§ 3. Representations
1. Representations
Definition 1
Let be a Lie algebra over and a -module. A homomorphism of into the Lie Algebra is called a representation of on the module . An injective representation is called faithful. If is a field, the dimension (finite or infinite) of over is called the dimension of the representation. The representation of on the -module is called the adjoint representation of .
A representation of on is thus a -linear mapping of into the endomorphism module of such that
for all .
Example
Let G be a real Lie group, g its Lie algebra and θ an analytic representation of G on a finite-dimensional real vector space E. Then the corresponding homomorphism of g into gl(E) is a representation of g on E.
Let U be the enveloping algebra of g. Proposition 1 of § 2, no. 1 defines a one-to-one correspondence between the set of representations of g on M and the set of representations of U on M. On the other hand we know (Algebra, Chapter VIII, § 13, no. 1) that there is an equivalence between the notion of representation of the associative algebra U and that of left U-module.
Definition 2
Let g be a Lie algebra over K and U its enveloping algebra. A unitary left module over U is called a left g-module, or simply a g-module.
If M is a g-module and x ∈ U, x_M will denote the homothety of M defined by x (cf. Algebra, Chapter VIII, § 1, no. 2).
A unitary right module over U is called a right g-module. Such a module is identified with a left U^0-module, that is (§ 2, no. 4) with a left g^0-module.
Let φ be the principal antiautomorphism of U. If M is a right g-module, a left g-module structure is defined on M by writing a.m = m.φ(a) for m ∈ M and a ∈ U.
The notions and results of the theory of modules can be translated into the language of representations:
(1) Two representations ρ and ρ' of g on M and M' are called similar or isomorphic if the g-modules M and M' are isomorphic. For this it is necessary and sufficient that there exist an isomorphism u of the K-module M onto the K-module M' such that
for all x ∈ g.
(2) For all i ∈ I, let ρ_i be a representation of g on M_i. Let M be the g-module the direct sum of the g-modules M_i. There is a corresponding representation ρ of g on M, called the direct sum of the ρ_i and denoted by (or in the case of n representations ). If is an element of M and x ∈ g, then .
(3) A representation ρ of g on M is called simple or irreducible if the associated g-module is simple. It amounts to the same to say that there exists no sub-K-module of M (other than {0} and M) stable under all the . A class of simple g-modules (Algebra, Chapter VIII, § 3, no. 2) defines a class of simple representations of g.
(4) A representation ρ of g on M is called semi-simple or completely reducible if the associated g-module is semi-simple. It amounts to the same to say that ρ is similar to a direct sum of simple representations or that every sub-K-module of
M stable under the () has a supplement stable under the () (cf. Algebra, Chapter VIII, § 3, no. 3).
(5) Let be a class of simple representations of corresponding to a class C of simple -modules. On the other hand let be a representation of on M. The isotypical component of species C of the -module M (Algebra, Chapter VIII, § 3, no. 4) is also called the isotypical component of M of species . This component is the sum of the sub-K-modules of M stable under the and on which the induce a representation of class ; it is the direct sum of certain of these submodules; if is of length , is said to contain n times. The sum of the different is direct; it is equal to M if and only if is semi-simple.
(6) Let be two representations of . is called a subrepresentation (resp. quotient representation) of if the module of is a submodule (resp. quotient module) of the module of .
Let M be a K-module. The zero representation of on M defines on M a -module structure. With this structure M is called a trivial -module.
Let M be a -module. The quotient -modules of the sub--modules of M are also the sub--modules of the quotient modules of M: they are obtained by considering two sub--modules U, of M such that and forming the -module . Then if all the simple modules of the above type are isomorphic to a given simple -module N, M is called a pure -module of species N. If and are the representations of corresponding to M and N, we also say that is pure of species .
Let be a sub--module of M. For M to be pure of species N, it is necessary and sufficient that and be pure of species N. For the condition is obviously necessary. Suppose that it holds and let U, be sub--modules of M such that and is simple; let be the canonical homomorphism of M onto ; if , is isomorphism to and hence isomorphic to N; if , then , hence is isomorphic to a simple submodule of and the latter module is itself isomorphic to ; hence is again isomorphic to N, so that M is pure of species N.
Henceforth let M be a -module and suppose that the set of sub--modules of M which are pure of species N admits a maximal element . Then every submodule of M which is pure of species N is contained in . For and are pure of species N, hence is pure of species N by the above and hence .
Suppose that the -module M admits a Jordan-Hölder series . For M to be pure of species N, it is necessary and sufficient that be isomorphic to N; for the condition is obviously necessary and its sufficiency follows immediately by induction on from what we have seen above.
