Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2013, Article ID 204319, 12 pages http://dx.doi.org/10.1155/2013/204319 Research Article The Linear Span of Projections in AH Algebras and for Inclusions of πΆ∗-Algebras Dinh Trung Hoa,1 Toan Minh Ho,2 and Hiroyuki Osaka3 1 Center of Research and Development, Duy Tan University, K7/25 Quang Trung, Da Nang, Vietnam Institute of Mathematics, VAST, 18 Hoang Quoc Viet, Ha Noi 10307, Vietnam 3 Department of Mathematical Sciences, Ritsumeikan University, Kusatsu, Shiga 525-8577, Japan 2 Correspondence should be addressed to Hiroyuki Osaka; osaka@se.ritsumei.ac.jp Received 18 October 2012; Accepted 6 January 2013 Academic Editor: Ivanka Stamova Copyright © 2013 Dinh Trung Hoa et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. (π΄ π , ππ ) has the LP property if and only if every element of the In the first part of this paper, we show that an AH algebra π΄ = lim σ³¨→ centre of π΄ π belongs to the closure of the linear span of projections in π΄. As a consequence, a diagonal AH-algebra has the LP property if it has small eigenvalue variation in the sense of Bratteli and Elliott. The second contribution of this paper is that for an inclusion of unital πΆ∗ -algebras π ⊂ π΄ with a finite Watatani index, if a faithful conditional expectation πΈ : π΄ → π has the Rokhlin property in the sense of Kodaka et al., then π has the LP property under the condition thatπ΄ has the LP property. As an application, let π΄ be a simple unital πΆ∗ -algebra with the LP property, πΌ an action of a finite group πΊ onto Aut(π΄). If πΌ has the Rokhlin property in the sense of Izumi, then the fixed point algebra π΄πΊ and the crossed product algebra π΄ βπΌ πΊ have the LP property. We also point out that there is a symmetry on the CAR algebra such that its fixed point algebra does not have the LP property. 1. Introduction A πΆ∗ -algebra is said to have the LP property if the linear span of projections (i.e., the set of all linear combinations of projections in the algebra) is dense in this algebra. A picture of the problem which asks to characterize the simple πΆ∗ algebras to have the LP property was considered in [1]. The LP property of a πΆ∗ -algebra is weaker than real rank zero since the latter means that every self-adjoint element can be arbitrarily closely approximated by linear combinations of orthogonal projections in this πΆ∗ -algebra. In the class of simple AH algebras with slow dimension growth, real rank zero and small eigenvalue variation in the sense of Bratteli and Elliott are equivalent (see [2, 3]). It is not known whether the equivalence still holds when the algebras do not have slow dimension growth. The concept of diagonal AH algebras (AH algebra which can be written as an inductive limit of homogeneous πΆ∗ algebras with diagonal connecting maps) was introduced in [4] or [5]. Let us denote by D the class of diagonal AH algebras. AF-, AI-, and AT-algebras, Goodearl algebras [6], and Villadsen algebras of the first type [7] are diagonal AH algebras. The algebras constructed by Toms in [8] specially which have the same πΎ-groups and tracial data