alpha \in L_1 and β∈L2\beta \in L_2. Hence, RR is a reduced root system in R4\mathbf{R}^4 (no. 4). The number of roots is n=8+(42)4+24=48n = 8 + \binom{4}{2} 4 + 2^4 = 48.

(II) Give R4\mathbf{R}^4 the lexicographic order defined by the basis (ε1,ε2,ε3,ε4)(\varepsilon_1, \varepsilon_2, \varepsilon_3, \varepsilon_4) (§ 1, no. 7). In particular, we have ε1>ε2>ε3>ε4\varepsilon_1 > \varepsilon_2 > \varepsilon_3 > \varepsilon_4. The positive roots are

εi,εi±εj (i<j),12(ε1±ε2±ε3±ε4). \varepsilon_i,\quad \varepsilon_i \pm \varepsilon_j\ (i < j),\quad \frac{1}{2}(\varepsilon_1 \pm \varepsilon_2 \pm \varepsilon_3 \pm \varepsilon_4).
The smallest root is α3=ε4\alpha_3 = \varepsilon_4. Among the roots belonging to Rε3+Rε4\mathbf{R}\varepsilon_3 + \mathbf{R}\varepsilon_4 but not to Rε4\mathbf{R}\varepsilon_4, the smallest is α2=ε3−ε4\alpha_2 = \varepsilon_3 - \varepsilon_4. Among the positive roots belonging to Rε2+Rε3+Rε4\mathbf{R}\varepsilon_2 + \mathbf{R}\varepsilon_3 + \mathbf{R}\varepsilon_4 but not to Rε3+Rε4\mathbf{R}\varepsilon_3 + \mathbf{R}\varepsilon_4, the smallest is α1=ε2−ε3\alpha_1 = \varepsilon_2 - \varepsilon_3. Among the positive roots not belonging to Rε2+Rε3+Rε4\mathbf{R}\varepsilon_2 + \mathbf{R}\varepsilon_3 + \mathbf{R}\varepsilon_4, the smallest is α4=12(ε1−ε2−ε3−ε4)\alpha_4 = \frac{1}{2}(\varepsilon_1 - \varepsilon_2 - \varepsilon_3 - \varepsilon_4). None of the αi\alpha_i is a sum of 2 positive roots. Hence, (α1,α2,α3,α4)(\alpha_1, \alpha_2, \alpha_3, \alpha_4) is a basis of RR (§ 1, no. 6, Cor. 1 to Prop. 19). We have ∥α1∥=∥α2∥=2,∥α3∥=∥α4∥=1,(α1∣α2)=(α2∣α3)=−1,(α3∣α4)=−12,(α1∣α3)=(α1∣α4)=(α2∣α4)=0\| \alpha_1 \| = \| \alpha_2 \| = 2, \| \alpha_3 \| = \| \alpha_4 \| = 1, (\alpha_1|\alpha_2) = (\alpha_2|\alpha_3) = -1, (\alpha_3|\alpha_4) = -\frac{1}{2}, (\alpha_1|\alpha_3) = (\alpha_1|\alpha_4) = (\alpha_2|\alpha_4) = 0. We see that the Dynkin graph of RR is of type F4F_4, and hence is irreducible.

(III) We have h=nl=12h = \frac{n}{l} = 12.

(IV) Let α~=ε1+ε2=2α1+3α2+4α3+2α4\tilde{\alpha} = \varepsilon_1 + \varepsilon_2 = 2\alpha_1 + 3\alpha_2 + 4\alpha_3 + 2\alpha_4. The sum of the coordinates of α~\tilde{\alpha} with respect to (αi)(\alpha_i) is 11=h−111 = h - 1, so α~\tilde{\alpha} is the highest root. We have (α~∣α1)=1,(α~∣α2)=(α~∣α3)=(α~∣α4)=0(\tilde{\alpha}|\alpha_1) = 1, (\tilde{\alpha}|\alpha_2) = (\tilde{\alpha}|\alpha_3) = (\tilde{\alpha}|\alpha_4) = 0.

The completed Dynkin graph is

!Dynkin graph of F_4

(V) The formula α∗=2α(α∣α)\alpha^* = \frac{2\alpha}{(\alpha|\alpha)} gives for R−R^- the set of vectors ±2εi,±εi±εj,±ε1±ε2±ε3±ε4\pm 2\varepsilon_i, \pm \varepsilon_i \pm \varepsilon_j, \pm \varepsilon_1 \pm \varepsilon_2 \pm \varepsilon_3 \pm \varepsilon_4. The Dynkin graph of R−R^- is obtained from that of RR by the procedure explained in no. 2, and we see that R−R^- is of type F4F_4.

The roots not orthogonal to β=ε1\beta = \varepsilon_1 are ±ε1,±ε1±εj (j≥2)\pm \varepsilon_1, \pm \varepsilon_1 \pm \varepsilon_j \ (j \geq 2), and 12(±ε1±ε2±ε3±ε4)\frac{1}{2}(\pm \varepsilon_1 \pm \varepsilon_2 \pm \varepsilon_3 \pm \varepsilon_4): the number n(α∣β)=2(α∣β)n(\alpha|\beta) = 2(\alpha|\beta) is equal to ±2\pm 2 for the first 14 of these roots and to ±1\pm 1 for the last 16; thus, for ΦR\Phi_R, the square of the length of β\beta is 4(14.4+16.1)−1=1184(14.4 + 16.1)^{-1} = \frac{1}{18}; hence

ΦR(x,y)=(x∣y)18. \Phi_R(x, y) = \frac{(x|y)}{18}.

We now apply formula (18) of § 1, no. 12, with x=y=βx = y = \beta; this gives

2+12.14+16.1/41=γ(R).118 2 + 12.\frac{1}{4} + 16.\frac{1/4}{1} = \gamma(R).\frac{1}{18}

so

γ(R)=2.34. \gamma(R) = 2.3^4.

