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of a root is a root Accordingly, the set of nonzero roots may be split into a subset + of positive roots and the corresponding subset of negative roots = { , + } The set + is contained in a simplex (convex pyramid) in h , the edges of which are the so-called simple positive roots, that is, positive roots which cannot be decomposed as the sum of two other positive roots Of course, the same holds for The consideration of root systems is the basis of the Cartan classi cation of simple Lie algebras into four in nite series A , B , C , D and ve exceptional algebras G 2 , F 4 , E 6 , E 7 , E 8 [225] In addition to the Lie algebra g, one may also consider the universal enveloping algebra U(g), which consists of all polynomials in the elements of g, taking into account the commutation relations (B3) Of special interest are the so-called Casimir elements, that generate the center of U(g), and in particular the quadratic Casimir n i k i element C 2 = i,k=1 g ik X X , where {X } is the basis of g dual to {X i }, that is, i i B(X , X j ) = j and g ik is the Cartan Killing metric The element C 2 does not depend on the choice of the basis {X i } In a Cartan Chevalley basis {H j , E }, one gets C2 =



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In the same way, one de nes a real Lie algebra as a real vector space with an antisymmetric bracket [ , ] that satis es the Jacobi identity The two concepts are closely related If g is a real Lie algebra, one can de ne its complexi cation gc by complexifying it as a vector space and extending the Lie bracket by linearity If dim g = n, the complex dimension of gc is still n, but its real dimension is 2n Conversely, if g is a complex Lie algebra, and one restricts its parameter space to real numbers, one obtains a real form gr , that is, a real Lie algebra whose complexi cation is again g A given complex Lie algebra has in general several nonisomorphic real forms (also classi ed by Cartan), among them a unique compact one, characterized by the fact that the Cartan Killing metric g i j is negative-de nite For instance, the complex Lie algebra A2 yields two real forms, su(3), the compact one, and su(2, 1) For physical applications, it is not so much the Lie algebras themselves that matter, but their representations in Hilbert spaces The key ingredient for building the latter, also due to Cartan, is the notion of a weight vector Let T be a representation of the Lie algebra g in the Hilbert space h, that is, a linear map of g into the operators on h such that T ([X , Y ]) = [T (X ), T (Y )] , X,Y g (B9)

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The representation T is called Hermitian if T (X ) = T (X ) , for every X g By Schur s lemma, it follows that the Casimir elements of U(g) are simultaneously diagonalizable in any irreducible Hermitian representation of g, and in fact their eigenvalues characterize the representation uniquely Let {H j , E } be a Cartan Chevalley basis of the complexi ed Lie algebra gc of g Then a weight for T is a linear form h , for which there exists a nonzero vector

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