but different Cuntz semigroups are Villadsen algebras of the first type and so belong to D. This means that the class D contains “ugly” and interesting πΆ∗ -algebras and has not been classified by Elliott’s program so far. Note that the classification program of Elliott, the goal of which is to classify amenable πΆ∗ -algebras by their πΎtheoretical data, has been successful for many classes of πΆ∗ algebras, in particular for simple AH algebras with slow dimension growth (see, e.g., [9–11]). Unfortunately, for AH algebras with higher dimension growth, very little is known. In the first part of this paper (Section 2), we consider the LP property of inductive limits of matrix algebras over πΆ∗ algebras. The necessary and sufficient conditions for such an inductive limit to have the LP property will be presented in Theorem 1. In particular, we will show that an AH algebra π΄ = lim(π΄ π , ππ ) (which need not be diagonal nor simple) σ³¨→ 2 Abstract and Applied Analysis has the LP property provided that the image of every element of the centre of the building blocks π΄ π can be approximated by a linear combination of projections in π΄ (Corollary 2). In Section 2.4, using the idea of bubble sort, we can rearrange the entries on a diagonal element in ππ (πΆ(π)) to obtain a new diagonal element with increasing entries such that the eigenvalue variations are the same (Lemma 5) and the eigenvalue variation of the latter element is easy to evaluate. As a consequence, it will be shown that a diagonal AH algebra has the LP property if it has the small eigenvalue property (Theorem 6) without any condition on the dimension growth. It is well known that the LP property of a πΆ∗ -algebra π΄ is inherited to the matrix tensor product ππ (π΄) and the quotient π(π΄) for any ∗-homomorphism π. But it is not stable under the hereditary subalgebra of π΄. In the second part of this paper (Section 3), we will present the stability of the LP property of an inclusion of a unital πΆ∗ -algebra with certain conditions and some examples illustrated the instability of such the property. More precisely, let 1 ∈ π ⊂ π΄ be an inclusion of unital πΆ∗ -algebras with a finite Watatani index and πΈ : π΄ → π a faithful conditional expectation. Then the LP property of π can be inherited from that of π΄ provided that πΈ has the Rokhlin property in the sense of Osaka and Teruya (Theorem 23). As a consequence, given a simple unital πΆ∗ algebra π΄ with the LP property if an action πΌ of a finite group πΊ to Aut(π΄) has the Rokhlin property in the sense of Izumi, then the fixed point algebra π΄πΊ and the crossed product π΄ βπΌ πΊ have the LP property (Theorem 24). Furthermore, we also give an example of a simple unital πΆ∗ -algebra with the LP property, but its fixed point algebra does not have the LP property (Example 14). Let us recall some notations. Throughout the paper, ππ stands for the algebra of all π × π complex matrices, π = {ππ π‘ }π ,π‘=1,π denotes the standard basis of ππ (for convenience, we also use this system of matrix unit for any size of matrix algebras). Let us denote by ππ (πΆ(π)) the matrix algebra with