(VI) Calculating the fundamental weights gives

ω1=ε1+ε2=2α1+3α2+4α3+2α4=α~ω2=2ε1+ε2+ε3=3α1+6α2+8α3+4α4ω3=12(3ε1+ε2+ε3+ε4)=2α1+4α2+6α3+3α4ω4=ε1=α1+2α2+3α3+2α4. \begin{align*} \omega_1 &= \varepsilon_1 + \varepsilon_2 = 2\alpha_1 + 3\alpha_2 + 4\alpha_3 + 2\alpha_4 = \tilde{\alpha} \\ \omega_2 &= 2\varepsilon_1 + \varepsilon_2 + \varepsilon_3 = 3\alpha_1 + 6\alpha_2 + 8\alpha_3 + 4\alpha_4 \\ \omega_3 &= \frac{1}{2}(3\varepsilon_1 + \varepsilon_2 + \varepsilon_3 + \varepsilon_4) = 2\alpha_1 + 4\alpha_2 + 6\alpha_3 + 3\alpha_4 \\ \omega_4 &= \varepsilon_1 = \alpha_1 + 2\alpha_2 + 3\alpha_3 + 2\alpha_4. \end{align*}

(VII) The sum of the positive roots is

2ρ=11ε1+5ε2+3ε3+ε4=16α1+30α2+42α3+22α4. 2\rho = 11\varepsilon_1 + 5\varepsilon_2 + 3\varepsilon_3 + \varepsilon_4 = 16\alpha_1 + 30\alpha_2 + 42\alpha_3 + 22\alpha_4.

(VIII) We have Q(R)=L2Q(R) = L_2 (no. 4), and P(R)=Q(R)P(R) = Q(R) by (VI). Hence, the connection index is 1.

(IX) The family of exponents has 4 terms, and since h=12h = 12, it must contain the integers 1, 5, 7, 11, coprime to 12 (§ 1, no. 11, Prop. 30); consequently, these are all the exponents of W(R)W(R).

(X) and (XI) The only automorphism of the Dynkin graph is the identity, so A(R)=W(R)A(R) = W(R) and w0=−1w_0 = -1. Let R′R' be the set of longest elements of RR, that is, the ±εi±εj\pm \varepsilon_i \pm \varepsilon_j; R′R' is the root system of type D4D_4 constructed in no. 8. Clearly, every element of A(R)A(R) is an element of A(R′)A(R'). Conversely, an element of A(R′)A(R') leaves L1L_1 stable (since it is generated by R′R'), hence also its associated L2L_2, and hence also RR. So W(R)=A(R)=A(R′)W(R) = A(R) = A(R'). By no. 8, W(R)W(R) is the semi-direct product of S3S_3 by W(R′)W(R'), W(R′)W(R') itself being the semi-direct product of S4S_4 by (Z/2Z)3(\mathbf{Z}/2\mathbf{Z})^3. The order of W(R)W(R) is 3!4!23=27.323!4!2^3 = 2^7.3^2.

10. System of type e_8

(I) Consider the group L_3 (no. 4) in R8\mathbf{R}^8. Let R be the set of α∈L3\alpha \in L_3 such that (α∣α)=2(\alpha|\alpha) = 2; it contains the vectors

±εi±εj(i<j),12∑i=18(−1)ν(i)εi(∑i=18ν(i) even). \pm \varepsilon_i \pm \varepsilon_j \quad (i < j), \quad \frac{1}{2} \sum_{i=1}^8 (-1)^{\nu(i)} \varepsilon_i \quad (\sum_{i=1}^8 \nu(i) \text{ even}).

Conversely, if an element α∈L3\alpha \in L_3 is such that (α∣α)=2(\alpha|\alpha) = 2, its coordinates must be among the values 0,±12,±10, \pm \frac{1}{2}, \pm 1: by no. 4, either these coordinates are all integers, giving the vectors ±εi±εj\pm \varepsilon_i \pm \varepsilon_j, or they are all equal to ±12\pm \frac{1}{2} with an integer sum, giving the vectors

12∑i=18(−1)ν(i)εi \frac{1}{2} \sum_{i=1}^8 (-1)^{\nu(i)} \varepsilon_i

with ∑i=18ν(i)\sum_{i=1}^8 \nu(i) even.

We have seen (no. 4) that (α∣β)∈Z(\alpha|\beta) \in \mathbf{Z} for all α,β∈L3\alpha, \beta \in L_3. Hence, R is a reduced root system. The number of roots is n=(82).4+27=240n = \binom{8}{2} . 4 + 2^7 = 240.

(II) Let ρ\rho be the vector (0,1,2,3,4,5,6,23)(0, 1, 2, 3, 4, 5, 6, 23) of L3L_3. No element of R is orthogonal to ρ\rho (this is clear for the ±εi±εj\pm \varepsilon_i \pm \varepsilon_j; if 12∑i=18(−1)ν(i)εi\frac{1}{2} \sum_{i=1}^8 (-1)^{\nu(i)} \varepsilon_i were orthogonal to ρ\rho, we would have ∑i=16i(−1)ν(i+1)+23(−1)ν(8)=0\sum_{i=1}^6 i(-1)^{\nu(i+1)} + 23(-1)^{\nu(8)} = 0, which is impossible since ∑i=16i<23\sum_{i=1}^6 i < 23). Hence (§ 1, no. 7, Cor. 2 of Prop. 20) the α∈R\alpha \in R such that (α∣ρ)>0(\alpha|\rho) > 0 are the positive roots relative to a certain chamber. These roots are the ±εi+εj (i<j)\pm \varepsilon_i + \varepsilon_j \ (i < j), and the

12(ε8+∑i=17(−1)ν(i)εi) \frac{1}{2} (\varepsilon_8 + \sum_{i=1}^7 (-1)^{\nu(i)} \varepsilon_i)

with ∑i=17ν(i)\sum_{i=1}^7 \nu(i) even. We have (α∣ρ)∈Z(\alpha|\rho) \in \mathbf{Z} for all α∈R\alpha \in R (no. 4), and (α∣ρ)(\alpha|\rho) is equal to 1 for the following roots:

