§ 1. The Lie algebra (2) and its representations
1. Canonical basis of (2)
Lemma 1 00XS
Let A be an associative algebra over and elements of A such that .
(i) for any integer .
(ii) If is an element of A such that , then, for any integer ,
The map from A to A is a derivation, which implies (i). With the assumptions in (ii),
On the other hand, by (i). Q.E.D.
Recall that we denote by the Lie algebra consisting of the square matrices of order 2, trace zero, and with entries in . This Lie algebra is simple of dimension 3 (Chap. I, §6, no. 7, Example). The canonical basis of is the basis , where
0 0
0 0 0 0 .
We have
Since the identity representation of is injective, is a semi-simple element of and are nilpotent elements of (Chap. I, §6, no. 3, Th. 3). By Chap. VII, §2, no. 1, Example is a Cartan subalgebra of . The map is an involutive automorphism of the Lie algebra , called the canonical involution of ; it transforms into .
The first and third relations follow from Lemma 1. The others can be deduced from them by using the canonical involution of .
2. Primitive elements of (2)-modules
Let E be an )-module. If and , we shall often write instead of . Let . If we say, by abuse of language, that is an element of E of weight , or that is the weight of . If E is finite dimensional, is semi-simple, so the set of elements of weight is the primary subspace of E relative to and (cf. Chap. VII, §1, no. 1).
Lemma 3 00XU
If is an element of weight , then is an element of weight and is an element of weight .
Indeed, , and similarly (cf. also Chap. VII, §1, no. 3, Prop. 10 (ii)).
Definition 1 00XV
Let E be an -module. An element of E is said to be primitive if it is a non-zero eigenvector of and belongs to the kernel of .
A non-zero element of E is primitive if and only if is stable under the operation of ; this follows for example from Lemma 3.
Examples The element is primitive of weight 2 for the adjoint representation of . The element of is primitive of weight 1 for the identity representation of on .
Lemma 4 00XW
Let E be a non-zero finite dimensional -module. Then E has primitive elements.
Since is a nilpotent element of is nilpotent. Assume that and = 0. By Lemma 2,
and hence the elements of -- are primitive.
Proposition 1 00XX
Let E be an -module, and a primitive element of E of weight . Put for , and . Then
The first formula follows from Lemma 3, and the second from the definition of the . We prove the third by induction on . It is satisfied for since . If ,
Corollary 00XY
The submodule of E generated by is the vector subspace generated by the .
This follows from the formulas (2).
The integers such that constitute an interval in , and the corresponding elements form a basis over of the submodule generated by (indeed, they are linearly independent because they are non-zero elements of distinct weights). This basis will be said to be associated to the primitive element .
Proposition 2 00XZ
If the submodule V of E generated by the primitive element is finite dimensional, then:
(i) the weight of is integral and equal to dim ;
(ii) is a basis of V, and for ;
(iii) the eigenvalues of are ; they are all of multiplicity 1;
(iv) every primitive element of V is proportional to ;
(v) the commutant of the module V is reduced to the scalars; in particular, V is absolutely simple.
Let be the largest integer such that . Then , so ; since is a basis of V, this proves (i) and (ii). Assertion (iii) follows from the equality . We have for , hence (iv). Let be an element of the commutant of the module V. Then , so there exists such that ; then
for all , so , proving (v).
Corollary 00Y0
Let E be a finite dimensional -module.
(i) The endomorphism is diagonalizable and its eigenvalues are rational integers.
(ii) For any , let be the eigenspace of corresponding to the eigenvalue . Let be an integer . The map is injective for , bijective for , and surjective for . The map is injective for , bijective for , and surjective for .
(iii) The length of E is equal to dim Ker and to dim Ker.
(iv) Let (resp. ) be the sum of the for even (resp. odd). Then (resp. ) is the sum of the simple submodules of E of odd (resp. even) dimension; and . The length of is dim , and that of is dim .
(v) Ker Im and Ker Im.
If E is simple, E is generated by a primitive element (Lemma 4), and it suffices to apply Propositions 1 and 2. The general case follows since every finite dimensional )-module is semi-simple.
3. The simple modules v()
Let be the canonical basis of . For the identity representation of ,
Consider the symmetric algebra of Algebra, Chap. III, §6, no. 1, Def. 1). The elements of extend uniquely to derivations of , giving the structure of an )-module (Chap. I, §3, no. 2). Let be the set of homogeneous elements of of degree . Then is an )-submodule of of dimension , the th symmetric power of (Chap. III, Appendix). If are integers such that , put
Proposition 3 00Y1
For any integer , is an absolutely simple -module. In this module, is primitive of weight .
We have and , so is primitive of weight . The submodule of generated by is of dimension (Prop. 2 (i)) and so is equal to . By Prop. 2 (v), is absolutely simple.
Theorem 1 00Y2
Every simple -module of finite dimension is isomorphic to . Every finite dimensional -module is a direct sum of submodules isomorphic to the modules .
