12.07.2015 Views

100 Years of Relativity Space-Time Structure: Einstein and Beyond ...

100 Years of Relativity Space-Time Structure: Einstein and Beyond ...

100 Years of Relativity Space-Time Structure: Einstein and Beyond ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

58 H. Nicolai4. Basics <strong>of</strong> Kac Moody TheoryWe here summarize some basic results from the theory <strong>of</strong> KM algebras,referring the reader to 15,16,17 for comprehensive treatments. Every KM algebrag ≡ g(A) can be defined by means <strong>of</strong> an integer-valued Cartan matrixA <strong>and</strong> a set <strong>of</strong> generators <strong>and</strong> relations. We shall assume that the Cartanmatrix is symmetrizable since this is the case encountered for cosmologicalbilliards. The Cartan matrix can then be written as (i, j = 1, . . . r, with rdenoting the rank <strong>of</strong> g(A))A ij = 2〈α i|α j 〉〈α i |α i 〉(43)where {α i } is a set <strong>of</strong> r simple roots, <strong>and</strong> where the angular brackets denotethe invariant symmetric bilinear form <strong>of</strong> g(A). 15 Recall that the rootscan be abstractly defined as linear forms on the Cartan subalgebra (CSA)h ⊂ g(A). The generators, which are also referred to as Chevalley-Serregenerators, consist <strong>of</strong> triples {h i , e i , f i } with i = 1, . . . , r, <strong>and</strong> for each iform an sl(2, R) subalgebra. The CSA h is then spanned by the elementsh i , so that[h i , h j ] = 0 (44)The remaining relations generalize the ones we already encountered in Eqs.(26) <strong>and</strong> (29): Furthermore,<strong>and</strong>[e i , f j ] = δ ij h j (45)[h i , e j ] = A ij e j , [h i , f j ] = −A ij f j (46)so that the value <strong>of</strong> the linear form α j , corresponding to the raising operatore j , on the element h i <strong>of</strong> the preferred basis {h i } <strong>of</strong> h is α j (h i ) = A ij . Moreabstractly, <strong>and</strong> independently <strong>of</strong> the choice <strong>of</strong> any basis in the CSA, theroots appear as eigenvalues <strong>of</strong> the adjoint action <strong>of</strong> any element h <strong>of</strong> theCSA on the raising (e i ) or lowering (f i ) generators: [h, e i ] = +α i (h)e i ,[h, f i ] = −α i (h)f i . Last but not least we have the so-called Serre relationsad (e i ) 1−Aij ( e j)= 0 , ad (fi ) 1−Aij ( f j)= 0 (47)A key property <strong>of</strong> every KM algebra is the triangular decompositiong(A) = n − ⊕ h ⊕ n + (48)where n + <strong>and</strong> n − , respectively, are spanned by the multiple commutators<strong>of</strong> the e i <strong>and</strong> f i which do not vanish on account <strong>of</strong> the Serre relations or the

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!