α1=12(ε1+ε8)−12(ε2+ε3+ε4+ε5+ε6+ε7),α2=ε1+ε2, α3=ε2−ε1, α4=ε3−ε2, α5=ε4−ε3,α6=ε5−ε4, α7=ε6−ε5, α8=ε7−ε6. \begin{align*} \alpha_1 &= \frac{1}{2} (\varepsilon_1 + \varepsilon_8) - \frac{1}{2} (\varepsilon_2 + \varepsilon_3 + \varepsilon_4 + \varepsilon_5 + \varepsilon_6 + \varepsilon_7), \\ \alpha_2 &= \varepsilon_1 + \varepsilon_2, \ \alpha_3 = \varepsilon_2 - \varepsilon_1, \ \alpha_4 = \varepsilon_3 - \varepsilon_2, \ \alpha_5 = \varepsilon_4 - \varepsilon_3, \\ \alpha_6 &= \varepsilon_5 - \varepsilon_4, \ \alpha_7 = \varepsilon_6 - \varepsilon_5, \ \alpha_8 = \varepsilon_7 - \varepsilon_6. \end{align*}

and these eight vectors form a basis of R8\mathbf{R}^8. By § 1, no. 6, Cor. 1 of Prop. 19, (α1,α2,…,α8)(\alpha_1, \alpha_2, \ldots, \alpha_8) is a basis of R for which the positive roots are those which have been defined above. We have

(α4∣α5)=(α5∣α6)=(α6∣α7)=(α7∣α8)=(α4∣α2)=(α4∣α3)=(α3∣α1)=−1, (\alpha_4|\alpha_5) = (\alpha_5|\alpha_6) = (\alpha_6|\alpha_7) = (\alpha_7|\alpha_8) = (\alpha_4|\alpha_2) = (\alpha_4|\alpha_3) = (\alpha_3|\alpha_1) = -1,

and (αi∣αj)=0(\alpha_i|\alpha_j) = 0 for all other pairs of indices. Hence, the Dynkin graph of R is of type E_8, and R is irreducible.

(III) We have h=n8=30h = \frac{n}{8} = 30.

(IV) Let

α~=ε7+ε8=2α1+3α2+4α3+6α4+5α5+4α6+3α7+2α8, \tilde{\alpha} = \varepsilon_7 + \varepsilon_8 = 2\alpha_1 + 3\alpha_2 + 4\alpha_3 + 6\alpha_4 + 5\alpha_5 + 4\alpha_6 + 3\alpha_7 + 2\alpha_8,
which is a root. The sum of its coordinates with respect to (αi)(\alpha_i) is 29=h−129 = h - 1, so α~\tilde{\alpha} is the highest root. It is orthogonal to all the αi\alpha_i except α8\alpha_8, and (α~∣α8)=1(\tilde{\alpha}|\alpha_8) = 1. Hence, the completed Dynkin graph is:

!Dynkin graph of E_8

(V) Since (α∣α)=2(\alpha|\alpha) = 2 for all α∈R\alpha \in R, we have R−=RR^- = R.

For ΦR\Phi_R, the squared length of the roots is 130\frac{1}{30} (§ 1, no. 12). Hence, ΦR(x,y)=(x∣y)/60\Phi_R(x, y) = (x|y)/60 and γ(R)=900\gamma(R) = 900 (§ 1. no. 12, formula (20)).

(VI) Calculating the fundamental weights gives

ω1=2ε8=4α1+5α2+7α3+10α4+8α5+6α6+4α7+2α8ω2=12(ε1+ε2+ε3+ε4+ε5+ε6+ε7+5ε8)=5α1+8α2+10α3+15α4+12α5+9α6+6α7+3α8ω3=12(−ε1+ε2+ε3+ε4+ε5+ε6+ε7+7ε8)=7α1+10α2+14α3+20α4+16α5+12α6+8α7+4α8ω4=ε3+ε4+ε5+ε6+ε7+5ε8=10α1+15α2+20α3+30α4+24α5+18α6+12α7+6α8ω5=ε4+ε5+ε6+ε7+4ε8=8α1+12α2+16α3+24α4+20α5+15α6+10α7+5α8ω6=ε5+ε6+ε7+3ε8=6α1+9α2+12α3+18α4+15α5+12α6+8α7+4α8ω7=ε6+ε7+2ε8=4α1+6α2+8α3+2α4+10α5+8α6+6α7+3α8ω8=ε7+ε8=5α1+8α2+10α3+15α4+12α5+9α6+6α7+3α8=α~. \begin{align*} \omega_1 &= 2\varepsilon_8 = 4\alpha_1 + 5\alpha_2 + 7\alpha_3 + 10\alpha_4 + 8\alpha_5 + 6\alpha_6 + 4\alpha_7 + 2\alpha_8 \\ \omega_2 &= \frac{1}{2}(\varepsilon_1 + \varepsilon_2 + \varepsilon_3 + \varepsilon_4 + \varepsilon_5 + \varepsilon_6 + \varepsilon_7 + 5\varepsilon_8) \\ &= 5\alpha_1 + 8\alpha_2 + 10\alpha_3 + 15\alpha_4 + 12\alpha_5 + 9\alpha_6 + 6\alpha_7 + 3\alpha_8 \\ \omega_3 &= \frac{1}{2}(-\varepsilon_1 + \varepsilon_2 + \varepsilon_3 + \varepsilon_4 + \varepsilon_5 + \varepsilon_6 + \varepsilon_7 + 7\varepsilon_8) \\ &= 7\alpha_1 + 10\alpha_2 + 14\alpha_3 + 20\alpha_4 + 16\alpha_5 + 12\alpha_6 + 8\alpha_7 + 4\alpha_8 \\ \omega_4 &= \varepsilon_3 + \varepsilon_4 + \varepsilon_5 + \varepsilon_6 + \varepsilon_7 + 5\varepsilon_8 \\ &= 10\alpha_1 + 15\alpha_2 + 20\alpha_3 + 30\alpha_4 + 24\alpha_5 + 18\alpha_6 + 12\alpha_7 + 6\alpha_8 \\ \omega_5 &= \varepsilon_4 + \varepsilon_5 + \varepsilon_6 + \varepsilon_7 + 4\varepsilon_8 \\ &= 8\alpha_1 + 12\alpha_2 + 16\alpha_3 + 24\alpha_4 + 20\alpha_5 + 15\alpha_6 + 10\alpha_7 + 5\alpha_8 \\ \omega_6 &= \varepsilon_5 + \varepsilon_6 + \varepsilon_7 + 3\varepsilon_8 \\ &= 6\alpha_1 + 9\alpha_2 + 12\alpha_3 + 18\alpha_4 + 15\alpha_5 + 12\alpha_6 + 8\alpha_7 + 4\alpha_8 \\ \omega_7 &= \varepsilon_6 + \varepsilon_7 + 2\varepsilon_8 \\ &= 4\alpha_1 + 6\alpha_2 + 8\alpha_3 + 2\alpha_4 + 10\alpha_5 + 8\alpha_6 + 6\alpha_7 + 3\alpha_8 \\ \omega_8 &= \varepsilon_7 + \varepsilon_8 \\ &= 5\alpha_1 + 8\alpha_2 + 10\alpha_3 + 15\alpha_4 + 12\alpha_5 + 9\alpha_6 + 6\alpha_7 + 3\alpha_8 = \tilde{\alpha}. \end{align*}

