Families of type III KMS states on a class of C*-algebras containing On and QN

被引:5
|
作者
Carey, A. L. [2 ]
Phillips, J. [1 ]
Putnam, I. F. [1 ]
Rennie, A. [2 ]
机构
[1] Univ Victoria, Dept Math & Stat, Victoria, BC, Canada
[2] Australian Natl Univ, Inst Math Sci, Canberra, ACT, Australia
基金
加拿大自然科学与工程研究理事会; 澳大利亚研究理事会;
关键词
KMS state; III lambda factor; Modular index; Twisted cyclic theory; K-theory; TWISTED CYCLIC THEORY; SPECTRAL FLOW; INVARIANTS;
D O I
10.1016/j.jfa.2010.12.031
中图分类号
O1 [数学];
学科分类号
0701 ; 070101 ;
摘要
We construct a family of purely infinite C*-algebras, Q(lambda) for A E (0, 1) that are classified by their K groups. There is an action of the circle T with a unique KMS state on each Q(lambda). For lambda = 1/n, Q(1/n) congruent to O-n, with its usual T action and KMS state. For lambda = p/q, rational in lowest terms, Q(1/n) congruent to O-n (n=q-p+1) with UHF fixed point algebra of type (pq)(infinity). For any n > 1, Q(1/n) congruent to O-n for infinitely many A with distinct KMS states and UHF fixed-point algebras. For any lambda is an element of (0, 1), QA 0 O-infinity. For lambda irrational the fixed point algebras, are NOT AF and the QA are usually NOT Cuntz algebras. For lambda transcendental, K-1 (Q(lambda)) congruent to K-0(Q(lambda))L congruent to Z(infinity), so that Q(lambda) is Cuntz' Q(N) [Cuntz (2008) [16]]. If lambda and lambda(-1) are both algebraic integers, the only O-n which appear are those for which n equivalent to 3 (mod 4). For each lambda, the representation of Q(lambda) defined by the KMS state ip generates psi type III lambda factor. These algebras fit into the framework of modular index theory/twisted cyclic theory of Carey et al. (2010) [8], Carey et al. (2009) [12], Carey et al. (in press) [5]. (C) 2011 Elsevier Inc. All rights reserved.
引用
收藏
页码:1637 / 1681
页数:45
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