entries from the algebra πΆ(π) of all continuous functions on space π. If π has finitely many connected components ππ and π = βππ=1 ππ , then π ππ (πΆ (π)) =β¨ ππ (πΆ (ππ )) . (1) π=1 Hence, without lots of generality we can always assume that the spectrum of each component of a homogeneous πΆ∗ algebra is connected. Denote by diag(π1 , π2 , . . . , ππ ) the block diagonal matrix with entries π1 , π2 , . . . , ππ in some algebras. Let π΄ be a πΆ∗ -algebra. Any element π in π΄ can be considered as an element in ππ (π΄) via the embedding π → diag(π, 0). We also denote by πΏ(π΄) the closure of the set of all linear combinations of finitely many projections in π΄. The last two authors appreciate Duy Tan University for the warm hospitality during our visit in September 2012 and the third author would also like to thank Teruya Tamotsu for fruitful discussions about the πΆ∗ -index theory. 2. Linear Span of Projections in AH Algebras 2.1. Linear Span of Projections in an Inductive Limit of Matrix Algebras over πΆ∗ -Algebras. Let π΄ = lim (π΄ π , ππ ) , σ³¨→ (2) π π where π΄ π = ⊕π‘=1 ππππ‘ (π΅ππ‘ ) and π΅ππ‘ are πΆ∗ -algebras. Let πππ‘ be a spanning set of π΅ππ‘ (as a vector space) and ππ be the union of πππ‘ for π‘ = 1, . . . , ππ . Since every element of a πΆ∗ -algebra can be written as a sum of two self-adjoint elements, we can assume that all elements of ππ are self-adjoint. Theorem 1. Let π΄ be an inductive limit πΆ∗ -algebra as above. Then the following statements are equivalent. (i) π΄ has the LP property. (ii) For any integer π, any π₯ ∈ ππ and any π > 0, there exists an integer π ≥ π such that πππ (π₯) can be approximated by an element in πΏ(π΄ π ) to within π. (iii) For any integer π, there exist a spanning set of π΄ π such that the images of all elements in that spanning set under ππ∞ belong to πΏ(π΄). Proof. The implication (iii) ⇒ (i) is obvious. To prove the implication (i) ⇒ (ii), it suffices to mention that every element (projection) in π΄ can be arbitrarily closely approximated by elements (projections, resp.) in π΄ π . Let us prove the implication (ii) ⇒ (iii). Clearly, without lots of generality we can assume that π΄ π = πππ (π΅π ) for every π. For a fixed integer π, we put π ⊗ ππ = {ππ π‘ ⊗ π₯ + ππ‘π ⊗ π₯∗ , π₯ ∈ ππ } . (3) Hence, there exists a unitary π’ ∈ πππ such that 0 π₯ 0 π’ (ππ π‘ ⊗ π₯ + ππ‘π ⊗ π₯) π’∗ = (π₯ 0 0) , 0 0 0 (4) where the 0 in the last column and the last row is of order ππ − 2. It is evident that every element in π΄ π is a linear combination of elements in π ⊗ ππ ∪ π·, where π· is the set of all diagonal elements with coefficients in ππ . Thus, π ⊗ ππ ∪ π· is the spanning set of π΄ π . Now, we claim that this spanning set satisfies the requirement of (iii). Firstly, let π = diag(π₯1 , . . . , π₯ππ ) (π₯π‘ ∈ ππ ) be an element in π·. By (ii), ππ∞ (π₯π‘ ) ∈ πΏ(π΄) for every π‘. Hence ππ∞ (π) ∈ πΏ(π΄). Lastly, let π ∈ π ⊗ ππ . By Identity (4), π can be assumed to be 0 π₯ 0 (π₯ 0 0) 0 0 0 for some π₯ ∈ ππ . (5) Moreover, −π₯ 0 0 π = π’∗ ( 0 π₯ 0) π’, 0 0 0 1 1 0 √2 √2 1 where π’ = (− 1 0) . √2 √2 0 0 1 (6) Abstract and Applied Analysis 3 In addition, there