(VII) Half the sum of the positive roots is the sum of the fundamental weights (§ 1, no. 10, Prop. 29); this gives

ρ=ε2+2ε3+3ε4+4ε5+5ε6+6ε7+23ε8=46α1+68α2+91α3+135α4+110α5+84α6+57α7+29α8. \begin{align*} \rho &= \varepsilon_2 + 2\varepsilon_3 + 3\varepsilon_4 + 4\varepsilon_5 + 5\varepsilon_6 + 6\varepsilon_7 + 23\varepsilon_8 \\ &= 46\alpha_1 + 68\alpha_2 + 91\alpha_3 + 135\alpha_4 + 110\alpha_5 + 84\alpha_6 + 57\alpha_7 + 29\alpha_8. \end{align*}

(VIII) The group Q(R) is generated by the εi±εj\varepsilon_i \pm \varepsilon_j and 12∑i=18εi\frac{1}{2} \sum_{i=1}^8 \varepsilon_i, and is equal to L_3 (no. 4). Hence P(R), which is associated to Q(R̄) = Q(R) = L_3, is L_3 (no. 4). The connection index is 1.

(IX) The family of exponents has 8 terms, and since h=30h = 30, the integers 1, 7, 11, 13, 17, 19, 23, 29, coprime to 30, must feature in this family; consequently, these are the exponents of W(R).

(X) From (IX) and Chap. V. § 6, no. 2, Cor. 1 of Prop. 3, it follows that the order of W(R) is

2.8.12.14.18.20.24.30=214.35.52.7. 2.8.12.14.18.20.24.30 = 2^{14}.3^5.5^2.7.

(XI) The only automorphism of the Dynkin graph is the identity since the three chains issuing from the ramification point have distinct lengths. Hence, A(R)=W(R)A(R) = W(R) and w0=−1w_0 = -1.

11. System of type e_7

(I) and (II) Let E=R8E = \mathbf{R}^8, and let R_8 be the root system in E constructed in no. 10. Let V be the hyperplane in E generated by the roots α1,…,α7\alpha_1, \ldots, \alpha_7 of R_8; it is orthogonal to the eighth fundamental weight ω=ε7+ε8\omega = \varepsilon_7 + \varepsilon_8 of R_8.

Let R=R8∩VR = R_8 \cap V. Then R is a reduced root system with basis (α1,…,α7)(\alpha_1, \ldots, \alpha_7), cf. § 1, no. 7, Cor. 4 of Prop. 20; hence, this system is of type E_7. Its elements are:

±εi±εj(1≤i≤j≤6),±(ε7−ε8), \pm \varepsilon_i \pm \varepsilon_j \quad (1 \leq i \leq j \leq 6), \quad \pm (\varepsilon_7 - \varepsilon_8),
±12(ε7−ε8+∑i=18(−1)ν(i)εi)with ∑i=18ν(i) odd. \pm \frac{1}{2} (\varepsilon_7 - \varepsilon_8 + \sum_{i=1}^8 (-1)^{\nu(i)} \varepsilon_i) \quad \text{with } \sum_{i=1}^8 \nu(i) \text{ odd}.

The number of roots is n=2+(62).4+26=126n = 2 + \binom{6}{2}.4 + 2^6 = 126. The positive roots are

±εi+εj(1≤i<j≤6),−ε7+ε8, \pm \varepsilon_i + \varepsilon_j \quad (1 \leq i < j \leq 6), \quad -\varepsilon_7 + \varepsilon_8,
12(−ε7+ε8+∑i=16(−1)ν(i)εi)with ∑i=16ν(i) odd. \frac{1}{2} (-\varepsilon_7 + \varepsilon_8 + \sum_{i=1}^6 (-1)^{\nu(i)} \varepsilon_i) \quad \text{with } \sum_{i=1}^6 \nu(i) \text{ odd}.

(III) We have h=nl=18h = \frac{n}{l} = 18.

(IV) Let α~=ε8−ε7=2α1+2α2+3α3+4α4+3α5+2α6+α7\tilde{\alpha} = \varepsilon_8 - \varepsilon_7 = 2\alpha_1 + 2\alpha_2 + 3\alpha_3 + 4\alpha_4 + 3\alpha_5 + 2\alpha_6 + \alpha_7, which is a root. The sum of its coordinates with respect to (αi)(\alpha_i) is 17 = h−1h - 1. It is therefore the highest root. It is orthogonal to αi\alpha_i for 2≤i≤72 \leq i \leq 7, and (α~∣α1)=1(\tilde{\alpha}|\alpha_1) = 1. The completed Dynkin graph is

!Dynkin graph for E_7

(V) Since (α∣α)=2(\alpha|\alpha) = 2 for all α∈R\alpha \in R, we have R−=RR^- = R. For ΦR\Phi_R, the squared length of the roots is 118\frac{1}{18}, so

ΦR(x,y)=(x∣y)/36,andγ(R)=22⋅34 \Phi_R(x, y) = (x|y)/36, \quad \text{and} \quad \gamma(R) = 2^2 \cdot 3^4
(§ 1. no. 12, formula (20)).

