Composition series

Abstract: Let be the Lie algebra of the Lorentz group or, what is the same, of the group . We denote by the Lie algebra of its maximal compact subgroup, that is, of . Let be the finite-dimensional irreducible modules (the finite-dimensional representations of ). Consider an -module . The authors call a Harish-Chandra module if, regarded as -module, it can be written as a sum of finite-dimensional irreducible modules . Here, for each , only finitely many -submodules equivalent to are supposed to occur in the decomposition of .A Harish-Chandra module is called indecomposable if it cannot be decomposed into the direct sum of -modules. In this paper the indecomposable Harish-Chandra modules over are completely described. We find that there are two types of indecomposable Harish-Chandra modules. The modules of the first type are the non-singular Harish-Chandra modules and are defined by the following invariants: an integer (), a complex number , and an integer . The first two of these invariants are already known as invariants of the irreducible representations of the Lorentz group (see [2]). The case of non-singular modules has been investigated earlier by Zhelobenko [3] from a somewhat different approach.The case of singular Harish-Chandra modules is of the greatest interest. The solution of this problem reduces to a non-trivial problem of linear algebra, which is investigated in detail in Chapter 2. The invariants of singular indecomposable modules are, as before, numbers , , , integral and integral.However, instead of the one additional invariant , there are now more invariants. Two types of singular modules are possible: those of the first and those of the second kind.Singular modules of the first kind are characterized, in addition to the invariants and , by a sequence of integers of arbitrary length. Singular indecomposable modules of the second kind are characterized by the following collection of invariants: the numbers , given above, a set of integers , an integer , and a further arbitrary complex parameter . The presence of this parameter is particularly interesting, because it indicates the possibility of deforming an indecomposable module with and fixed.The problems of linear algebra that are used in establishing the facts set out above are of independent interest in that the authors develop and use the apparatus of MacLane's theory of linear relations [4].

Abstract: In this paper, we consider the connected split rank one 1 1 Lie group of real type F4 which we denote by F4. We first exhibit F4 as a group of operators on the complexification of A. A. Albert's exceptional simple Jordan algebra. This enables us to explicitly realize the symmetric space 1 16 15 F4/Spin(9) as the unit ball in R with boundary S . After decomposing the space of spherical harmonics under the action of Spin(9), we obtain the matrix of a transvection operator of F4/Spin(9) acting on a spherical principal series representation. We are then able to completely determine the Jordan Holder series of any spherical principal series representation of F4.

Abstract: We propose a very general construction of simple Virasoro modules generalizing and including both highest weight and Whittaker modules. This construction enables us to classify all simple Virasoro modules that are locally finite over a positive part. To obtain those irreducible Virasoro modules, we use simple modules over a family of finite dimensional solvable Lie algebras. For one of these algebras, all simple modules are classified by R. Block and we extend this classification to the next member of the family. As a result, we recover many known but also construct a lot of new simple Virasoro modules. We also propose a revision of the setup for study of Whittaker modules.