Proposition 1
Let g be a Lie algebra over K and a an ideal of g. Let M be a g-module* and a simple -module. Consider as an -module and suppose that the set of sub--modules of which are pure of species admits a maximal element . Then is a sub--module of .
Let . Let be the canonical mapping of onto and the mapping of into . It suffices to show that . Let . Then, for ,
Now , whence ; on the other hand,
Hence . It follows that is a sub--module of isomorphic to a quotient of and hence pure of species ; hence .
Corollary
Let be a Lie algebra over and an ideal of . Let be a simple -module, of finite length as a -module. There exists a simple -module such that is a pure -module of species .
Since the -module is of finite length, there exists a minimal element in the set of sub--modules of : it is a simple sub--module of . The largest sub--module of which is pure of species is therefore and is a sub--module of (Proposition 1) and is therefore identical with .
2. Tensor product of representations
We have defined in no. 1 the direct sum of a family of representations of . We shall now define other operations on representations.
Let be two Lie algebras over and a -module (). Let be the enveloping algebra of and the canonical mapping of into . Then is a left -module and hence has a canonical left -module structure. Now is the enveloping algebra of and the mapping is the canonical mapping of into this enveloping algebra (§ 2, no. 2). Hence there exists a -module structure on such that:
This structure defines a representation of on .
If now , the homomorphism of into , composed with the above representation, defines a representation of on and hence a -module structure on such that:
By an analogous argument we see that:
Proposition 2
Let be a Lie algebra over and a -module (). On the tensor product , there exists one and only one -module structure such that
for all .
The corresponding representation is called the tensor product of the given representations of on the .
In particular, if is a -module, Proposition 2 defines a -module structure on each and hence on the tensor algebra of .
Formula (3) shows that, for all is the unique derivation of the algebra which extends . We know (§ 2, no. 8) that defines on passing to the quotient a derivation of the symmetric algebra of . Hence can be considered as a quotient -module of and the are derivations of .
Still more particularly, consider as a -module by means of the adjoint representation of . Let be the enveloping algebra of . By Proposition 7 of § 2, defines on passing to the quotients a derivation of which is just the inner derivation defined by ( denoting the canonical mapping of into ). Then can be considered as a quotient -module of . If is a field of characteristic 0, the canonical isomorphism of onto is a -module isomorphism (§ 2, no. 8).
3. Representations on homomorphism modules
Again let and be two Lie algebras over and a -module (). Let be the enveloping algebra of and the canonical mapping of into . Then is a left -module and hence has a canonical left -module structure. Now is the enveloping algebra of and the mapping
is the canonical mapping of into this enveloping algebra. Hence there exists a -module structure on such that
for all . This structure defines a representation of on .
If now , the homomorphism of into , composed with the above representation, defines a representation of on and hence a -module structure on such that
or
Combining these results with Proposition 2, we see that:
Proposition 3
Let be a Lie algebra over and a -module (). Let be the -module of multilinear mappings of into . There exists one and only one -module structure on such that
for all and ().
In particular, let be a Lie algebra over and a -module and consider as a trivial -module. Proposition 3 defines a -module structure on . The corresponding representation is called the dual representation of the representation . We have:
for all . In other words:
When is a field and is finite-dimensional, the -module is simple (resp. semi-simple) if and only if the -module is simple (resp. semi-simple).
Proposition 4
Let be two -modules. The canonical -linear mappings* (Algebra, Chapter II, § 4, no. 2, Proposition 2 and no. 1, Proposition 1):
(where the second is bijective) are -module homomorphisms.
We write
Then, for ,
and hence . On the other hand, for :
and hence , which completes the proof.
The -modules and are identified under the isomorphism . If and have finite bases, is an isomorphism (Algebra, Chapter II, § 4, no. 2, Proposition 2), which allows us to identify the -modules and ; in that case, we can therefore identify the -modules and .
4. Examples
Example 1
Let be a Lie algebra over and a -module. The -module structure on and the trivial -module structure on define a -module structure on the -module of bilinear forms on . Then
for all in . If is a given element of , the set of such that is a subalgebra of .
Let be a -module and a bilinear form on . By the above, the set of such that
for all and is a Lie subalgebra of . Suppose that is a field, is finite-dimensional and is non-degenerate. Then every admits a left adjoint (relative to ) which is everywhere defined and the subalgebra in question is the set of such that . By this process we can construct two important examples of Lie algebras:
(a) Take and
We canonically identify with . Then the Lie algebra obtained is the Lie algebra of skew-symmetric matrices. *(When , this algebra is the Lie algebra of the orthogonal group ).
(b) Take and
Example 2
We preserve the notation of Example 1.
