Algebra IX: Finite Groups of Lie Type Finite-Dimensional by R. W. Carter (auth.), A. I. Kostrikin, I. R. Shafarevich

By R. W. Carter (auth.), A. I. Kostrikin, I. R. Shafarevich (eds.)

The finite teams of Lie variety are of crucial mathematical significance and the matter of realizing their irreducible representations is of significant curiosity. The illustration idea of those teams over an algebraically closed box of attribute 0 was once constructed via P.Deligne and G.Lusztig in 1976 and hence in a sequence of papers by way of Lusztig culminating in his ebook in 1984. the aim of the 1st a part of this booklet is to offer an outline of the topic, with no together with distinctive proofs. the second one half is a survey of the constitution of finite-dimensional department algebras with many define proofs, giving the fundamental concept and techniques of building after which is going directly to a deeper research of department algebras over valuated fields. An account of the multiplicative constitution and decreased K-theory offers fresh paintings at the topic, together with that of the authors. therefore it types a handy and extremely readable creation to a box which within the final 20 years has obvious a lot progress.

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Additional info for Algebra IX: Finite Groups of Lie Type Finite-Dimensional Division Algebras

Example text

We shall therefore concentrate on the determination of the G-orbits of nilpotent elements in L( G). 5 The lacobson-Morozov Theorem The Lie algebra of the group SL 2 (K) is the algebra sI2(K) of all 2 x 2 matrices of trace 0 under Lie multiplication. This algebra has a basis (e, h,f) where h=G 0) /=(0 0) = =-2/ = e=(~ ~) -1 1 0 These basis elements satisfy the relations [he] 2e [hf] [ef] h The elements e and / are nilpotent. The Jacobson-Morozov theorem asserts that, under certain circumstances, every non-zero nilpotent element e E L(G) lies in a three-dimensional subalgebra (e, h,f) isomorphic to sI2(K).

Y. -stable points by considering a geometrical construct called the Brauer complex. This is defined as follows. Let F- 1 (y) = {y E Y®

Then End (1gJ) is the Hecke algebra H(GF , BF ). 3 that this algebra has dimension IWFI and basis Tw, WE WF. WF is a Coxeter group with Coxeter generators SJ corresponding to the F-orbits J on the Dynkin diagram of G. The multiplication of the basis elements is determined by the relations T. T. Jw+(PJ-1)Tw ifl(sJw)=I(w)-1 where W E WF, i is the length function on WF, and PJ = IUF n (UF)WOSJI. We now turn to the general case. It was shown by Howlett and Lehrer that End (,pff:) has dimension IWol where Wo is the subgroup of WF given by J Wo = {w E WF; w(J) = J, W,p = ,p}.

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