exists an integer π ≥ π such that πππ (π₯) can be approximated by an element of πΏ(π΄ π ) to within π. Hence πππ (π) can be approximated by an element of πΏ(π΄ π ) to within π. Corollary 2. Let π΄ = lim(π΄ π , ππ ) be an AH algebra, where π σ³¨→ π π΄ π = ⊕π‘=1 ππππ‘ (πΆ(πππ‘ )) and πππ‘ are connected compact Hausdorff spaces. Then the following statements are equivalent. (i) π΄ has the LP property. π π πΆ(πππ‘ ) and any π > 0, (ii) For any integer π, any π ∈ ∪π‘=1 there exists an integer π ≥ π such that πππ (π) can be approximated by an element in πΏ(π΄ π ) to within π. From the proof of Theorem 1, we can obtain the following. Let π΅ be a πΆ∗ -algebra. Suppose that π π΅ =β¨ πΆ (ππ ) ⊗ πππ , (10) π=1 where ππ is a connected compact Hausdorff space for every π. Set π = βππ=1 ππ . The following theorem and notations are quoted from [2, 12]. Let π be any self-adjoint element in π΅. For any π₯ in ππ , any positive integer π, 1 ≤ π ≤ ππ , let π π denote the πth lowest eigenvalue of π(π₯) counted with multiplicity. So π π is a function on each ππ , for π = 1, 2, . . . , π. The fact is σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨π π (π₯) − π π (π¦)σ΅¨σ΅¨σ΅¨ ≤ σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨π (π₯) − π (π¦)σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨ . (11) Corollary 3. Let π΄ be a πΆ∗ -algebra. If π΄ has the LP property, then π΄ ⊗ ππ and π΄ ⊗ πΎ have the LP property, where πΎ is the algebra of compact operators on a separable Hilbert space. Hence, π π is continuous, for π = 1, 2, . . . , π for a given summand of π΅. The variation of the eigenvalues of π, denoted by EV(π), is defined as the maximum of the nonnegative real numbers 2.2. Linear Span of Projections in a Diagonal AH Algebra. For convenience of the reader, let us recall the notions from [4]. Let π and π be compact Hausdorff spaces. A ∗homomorphism π from ππ (πΆ(π)) to πππ+π (πΆ(π)) is said to be diagonal if there exist continuous maps {π π , π = 1, π} from π to π such that σ΅¨ σ΅¨ sup {σ΅¨σ΅¨σ΅¨π π (π₯) − π π (π¦)σ΅¨σ΅¨σ΅¨ ; π₯, π¦ ∈ ππ } , π (π) = diag (π β π 1 , π β π 2 , . . . , π β π π , 0) , π ∈ ππ (πΆ (π)) , (7) where 0 is a zero matrix of order π (π ≥ 0). If the size π = 0, the map is unital. The π π are called the eigenvalue maps (or simply eigenvalues) of π. The family {π 1 , π 2 , . . . , π π } is called the eigenvalue pattern of π. In addition, let π and π be projections in ππ (πΆ(π)) and πππ+π (πΆ(π)), respectively. An ∗homomorphism π from πππ (πΆ(π))π to ππππ+π (πΆ(π))π is called diagonal if there exists a diagonal ∗-homomorphism π from ππ (πΆ(π)) to πππ+π (πΆ(π)) such that π is reduced from π on πππ (πΆ(π))π and π(π) = π. This definition can also be extended to a ∗-homomorphism π π π=1 π=1 π :β¨ ππ πππ (πΆ (ππ )) ππ σ³¨→ β¨ ππ πππ (πΆ (ππ )) ππ over all π and all possible values of π. The variation of the normalized trace of π, denoted by TV(π), is defined as σ΅¨σ΅¨ σ΅¨σ΅¨ ππ σ΅¨σ΅¨ σ΅¨σ΅¨ 1 sup {σ΅¨σ΅¨σ΅¨ ∑ (π π (π₯) − π π (π¦))σ΅¨σ΅¨σ΅¨ ; π₯, π¦ ∈ ππ } σ΅¨σ΅¨ σ΅¨σ΅¨ ππ π=1 σ΅¨ σ΅¨ σ΅¨ σ΅¨σ΅¨ = sup {σ΅¨σ΅¨tr (π (π₯)) − tr (π (π¦))σ΅¨σ΅¨σ΅¨ π₯, π¦ ∈ ππ } (13) over all π, where tr denotes the normalized trace of ππ for any positive integer π. Theorem 4 (see [2]). Let π΅ be an inductive limit of homogeneous πΆ∗ -algebras π΅π with morphisms πππ from π΅π to π΅π . Suppose that π΅π has the form ππ π΅π = β¨ ππππ‘ (πΆ (πππ‘ )) , (14) π‘=1 (8) by requiring that each partial map ππ,π : ππ πππ (πΆ (ππ )) ππ σ³¨→ ππ πππ (πΆ (ππ )) ππ (12) (9) induced by π be diagonal. 