The -module structure on defines on the -module of endomorphisms of a -module structure. By (6), for all and :
5. Invariant elements
Definition 3
Let be a Lie algebra and a -module. An element is called invariant (with respect to the -module structure on or with respect to the corresponding representation of ) if for all .
Let be a connected real Lie group, its Lie algebra, an analytic representation of on a finite-dimensional real vector space and the corresponding representation of on . Let . The element is invariant with respect to if and only if for all . This justifies the use of the word "invariant".
Example 1
Let be two -modules and . For an element of to be invariant, it is necessary and sufficient, by (6), that be a homomorphism of the -module into the -module . In particular, if and for all , is invariant if and only if is permutable with the .
Example 2
Let M be a K-module with a finite basis. If M has a g-module structure, and have g-module structures and the canonical mapping of into is a g-module isomorphism (Proposition 4). As is obviously an invariant (cf. Example 1), the corresponding element of is an invariant. If is a basis of M and is the dual basis, we have .
Example 3
Let M be a g-module. Let be a bilinear form on M and f the corresponding element of . For to be invariant, it is necessary and sufficient that f be a g-module homomorphism (Proposition 4 and Example 1). Suppose that K is a field and that . A non-degenerate invariant bilinear form on M defines an isomorphism of the g-module M onto the g-module and hence an isomorphism of the g-module onto the g-module . Thus, by Example 2, giving defines canonically an invariant element c in the g-module , which can be constructed as follows: let be a basis of M and the basis of M such that ; then .
Proposition 5
Let g be a Lie K-algebra, h an ideal of g, a representation of g on M and the restriction of to h. Then the set N of elements of M invariant with respect to is stable under .
Let and ; for all and hence
Proposition 6
Let M be a semi-simple g-module. Then the submodule of invariant elements of M admits one and only one supplement stable under the , namely the submodule generated by the ().
Let be a submodule of M which is stable under the and a supplement of in M. For all with , and hence . Hence . Let be a submodule of stable under the and supplementary to in . For all ,
6. Invariant bilinear forms
Let g be a Lie algebra over K. The adjoint representation of g on g and the zero representation of g on K define a g-module structure on the K-module
of bilinear forms on . Briefly we say that a bilinear form on is invariant if it is invariant under the representation . By formula (10) the necessary and sufficient condition for this to be so is that:
for all in .
Now let be the Lie algebra of derivations of . The identity representation of and the zero representation of on define a representation of on . Briefly we say that a bilinear form on is completely invariant if it is invariant under the representation . A completely invariant bilinear form is invariant. For a bilinear form on to be completely invariant, it is necessary and sufficient that:
for all in and .
Proposition 7
Let be a Lie algebra, an invariant symmetric bilinear form on and an ideal of .
(a) The orthogonal of with respect to is an ideal of . (b) If is characteristic and is completely invariant, is characteristic. (c) If is non-degenerate, is commutative.
Let be a derivation of . Suppose that is stable under and that for in . Then implies , since, for all , and hence . Thus is stable under . This establishes (a) and (b).
Now let be an ideal of and suppose that the restriction of to is zero. For in and , , for . Thus is orthogonal to . If is non-degenerate, is therefore commutative. This result applied to proves (c).
Definition 4
Let be a Lie -algebra and a -module. Suppose that , considered as a -module, admits a finite basis. The bilinear form associated with the -module (or with the corresponding representation) is the symmetric bilinear form on . If the representation in question is the adjoint representation, the associated bilinear form is called the Killing form of .
Proposition 8
Let be a Lie algebra and a -module. Suppose that , considered as a -module, admits a finite basis. The bilinear form associated with is invariant.
For in , we have:
Proposition 9
Suppose that is a field and that the Lie algebra is finite-dimensional* over . *Let be an ideal of , the Killing form of and the Killing form of . Then is the restriction of to .
Let be an endomorphism of the vector space which leaves stable. Let be the restriction of to and the endomorphism of the vector space derived from when passing to the quotient. Then as is seen by taking a basis of of which the first elements form a basis of . Then let and apply the above formula to the case where . Then and . Hence .
Proposition 10
Suppose that is a field and that the Lie algebra is finite-dimensional over . The Killing form of is completely invariant.
Let be a derivation of . There exists a Lie algebra containing as an ideal of codimension 1 and an element of such that for all (§ 1, no. 8, Example 1). Let be the Killing form of . For in , , that is . Now the restriction of to is (Proposition 9). Hence the proposition.
7. Casimir element
Proposition 11
Let be a Lie algebra over a field , its enveloping algebra, a finite-dimensional ideal of and an invariant bilinear form on , whose restriction to is non-degenerate. Let be two bases of such that . Then the element of belongs to the centre of and is independent of the choice of basis .