(VI) Calculating the fundamental weights gives

ω1=ε8−ε7=2α1+2α2+3α3+4α4+3α5+2α6+α7ω2=12(ε1+ε2+ε3+ε4+ε5+ε6−2ε7+2ε8)=12(4α1+7α2+8α3+12α4+9α5+8α6+3α7)ω3=12(−ε1+ε2+ε3+ε4+ε5+ε6−3ε7+3ε8)=3α1+4α2+6α3+8α4+6α5+4α6+2α7ω4=ε3+ε4+ε5+ε6+2(ε8−ε7)=4α1+6α2+8α3+12α4+9α5+6α6+3α7ω5=ε4+ε5+ε6+32(ε8−ε7)=12(6α1+9α2+12α3+18α4+15α5+10α6+5α7)ω6=ε5+ε6−ε7+ε8=2α1+3α2+4α3+6α4+5α5+4α6+2α7ω7=ε6+12(ε8−ε7)=12(2α1+3α2+4α3+6α4+5α5+4α6+3α7). \begin{align*} \omega_1 &= \varepsilon_8 - \varepsilon_7 = 2\alpha_1 + 2\alpha_2 + 3\alpha_3 + 4\alpha_4 + 3\alpha_5 + 2\alpha_6 + \alpha_7 \\ \omega_2 &= \frac{1}{2}(\varepsilon_1 + \varepsilon_2 + \varepsilon_3 + \varepsilon_4 + \varepsilon_5 + \varepsilon_6 - 2\varepsilon_7 + 2\varepsilon_8) \\ &= \frac{1}{2}(4\alpha_1 + 7\alpha_2 + 8\alpha_3 + 12\alpha_4 + 9\alpha_5 + 8\alpha_6 + 3\alpha_7) \\ \omega_3 &= \frac{1}{2}(-\varepsilon_1 + \varepsilon_2 + \varepsilon_3 + \varepsilon_4 + \varepsilon_5 + \varepsilon_6 - 3\varepsilon_7 + 3\varepsilon_8) \\ &= 3\alpha_1 + 4\alpha_2 + 6\alpha_3 + 8\alpha_4 + 6\alpha_5 + 4\alpha_6 + 2\alpha_7 \\ \omega_4 &= \varepsilon_3 + \varepsilon_4 + \varepsilon_5 + \varepsilon_6 + 2(\varepsilon_8 - \varepsilon_7) \\ &= 4\alpha_1 + 6\alpha_2 + 8\alpha_3 + 12\alpha_4 + 9\alpha_5 + 6\alpha_6 + 3\alpha_7 \\ \omega_5 &= \varepsilon_4 + \varepsilon_5 + \varepsilon_6 + \frac{3}{2}(\varepsilon_8 - \varepsilon_7) \\ &= \frac{1}{2}(6\alpha_1 + 9\alpha_2 + 12\alpha_3 + 18\alpha_4 + 15\alpha_5 + 10\alpha_6 + 5\alpha_7) \\ \omega_6 &= \varepsilon_5 + \varepsilon_6 - \varepsilon_7 + \varepsilon_8 \\ &= 2\alpha_1 + 3\alpha_2 + 4\alpha_3 + 6\alpha_4 + 5\alpha_5 + 4\alpha_6 + 2\alpha_7 \\ \omega_7 &= \varepsilon_6 + \frac{1}{2}(\varepsilon_8 - \varepsilon_7) \\ &= \frac{1}{2}(2\alpha_1 + 3\alpha_2 + 4\alpha_3 + 6\alpha_4 + 5\alpha_5 + 4\alpha_6 + 3\alpha_7). \end{align*}

(VII) The sum 2ρ2\rho of the positive roots is 2∑i=17ωi2 \sum_{i=1}^7 \omega_i (§ 1. no. 10. Prop. 29), so

2ρ=2ε2+4ε3+6ε4+8ε5+10ε6−17ε7+17ε8=34α1+49α2+66α3+96α4+75α5+52α6+27α7. \begin{align*} 2\rho &= 2\varepsilon_2 + 4\varepsilon_3 + 6\varepsilon_4 + 8\varepsilon_5 + 10\varepsilon_6 - 17\varepsilon_7 + 17\varepsilon_8 \\ &= 34\alpha_1 + 49\alpha_2 + 66\alpha_3 + 96\alpha_4 + 75\alpha_5 + 52\alpha_6 + 27\alpha_7. \end{align*}

(VIII) By no. 10 (VIII) and § 1, no. 10. Prop. 28, we have

Q(R)=Q(R8)∩V=L3∩VandP(R)=p(P(R8))=p(L3), Q(R) = Q(R_8) \cap V = L_3 \cap V \quad \text{and} \quad P(R) = p(P(R_8)) = p(L_3),
where pp denotes the orthogonal projection of EE onto VV. The group Q(R)Q(R) has basis (α1,…,α7)(\alpha_1, \ldots, \alpha_7); the group P(R)P(R) is generated by Q(R)Q(R) and
p(α8)=α8−12ω. p(\alpha_8) = \alpha_8 - \frac{1}{2}\omega.

We have ω∈P(R8)\omega \in P(R_8), 12ω∉P(R8)\frac{1}{2}\omega \notin P(R_8). so 2p(α8)∈Q(R)2p(\alpha_8) \in Q(R) and p(α8)∉Q(R)p(\alpha_8) \notin Q(R). Thus, P(R)/Q(R)P(R)/Q(R) is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z} and is generated by, for example, the image of ω7\omega_7.

The connection index is 2.

(IX) The sequence of exponents of W(R)W(R) has 7 terms. The numbers 1, 5, 7, 11, 13, 17, coprime to h=18h = 18, feature in this sequence. The last exponent mm must be such that m+m=18m + m = 18 (Chap. V, § 6, no. 2, formula (2)). Hence, the sequence of exponents is

1,5,7,9,11,13,17. 1, 5, 7, 9, 11, 13, 17.

(X) From (IX) and Chap. V, § 6, no. 2, Cor. 1 of Prop. 3, it follows that the order of W(R)W(R) is

2.6.8.10.12.14.18=210.34.5.7. 2.6.8.10.12.14.18 = 2^{10}.3^4.5.7.

(XI) The only automorphism of the Dynkin graph is the identity, so A(R)=W(R)A(R) = W(R) and w0=−1w_0 = -1.

(XII) P(R−)/Q(R−)P(R^-)/Q(R^-) has only one non-identity element. It interchanges the vertices corresponding to α0\alpha_0 and α7\alpha_7, α1\alpha_1 and α6\alpha_6, α3\alpha_3 and α5\alpha_5, and leaves α2\alpha_2 and α4\alpha_4 fixed.

