Đang chuẩn bị nút TẢI XUỐNG, xin hãy chờ
Tải xuống
Tuyển tập các báo cáo nghiên cứu khoa học ngành toán học tạp chí Journal of Operator Theory đề tài: Tản, từ, hệ thống động lực, và abelianness tiệm cận. | J. OPERATOR THEORY 13 1985 237-253 Copyright by INCREST 1985 DISSIPATIONS DERIVATIONS DYNAMICAL SYSTEMS AND ASYMPTOTIC ABELIANNESS AK1TAKA KISHĨMOTO and DEREK w. ROBINSON 1. INTRODUCTION Let 21 G a be a C -dynamical system where th is a simple c -algebra with identity and G is compact and abelian. Next let 5 be a linear operator from the G -finite elements 2lF of 21 into 2L There have been many recent investigations of this situation with the extra assumption that Ỏ commutes with a see for example 1 and the references therein . The principal aim of these investigations was to characterize those 5 which generate C0-groups of -automorphisms of 2Í or Co-semigroups of completely positive maps. In this paper we study the same questions without the assumption that Ô and a commute. Instead we assume that 21 is asymptotically abelian with respect to an automorphism T and that á and 5 commute with T. Somewhat surprisingly this latter assumption leads to similar but even stronger conclusions. Related results have previously been given by Takesaki 8 and Longo and Peligrad 9 . For example if Ỗ is a -derivation then 5 automatically vanishes on the fixed point algebra 21 of a Ô is closable and its closure Ỗ generates a group of -automorphisms j which commutes with a. Similarly if 5 is a -dissipation for which 5 2I 0 then Ỏ is closable and 5 generates a Co-semigroup of completely positive contractions ft which commutes with á. In both cases acts by multiplication on the spectral subspaces 2I y of 21 i.e. c v í lx X 6 2I y . If Ỗ is a -derivation then i p y A y is a homomorphism of G the dual of G into R. If Ỗ is a -dissipation then fl is a negative definite function. The key point in deriving these results is the observation that asymptotic abelianness defines a natural topology on the multiple tensor products of 21 with itself. This structure is analyzed in Section 2 and is exploited in Section 3 to obtain the generator results. In Section 3 we also examine almost periodic .