2.3. Eigenvalue Variation. Suppose that π΅ is a simple AH algebra. Then, π΅ has real rank zero if and only if its projections separate the traces provided that this algebra has slow dimension growth (see [12]). This equivalence was first studied when the dimensions of the spectra of the building blocks in the inductive limit decomposition of π΅ are not more than two, see [2]. where ππ and πππ‘ are positive integers, and πππ‘ is a connected compact Hausdorff space for every positive integer π and 1 ≤ π‘ ≤ ππ . Consider the following conditions. (1) The projections of π΅ separate the traces on π΅. (2) For any self-adjoint element π in π΅π and π > 0, there is a π ≥ π such that TV (πππ (π)) < π. (15) (3) For any self-adjoint element π in π΅π and any positive number π, there is a π ≥ π such that EV (πππ (π)) < π. (16) 4 Abstract and Applied Analysis (4) π΅ has real rank zero. Denote by π 1 and π 2 the eigenvalue maps of β; that is, (i) The following implications hold in general: (4) σ³¨⇒ (3) σ³¨⇒ (2) σ³¨⇒ (1) . (17) (ii) If π΅ is simple, then the following equivalences hold: (3) ⇐⇒ (2) ⇐⇒ (1) . (18) (iii) If π΅ is simple and has slow dimension growth, then all the conditions (1), (2), (3), and (4) are equivalent. Proof. The statements (i) and (ii) are proved in Theorem 1.3 of [2]. The statement (iii) is an immediate consequence of the statement (ii) and Theorem 2 of [12]. An AH πΆ∗ -algebra π΅ is said to have small eigenvalue variation (in the sense of Bratteli and Elliott, [3]) if π΅ satisfies statement (3) of Theorem 4. 2.4. Rearrange Eigenvalue Pattern. In order to evaluate the eigenvalue variation [3] of a diagonal element π = diag(π1 , . . . , ππ ) in ππ (πΆ(π)), we need to rearrange the ππ so that the obtained one π = diag(π1 , . . . , ππ ) with π1 ≤ π2 ≤ ⋅ ⋅ ⋅ ≤ ππ has the same eigenvalue variation of π. The eigenvalue variations of two unitary equivalent selfadjoint elements are equal since their eigenvalues are the same. However, the converse need not be true in general. More precisely, there is a self-adjoint element β in π2 (πΆ(π4 )) which is not unitarily equivalent to diag(π 1 , π 2 ) but the eigenvalue variations of both elements are equal, where π π is the πth lowest eigenvalue of β counted with multiplicity [13, Section 2]. In general, given a self-adjoint element β ∈ ππ (πΆ(π)), for each π₯ ∈ π, there is a (point-wise) unitary π’(π₯) ∈ ππ such that β(π₯) = π’(π₯) diag(π 1 (π₯), π 2 (π₯), . . . , π π (π₯))π’∗ (π₯), where π π (π₯) is the πth lowest eigenvalue of β(π₯) counted with multiplicity. Denote by EV(β) the eigenvalue variation of β, then EV(β) = EV(diag(π 1 , π 2 , . . . , π π )) but π’(π₯) need not be continuous. The fact is that if π’(π₯) is continuous for any