For let be the restriction to of . Then is a representation of on the vector space and the restriction of to is invariant under this representation. By no. 5, Example 3, the tensor is independent of the choice of basis and is an invariant element of the tensor algebra of . It is also an element of the tensor algebra of , which is invariant for the representation derived from the adjoint representation of . Its canonical image in , that is , is therefore independent of the choice of basis and is an invariant for the representation of on considered at the end of no. 2. This element is therefore permutable with every element of and therefore belongs to the centre of .
When is the bilinear form associated with a -module , the element of Proposition 11 is called the Casimir element associated with (or with the corresponding representation). This element exists if the restriction of to is non-degenerate.
Proposition 12
Let be a Lie algebra over a field , an ideal of of finite dimension n and M a g-module of finite dimension over K. Let c be the Casimir element (assumed to exist) associated with M and h.
(a) . (b) If M is simple and n is not divisible by the characteristic of K, is an automorphism of M.
In the notation of Proposition 11,
Hence, if n is not divisible by the characteristic of K, . On the other hand, as c belongs to the centre of U, is permutable with all the . If further M is simple, is therefore invertible in (Algebra, Chapter VIII, § 4, no. 3, Proposition 2).
8. Extension of the base ring
Let be a commutative ring with unit element and a homomorphism of K into mapping 1 to 1. Let g be a Lie K-algebra, U its enveloping algebra and M a left g-module, that is a left U-module. Then has a canonical left -module structure and hence a left -module structure. Let and be the representations of g and corresponding to M and : is said to be derived from by extending the base ring and the results of Algebra, Chapter VIII, § 13, no. 4 can be applied. If , is just the endomorphism of .
Suppose that K is a field, that is an extension of K and that is the canonical injection of K into . Let V and V' be vector subspaces of M. Let a be the vector subspace of g consisting of the such that . Let be the vector subspace of consisting of the such that . Then . For clearly . Now let . We may write , where the are in g and the are elements of linearly independent over K. For all , , that is , whence , hence and . This shows that . In particular, the centre of is derived from the centre of g by extending K to : it suffices to apply the above to the adjoint representation of g. It follows that for all . Similarly, let h be a subalgebra of g and n the normalizer of h in g. Then the normalizer of in is .
Let K, , g, , M be as in the last paragraph. Let b be a vector subspace of g and W a vector subspace of M. Let V be the vector subspace of M consisting of the such that . Let V' be the vector subspace of consisting of the such that . As above it is seen that . In particular, the vector subspace of invariants of is derived from the vector subspace of invariants of by extending the base field from to .
Let and be as at the beginning of this no. Let be a Lie -algebra and and -modules. If and are isomorphic -modules, and are isomorphic -modules. Conversely:
Proposition 13
Let be a field, an extension of , a Lie -algebra and two -modules of finite dimension over . If and are isomorphic -modules, and are isomorphic -modules.
The proof is in two steps.
(1) Suppose first that is an extension of of finite degree . Let be the enveloping algebra of , so that the enveloping algebra of is (§ 2, no. 9). As and are isomorphic as -modules they are a fortiori isomorphic as -modules; but as -modules they are respectively isomorphic to and . Now and are -modules of finite length; (resp. ) is therefore the direct sum of a family (resp. ) of submodules such that the (resp. ) are indecomposable and two (resp. ) of different indices are not isomorphic (Algebra, Chapter VIII, § 2, no. 2, Theorem 1). Then (resp. ) is isomorphic to the direct sum of the (resp. ); it follows (loc. cit.) that and that after permuting the if necessary and is isomorphic to for , hence is isomorphic to .
(2) General case. Let be the -module and the subspace of invariants of , that is the set of homomorphisms of the -module into the -module . In the -module , the subspace of invariants is . The hypothesis that and are isomorphic implies that and have the same dimension over and that there exists in an element which is an isomorphism of onto . Let be a basis of over and choose bases of and over . If for , the matrix of with respect to these bases has determinant which is a polynomial with coefficients in . When , this determinant is non-zero and hence the coefficients of are not all non-zero. Therefore, if is the algebraic closure of , there exists (since is infinite) elements such that (Algebra, Chapter IV, § 2, no. 5, Proposition 8). If is the algebraic extension of generated by the , it follows that is an isomorphism of onto ; but is of finite degree over (Algebra, Chapter V, § 3, no. 2, Proposition 5) and hence and are isomorphic by the first part of the argument.
Again let and be as the beginning of this no. Let be a representation of on a -module with a finite basis . Then the bilinear form on associated with is derived from the bilinear form associated with by extending the base ring to (for, if , has the same matrix with respect to as with respect to and hence and have the same trace). In particular, if the -module has a finite basis, the Killing form of is derived from that of by extending the base ring to .
Exercises
See the exercises for § 3.