12. System of type e_6

(I) and (II) Let E=R8E = \mathbf{R}^8, and let R8R_8 be the root system in EE constructed in no. 10. Let VV be the vector subspace of EE generated by the roots α1,…,α6\alpha_1, \ldots, \alpha_6 of R8R_8; this is the orthogonal complement of the plane generated by the last two fundamental weights ω=ε7+ε8\omega = \varepsilon_7 + \varepsilon_8 and π=ε6+ε7+2ε8\pi = \varepsilon_6 + \varepsilon_7 + 2\varepsilon_8 of R8R_8.

Let R=R8∩VR = R_8 \cap V. This is a reduced root system with basis (α1,…,α6)(\alpha_1, \ldots, \alpha_6), and hence of type E6E_6. Its elements are:

±εi±εj(1≤i<j≤5), \pm \varepsilon_i \pm \varepsilon_j \quad (1 \leq i < j \leq 5),
±12(ε8−ε7−ε6+∑i=15(−1)ν(i)εi) with ∑i=15ν(i) even. \pm \frac{1}{2} (\varepsilon_8 - \varepsilon_7 - \varepsilon_6 + \sum_{i=1}^5 (-1)^{\nu(i)} \varepsilon_i) \text{ with } \sum_{i=1}^5 \nu(i) \text{ even}.

The number of roots is n=(52).4+25=72n = \binom{5}{2}.4 + 2^5 = 72. The positive roots are

±εi+εj(1≤i<j≤5), \pm \varepsilon_i + \varepsilon_j \quad (1 \leq i < j \leq 5),
12(ε8−ε7−ε6+∑i=15(−1)ν(i)εi) with ∑i=15ν(i) even. \frac{1}{2} (\varepsilon_8 - \varepsilon_7 - \varepsilon_6 + \sum_{i=1}^5 (-1)^{\nu(i)} \varepsilon_i) \text{ with } \sum_{i=1}^5 \nu(i) \text{ even}.

(III) We have h=n6=12h = \frac{n}{6} = 12.

(IV) Let

α~=12(ε1+ε2+ε3+ε4+ε5−ε6−ε7+ε8) \tilde{\alpha} = \frac{1}{2} (\varepsilon_1 + \varepsilon_2 + \varepsilon_3 + \varepsilon_4 + \varepsilon_5 - \varepsilon_6 - \varepsilon_7 + \varepsilon_8)
=α1+2α2+2α3+3α4+2α5+α6, = \alpha_1 + 2\alpha_2 + 2\alpha_3 + 3\alpha_4 + 2\alpha_5 + \alpha_6,

which is a root. The sum of its coordinates with respect to (αi)(\alpha_i) is 11=h−111 = h - 1, so α~\tilde{\alpha} is the highest root. It is orthogonal to α1,α3,α4,α5,α6\alpha_1, \alpha_3, \alpha_4, \alpha_5, \alpha_6, and (α~∣α2)=1(\tilde{\alpha}|\alpha_2) = 1. The completed Dynkin graph is

!Dynkin graph

(V) Since (α∣α)=2(\alpha|\alpha) = 2 for all α∈R\alpha \in R, we have R′=RR' = R. For ΦR\Phi_R, the squared length of the roots is 112\frac{1}{12}, so

ΦR(x,y)=(x∣y)/24,andγ(R)=144. \Phi_R(x, y) = (x|y)/24, \quad \text{and} \quad \gamma(R) = 144.

(VI) Calculating the fundamental weights gives:

ω1=23(ε8−ε7−ε6)=13(4α1+3α2+5α3+6α4+4α5+2α6)ω2=12(ε1+ε2+ε3+ε4+ε5−ε6−ε7+ε8)=α1+2α2+2α3+3α4+2α5+α6=α~ω3=56(ε8−ε7−ε6)+12(−ε1+ε2+ε3+ε4+ε5)=13(5α1+6α2+10α3+12α4+8α5+4α6)ω4=ε3+ε4+ε5−ε6−ε7+ε8=2α1+3α2+4α3+6α4+4α5+2α6ω5=23(ε8−ε7−ε6)+ε4+ε5=13(4α1+6α2+8α3+12α4+10α5+5α6)ω6=13(ε8−ε7−ε6)+ε5=13(2α1+3α2+4α3+6α4+5α5+4α6). \begin{align*} \omega_1 &= \frac{2}{3}(\varepsilon_8 - \varepsilon_7 - \varepsilon_6) = \frac{1}{3}(4\alpha_1 + 3\alpha_2 + 5\alpha_3 + 6\alpha_4 + 4\alpha_5 + 2\alpha_6) \\ \omega_2 &= \frac{1}{2}(\varepsilon_1 + \varepsilon_2 + \varepsilon_3 + \varepsilon_4 + \varepsilon_5 - \varepsilon_6 - \varepsilon_7 + \varepsilon_8) \\ &= \alpha_1 + 2\alpha_2 + 2\alpha_3 + 3\alpha_4 + 2\alpha_5 + \alpha_6 = \tilde{\alpha} \\ \omega_3 &= \frac{5}{6}(\varepsilon_8 - \varepsilon_7 - \varepsilon_6) + \frac{1}{2}(-\varepsilon_1 + \varepsilon_2 + \varepsilon_3 + \varepsilon_4 + \varepsilon_5) \\ &= \frac{1}{3}(5\alpha_1 + 6\alpha_2 + 10\alpha_3 + 12\alpha_4 + 8\alpha_5 + 4\alpha_6) \\ \omega_4 &= \varepsilon_3 + \varepsilon_4 + \varepsilon_5 - \varepsilon_6 - \varepsilon_7 + \varepsilon_8 \\ &= 2\alpha_1 + 3\alpha_2 + 4\alpha_3 + 6\alpha_4 + 4\alpha_5 + 2\alpha_6 \\ \omega_5 &= \frac{2}{3}(\varepsilon_8 - \varepsilon_7 - \varepsilon_6) + \varepsilon_4 + \varepsilon_5 \\ &= \frac{1}{3}(4\alpha_1 + 6\alpha_2 + 8\alpha_3 + 12\alpha_4 + 10\alpha_5 + 5\alpha_6) \\ \omega_6 &= \frac{1}{3}(\varepsilon_8 - \varepsilon_7 - \varepsilon_6) + \varepsilon_5 \\ &= \frac{1}{3}(2\alpha_1 + 3\alpha_2 + 4\alpha_3 + 6\alpha_4 + 5\alpha_5 + 4\alpha_6). \end{align*}