self-adjoint β in ππ (πΆ(π)), then dim(π) is less than 3 [13]. However, when replacing the equality “=” by some approximation “≈” and in some spacial cases (diagonal elements) discussed below, we can get such a continuous unitary without any hypothesis on dimension. Let us see the idea via the following example. Let β = diag(π₯, 1 − π₯) ∈ π2 (πΆ[0, 1]). Given any 1/2 > π > 0. By [4, Lemma 2.5], there is a unitary π’ ∈ π2 (πΆ[0, 1]) such that (i) π’(π₯) = 1 ∈ π2 , for all π₯ ∈ [0, 1/2 − π], (ii) π’(π₯) = ( 01 10 ), for all π₯ ∈ [1/2 + π, 1]. { if π₯ ≤ { {π₯ π 1 (π₯) = { { {1−π₯ if π₯ > { 1 2 1 , 2 1 { { {1−π₯ if π₯ ≤ 2 π 2 (π₯) = { 1 { if π₯ > . {π₯ 2 { (19) Then EV(β) = EV(diag(π 1 , π 2 )) = 1/2. It is straightforward to check that βπ’βπ’∗ − diag(π 1 , π 2 )β ≤ π. Lemma 5. Let π be a connected compact Hausdorff space and β = diag(π1 , π2 , . . . , ππ ) a self-adjoint element in ππ (πΆ(π)), where π1 , π2 , . . . , ππ are continuous maps from π to R. For any positive number π, there is a unitary π’ ∈ ππ (πΆ(π)) such that σ΅©σ΅© σ΅©σ΅© ∗ (20) σ΅©σ΅©π’βπ’ − diag (π 1 , π 2 , . . . , π π )σ΅©σ΅© < π, where the π π (π₯) is the πth lowest eigenvalue of β(π₯) counted with multiplicity for every π₯ ∈ π. Proof. If π1 ≤ π2 ≤ ⋅ ⋅ ⋅ ≤ ππ , then the unitary π’ is just the identity of ππ and π π = ππ . Therefore, to prove the lemma, we, roughly speaking, only need to rearrange the given family {π1 , π2 , . . . , ππ } to obtain an increasing ordered family. For π = 1, the lemma is obvious. Otherwise, using the idea of bubble sort, we can reduce to the case π = 2. Let π = (π 1 − π 2 )−1 (−π/2, π/2). Set πΈ = {π₯ ∈ π : π1 (π₯) ≤ π2 (π₯)} ∩ (π \ π) and πΉ = {π₯ ∈ π : π1 (π₯) ≥ π2 (π₯)} ∩ (π \ π). It is clear that πΈ and πΉ are disjoint closed sets and π = πΈ ∪ πΉ ∪ π. We have π 1 (π₯) = min{π1 (π₯), π2 (π₯)} and π 2 (π₯) = max{π1 (π₯), π2 (π₯)} for all π₯ ∈ π. If πΈ(πΉ) is empty, then the unitary π’ can be chosen as ( 01 10 ) (1 ∈ π2 , resp.). Thus, we can assume both πΈ and πΉ are nonempty. By Urysohn’s Lemma, there is a continuous map π : π → [0, 1] such that π is equal to 0 on πΈ and 1 on πΉ. Since the space of unitary matrices of π2 is path connected, there is a unitary path π linking 0 1 π (0) = 1 to π (1) = ( ). 1 0 (21) Consequently, π’ = π β π is a unitary in π2 (πΆ(π)) and π’(π₯)β(π₯)π’∗ (π₯) = diag(π 1 (π₯), π 2 (π₯)) for all π₯ ∈ πΈ ∪ πΉ. For π₯ ∈ π \ (πΈ ∪ πΉ) = π, we have σ΅¨ π σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨π 1 (π₯) − π 2 (π₯)σ΅¨σ΅¨σ΅¨ < , σ΅¨σ΅¨ππ (π₯) − π 1 (π₯)σ΅¨σ΅¨σ΅¨ < , π = 1, 2. 2 2 (22) Hence, σ΅© π σ΅©σ΅© σ΅©σ΅©diag (π 1 (π₯) , π 2 (π₯)) − diag (π 1 (π₯) , π 1 (π₯))σ΅©σ΅©σ΅© < , 2 (23) σ΅©σ΅© π σ΅©σ΅© σ΅©σ΅©β (π₯) − diag (π 1 (π₯) , π 1 (π₯))σ΅©σ΅© < . 