This follows from Lemma 4 and Prop. 1, 2 and 3.
Remark 1 00Y3
The adjoint representation of defines on the structure of a simple )-module. This module is isomorphic to V(2) by an isomorphism that takes to to , and to .
Remark 3 00Y5
Let be the bilinear form on such that
if
If and , then . It is now easy to check that is invariant, and that is symmetric for even, and alternating for odd.
Proposition 4 00Y6
Let E be a finite dimensional -module, an integer , the set of primitive elements of weight . Let L be the vector space of homomorphisms from the -module to the -module E. The map from L to E is linear, injective, and its image is .
This map is clearly linear, and it is injective because generates the )-module . If ,
so . Let , and V the submodule of E generated by . By Prop. 1, there exists an isomorphism from the module to the module V that takes to . Then .
Corollary 00Y7
The isotypical component of E of type has length
dim(P.
4. Linear representations of the group sl(2)
Recall (Algebra, Chap. III, §8, no. 9) that we denote by the group of square matrices of order 2 with coefficients in whose determinant is equal to 1. If is nilpotent, then Algebra, Chap. VII, §5, Cor. 3 of Prop. 5) and . If E is a finite dimensional vector space and is a linear representation of on E, then is nilpotent and so is defined (Chap. I, §6, no. 3).
Definition 2 00Y8
Let E be a finite dimensional vector space, and (resp. ) a linear representation of (resp. ) on E. Then and are said to be compatible if, for every nilpotent element of .
In other words, and are compatible if, for every nilpotent element of , the restriction of to is compatible with the restriction of to the group (Chap. VII, §3, no. 1).
If and are compatible, so are the dual representations, the th tensor powers, and the th symmetric powers of and , respectively (Chap. VII, §5, no. 4, Lemma 1 (i) and (ii)). Similarly for the representations induced by and on a vector subspace stable under and loc. cit.).
In particular, the representation of on (no. 3) is compatible with the th symmetric power of the identity representation of . Putting as above, we have
= (3)
for and .
Theorem 2 00Y9
Let be a linear representation of on a finite dimensional vector space E.
(i) There exists a unique linear representation of on E that is compatible with .
(ii) A vector subspace F of E is stable under if and only if it is stable under .
(iii) Let . Then for all if and only if is invariant under that is, for all .
The existence of follows from the preceding and Th. 1. On the other hand, we know that the group is generated by the elements of the form
=
0 1 1
where Algebra, Chap. III, §8, no. 9, Prop. 17). This proves the uniqueness of .
Assertions (ii) and (iii) follow from what we have said, together with Chap. VII, §3, no. 1, Lemma 1 (i). Q.E.D.
Every finite dimensional )-module therefore has a unique -module structure, which is said to be associated to its )-module structure.
Remark 00YA
When is or or a complete non-discrete ultrametric field, is the Lie algebra of . Let and be as in Th. 2. The homomorphism is a homomorphism of Lie groups from to this is clear when , and the general case follows, in view of Th. 1. By Chap. VII, §3, no. . Hence (for a converse, see Exerc. 18).
Proposition 5 00YB
Let E, F be finite dimensional -modules, and let Hom. The following conditions are equivalent:
(i) is a homomorphism of -modules;
(ii) is a homomorphism of -modules.
Condition (i) means that is an invariant element of the )-module Hom, and condition (ii) means that is an invariant element of the )-module Hom. Since these module structures are associated by Chap. VII, §5, no. 4, Lemma 1 (iii), the proposition follows from Th. 2 (iii).
Definition 3 00YC
The adjoint representation of the group is the linear representation Ad of on defined by
Ad()
for all and all . When is or or a complete non-discrete ultrametric field, we recover Def. 7 of Chap. III, §3, no. 12 (cf. loc. cit., Prop. 49).
By Chap. VII, §5, no. 4, Lemma 1 (i) and (ii), the adjoint representations of and are compatible. By Chap. VII, §3, no. 1, Remark 2, Ad() Aut.
5. Some elements of sl(2)
For any , put
1
= 0 1 1 0 1
0 t)
= 0
With the notations of no. 3,
so
Hence, the element 0 operates by on . If
0
E is an odd-dimensional simple )-module, is thus an involutive automorphism of the vector space E. In particular, taking E to be the adjoint representation:
so that is the canonical involution of .
For any , put
Then , so
Proposition 6 01L4
Let E be a finite dimensional -module, and . Let be the set of elements of E of weight .
(i) is a bijection from to .
(ii) is the homothety with ratio on .
If , the proposition follows from formulas (4) and (6). The general case follows from Th. 1.
Corollary 00YD
Let be the decomposition of E defined in the Cor. of Prop. 2. The element of operates by +1 on
0
and by on .
This follows from (ii), applied to .
Exercises
The base field is assumed to be of characteristic zero.
Unless explicitly stated otherwise, Lie algebras are assumed to be finite dimensional.
We denote by the Lie algebra .
See the exercises for § 1.