(VII) Half the sum of the positive roots is ∑i=16ωi\sum_{i=1}^6 \omega_i, so

ρ=ε2+2ε3+3ε4+4ε5+4(ε8−ε7−ε6)=8α1+11α2+15α3+21α4+15α5+8α6. \begin{align*} \rho &= \varepsilon_2 + 2\varepsilon_3 + 3\varepsilon_4 + 4\varepsilon_5 + 4(\varepsilon_8 - \varepsilon_7 - \varepsilon_6) \\ &= 8\alpha_1 + 11\alpha_2 + 15\alpha_3 + 21\alpha_4 + 15\alpha_5 + 8\alpha_6. \end{align*}

(VIII) By no. 10 (VIII) and § 4, no. 10, Prop. 28,

Q(R)=Q(R8)∩V=L3∩VandP(R)=p(P(R8))=p(L3), Q(R) = Q(R_8) \cap V = L_3 \cap V \quad \text{and} \quad P(R) = p(P(R_8)) = p(L_3),

where pp denotes the orthogonal projection of EE onto VV. We have

p(α7)=α7−23π+ω,p(α8)=α8+π−2ω. p(\alpha_7) = \alpha_7 - \frac{2}{3}\pi + \omega, \quad p(\alpha_8) = \alpha_8 + \pi - 2\omega.
The group Q(R)Q(R) has basis (α1,…,α6)(\alpha_1, \ldots, \alpha_6). The group P(R)P(R) is generated by Q(R)Q(R) and p(α7)p(\alpha_7), since p(α8)∈P(R8)∩V=Q(R8)∩V=Q(R)p(\alpha_8) \in P(R_8) \cap V = Q(R_8) \cap V = Q(R). We have 3p(α7)∈Q(R)3p(\alpha_7) \in Q(R) and p(α7)∉Q(R)p(\alpha_7) \notin Q(R). Hence, the group P(R)/Q(R)P(R)/Q(R) is isomorphic to Z/3Z\mathbf{Z}/3\mathbf{Z}; it is generated, for example, by the image of ω6\omega_6.

The connection index is 3.

(IX) and (X) By § 2, no. 4, Prop. 7, the order of the Weyl group is 6!1.2.2.3.2.1.3=27.34.56!1.2.2.3.2.1.3 = 2^7.3^4.5. The sequence of exponents has 6 terms between 1 and 11, and contains the integers 1, 5, 7, 11 which are coprime to 12. The other exponents m,m′m, m' are integers such that

m+m′=12, m + m' = 12,
(m+1)(m′+1)(1+1)(5+1)(7+1)(11+1)=27.34.5, (m + 1)(m' + 1)(1 + 1)(5 + 1)(7 + 1)(11 + 1) = 2^7.3^4.5,
in view of Chap. V, § 6, no. 2, formula (2) and Cor. 1 of Prop. 3. The second relation gives (m+1)(m′+1)=45(m + 1)(m' + 1) = 45, and since m+m′+2=14m + m' + 2 = 14, we obtain m=4,m′=8m = 4, m' = 8. Hence, the sequence of exponents is
1,4,5,7,8,11. 1, 4, 5, 7, 8, 11.

(XI) and (XII) Since the roots all have the same length, the automorphisms of the Dynkin graph are those of the underlying graph. Apart from the identity, there is only the automorphism ε\varepsilon which transforms α1,α3,α4,α5,α6,α2\alpha_1, \alpha_3, \alpha_4, \alpha_5, \alpha_6, \alpha_2 into α6,α5,α4,α3,α1,α2\alpha_6, \alpha_5, \alpha_4, \alpha_3, \alpha_1, \alpha_2, respectively. Hence, A(R)/W(R)A(R)/W(R) is isomorphic to Z/2Z\mathbf{Z}/2\mathbf{Z}; since −1∈W(R)-1 \in W(R) (Chap. V, § 6, no. 2, Cor. 3 of Prop. 3), A(R)A(R) is isomorphic to W(R)×{1,−1}W(R) \times \{1, -1\} and w0w_0 can be identified with −ε-\varepsilon. It follows that the non-identity element of A(R)/W(R)A(R)/W(R) defines the automorphism x↦−xx \mapsto -x of P(R−)/Q(R−)P(R^-)/Q(R^-).

Moreover, P(R−)/Q(R−)P(R^-)/Q(R^-) has two non-identity elements of order 3. They define the two automorphisms of order 3 of the completed Dynkin graph.

13. System of type g_2

(I) Let EE be the hyperplane in R3\mathbf{R}^3 with equation

ξ1+ξ2+ξ3=0. \xi_1 + \xi_2 + \xi_3 = 0.
Let RR be the set of α∈L0∩V\alpha \in L_0 \cap V such that (α∣α)=2(\alpha|\alpha) = 2 or (α∣α)=6(\alpha|\alpha) = 6. The elements of RR are
±(ε1−ε2),±(ε1−ε3),±(ε2−ε3),±(2ε1−ε2−ε3), \pm (\varepsilon_1 - \varepsilon_2), \quad \pm (\varepsilon_1 - \varepsilon_3), \quad \pm (\varepsilon_2 - \varepsilon_3), \quad \pm (2\varepsilon_1 - \varepsilon_2 - \varepsilon_3),
±(2ε2−ε1−ε3),±(2ε3−ε1−ε2). \pm (2\varepsilon_2 - \varepsilon_1 - \varepsilon_3), \quad \pm (2\varepsilon_3 - \varepsilon_1 - \varepsilon_2).

Then, R generates V, and 2(α∣β)(β∣β)∈Z\frac{2(\alpha|\beta)}{(\beta|\beta)} \in \mathbf{Z} for all α,β∈R\alpha, \beta \in R: this is clear if β=±(εi−εj)\beta = \pm (\varepsilon_i - \varepsilon_j) with i≠ji \neq j; if β=2ε1−ε2−ε3\beta = 2\varepsilon_1 - \varepsilon_2 - \varepsilon_3 for example, we have (α∣β)∈3Z(\alpha|\beta) \in 3\mathbf{Z}, and again our assertion holds. Hence, R is a reduced root system in V. The number of roots is n=12n = 12.

(II) Put α1=ε1−ε2,α2=−2ε1+ε2+ε3\alpha_1 = \varepsilon_1 - \varepsilon_2, \alpha_2 = -2\varepsilon_1 + \varepsilon_2 + \varepsilon_3. Then the roots are

±α1,±(α1+α2),±(2α1+α2),±α2, \pm \alpha_1, \quad \pm (\alpha_1 + \alpha_2), \quad \pm (2\alpha_1 + \alpha_2), \quad \pm \alpha_2,
±(3α1+α2),±(3α1+2α2). \pm (3\alpha_1 + \alpha_2), \quad \pm (3\alpha_1 + 2\alpha_2).

Hence, (α1,α2)(\alpha_1, \alpha_2) is a basis of R. We have ∥α1∥2=2,∥α2∥2=6,(α1∣α2)=−3\| \alpha_1 \| ^2 = 2, \| \alpha_2 \| ^2 = 6, (\alpha_1|\alpha_2) = -3, so R is a system of type G_2. The positive roots are α1,α1+α2,2α1+α2,3α1+α2,3α1+2α2\alpha_1, \alpha_1 + \alpha_2, 2\alpha_1 + \alpha_2, 3\alpha_1 + \alpha_2, 3\alpha_1 + 2\alpha_2.

(III) We have h=n2=6h = \frac{n}{2} = 6.

(IV) The highest root is α~=3α1+2α2=−ε1−ε2+2ε3\tilde{\alpha} = 3\alpha_1 + 2\alpha_2 = -\varepsilon_1 - \varepsilon_2 + 2\varepsilon_3. We have (α~∣α1)=0,(α~∣α2)=3(\tilde{\alpha}|\alpha_1) = 0, (\tilde{\alpha}|\alpha_2) = 3. The completed Dynkin graph is

!Dynkin graph

(V) The inverse system is the following set of vectors:

±α1,±(α1+α2),±(2α1+α2),±13α2, \pm \alpha_1, \quad \pm (\alpha_1 + \alpha_2), \quad \pm (2\alpha_1 + \alpha_2), \quad \pm \frac{1}{3}\alpha_2,
±13(3α1+α2),±13(3α1+2α2). \pm \frac{1}{3}(3\alpha_1 + \alpha_2), \quad \pm \frac{1}{3}(3\alpha_1 + 2\alpha_2).

There are 10 roots not orthogonal to α1\alpha_1; we have n(β,α1)=±1n(\beta, \alpha_1) = \pm 1 for 4 of these roots, n(β,α1)=±3n(\beta, \alpha_1) = \pm 3 for 4 others, and n(β,α1)=±2n(\beta, \alpha_1) = \pm 2 for β=±α1\beta = \pm \alpha_1. Hence, the squared length of α1\alpha_1 for ΦR\Phi_R is 4(4.1+4.9+2.4)−1=1124(4.1 + 4.9 + 2.4)^{-1} = \frac{1}{12}. Hence, ΦR(x,y)=(x∣y)/24\Phi_R(x, y) = (x|y)/24. We now apply formula (18) of § 1, no. 12, with x=y=α1x = y = \alpha_1; this gives

2+4.14+4.14=γ(R).112 2 + 4.\frac{1}{4} + 4.\frac{1}{4} = \gamma(R).\frac{1}{12}

so γ(R)=48\gamma(R) = 48.

(VI) and (VII) Half the sum of the positive roots is

ρ=5α1+3α2. \rho = 5\alpha_1 + 3\alpha_2.

The fundamental weights ω1\omega_1 and ω2\omega_2 are orthogonal to α2\alpha_2 and α1\alpha_1, hence proportional to 2α1+α22\alpha_1 + \alpha_2 and 3α1+2α23\alpha_1 + 2\alpha_2. We have

ω1+ω2=ρ=5α1+3α2=(2α1+α2)+(3α1+2α2). \omega_1 + \omega_2 = \rho = 5\alpha_1 + 3\alpha_2 = (2\alpha_1 + \alpha_2) + (3\alpha_1 + 2\alpha_2).

Hence,

ω1=2α1+α2,ω2=3α1+2α2=α~. \omega_1 = 2\alpha_1 + \alpha_2, \quad \omega_2 = 3\alpha_1 + 2\alpha_2 = \tilde{\alpha}.

(VIII) Q(R) is generated by ε1−ε2\varepsilon_1 - \varepsilon_2 and ε1−ε3\varepsilon_1 - \varepsilon_3, for example. By (VI) and (VII), P(R) = Q(R). The connection index is 1.

(IX) The family of exponents has 2 terms; since 1 and h−1=5h - 1 = 5 are exponents, they are the only ones.

(X) We have (α1,α2‾)=5π6(\overline{\alpha_1, \alpha_2}) = \frac{5\pi}{6}, so W(R) is isomorphic to the dihedral group of order 12.

(XI) The only automorphism of the Dynkin diagram is the identity, so Λ(R)=W(R)\Lambda(R) = W(R) and w0=−1w_0 = -1.

14. Irreducible non-reduced root systems

The irreducible, non-reduced root systems can be obtained from the irreducible, reduced systems by using Props. 13 and 14 of § 1. no. 4. For each integer l≥1l \geq 1, there exists, up to isomorphism, a unique irreducible, non-reduced root system of rank ll: let R be a root system of type B_l, A the set of shortest roots of R; take the union of R and 2A. With the notation of no. 5, we obtain the 2l(l+1)2l(l+1) vectors

±εi, ±2εi, εi±εj (i<j). \pm \varepsilon_i,\ \pm 2\varepsilon_i,\ \varepsilon_i \pm \varepsilon_j\ (i < j).

Exercises

If R is a root system, denote by W+(R)W^+(R) the set of elements of W(R)W(R) of determinant 1.

See the exercises for § 4.

Transcribed from the printed volume. Not translated.