2 On account to (23) we have σ΅©σ΅© σ΅© ∗ σ΅©σ΅©π’ (π₯) β (π₯) π’ (π₯) − diag (π 1 (π₯) , π 2 (π₯))σ΅©σ΅©σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π’ (π₯) [β (π₯) − diag (π 1 (π₯) , π 1 (π₯))] π’∗ (π₯)σ΅©σ΅©σ΅© (24) σ΅© σ΅© + σ΅©σ΅©σ΅©diag (π 1 (π₯) , π 1 (π₯)) − diag (π 1 (π₯) , π 2 (π₯))σ΅©σ΅©σ΅© < π. Abstract and Applied Analysis 5 Therefore, σ΅©σ΅© σ΅© ∗ σ΅©σ΅©π’βπ’ − diag (π 1 , π 2 )σ΅©σ΅©σ΅© < π. (25) Thus, σ΅©σ΅© σ΅©σ΅© π+1 σ΅© σ΅©σ΅© σ΅©σ΅©π’ diag (π1 , π2 , . . . , ππ , ππ+1 ) π’∗ − ∑ πΏπ πππ σ΅©σ΅©σ΅© < 2π, σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© π=1 (32) where {πππ } is the standard basis of ππ+1 . This implies that σ΅© σ΅©σ΅© σ΅©σ΅©πππ (π) − πσ΅©σ΅©σ΅© < 2π, σ΅© σ΅© The main result of this section as follows. Theorem 6. Given an AH algebra π΄ = lim(π΄ π , ππ ), where σ³¨→ the ππ are diagonal ∗-homomorphisms from π΄ π to π΄ π+1 , where ππ π΄ π = ⊕π‘=1 ππππ‘ (πΆ(πππ‘ )) and the πππ‘ are connected compact Hausdorff spaces. If π΄ has small eigenvalue variation in the sense of Bratteli and Elliott, then π΄ has the LP property. Proof. By Corollary 2, it suffices to show that ππ∞ (π) ∈ πΏ(π΄) for every real-valued function π ∈ πΆ(πππ‘ ). By the same argument in the proof of Theorem 1, we can assume that each π΄ π‘ has only one component; that is, π΄ π‘ = πππ‘ (πΆ(ππ‘ )). Let π > 0 be arbitrary. Since π΄ has small eigenvalue variation in the sense of Bratteli and Elliott, there is an integer π ≥ π such that EV(πππ (π)) < π. Let {π1 , . . . , ππ } be the eigenvalue pattern of πππ (π = ππ /ππ ). Then, πππ (π) = πππ (diag (π, 0)) = diag (π β π1 , 0, π β π2 , 0, . . . , π β ππ , 0) (26) ∗ = π£ diag (π1 , π2 , . . . , ππ , 0) π£ , where ππ = π β ππ and π£ is the permutation matrix in πππ moving all the zero to the bottom left-hand corner. Note that EV (πππ (π)) = EV (diag (π1 , π2 , . . . , ππ , ππ+1 )) , (27) where ππ+1 (π₯) = 0 for all π₯ ∈ ππ . By Lemma 5, there exists a unitary π’ ∈ ππ+1 (πΆ(ππ )) and eigenvalue maps π 1 ≤ π 2 ≤ ⋅ ⋅ ⋅ ≤ π π+1 of diag(π1 , π2 , . . . , ππ , ππ+1 ) such that σ΅©σ΅© σ΅© ∗ σ΅©σ΅©π’ diag (π1 , π2 , . . . , ππ , ππ+1 ) π’ − diag (π 1 , . . . , π π+1 )σ΅©σ΅©σ΅© < π. (28) Put 1 πΏπ = (max π π (π₯) + min π π (π₯)) , π₯∈ππ 2 π₯∈ππ π = 1, 2, . . . , π + 1. (29) Then for any π, we have max π π (π₯) − min π π (π₯) ≤ EV (πππ (π)) < π π₯∈ππ π₯∈ππ (30) where π = π£∗ diag(π’∗ (∑π+1 π=1 πΏπ πππ )π’, 0)π£ is a linear combination of projections in π΄ π . Therefore, ππ∞ (π) ∈ πΏ (π΄) . σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨π π (π₯) − πΏπ σ΅¨σ΅¨σ΅¨ < π, ∀π₯ ∈ ππ . (31) (34) 2.5. Another Form of Theorem 6 Lemma 7. Let π΅ be a πΆ∗ -algebra, and π and π projections in π΅. If π and π are Murray-von Neumann equivalent, then ππ΅π is isomorphic to ππ΅π. In particular, if π΅ = ππ (πΆ(π)) (where π is a connected compact Hausdorff space) and π is a constant projection of rank π in π΅, then ππ΅π is ∗-isomorphic to ππ (πΆ(π)). Proof. By assumption, there exists a partial isometry π£ such that π = π£∗ π£ and π = π£π£∗ . Let us consider the following maps: π (π₯) = π£π₯π£∗ (π₯ ∈ ππ΅π) , π (π¦) = π£∗ π¦π£ (π¦ ∈ ππ΅π) . (35) It is straightforward to check that the compositions of π and π are the identity maps. In the case π΅ = ππ (πΆ(π)) and π is a constant projection of rank π in π΅, we have ππ΅π = ππ (πΆ(π)). Therefore, ππ΅π is ∗-isomorphic to ππ (πΆ(π)). Theorem 8 (another form of Theorem 6). Let π΄ = lim(π΄ π , ππ ) σ³¨→ be a diagonal AH algebra, where the πππ‘ are projections in ππ ππππ‘ (πΆ(πππ‘ )), π΄ π = ⊕π‘=1 πππ‘ ππππ‘ (πΆ(πππ‘ ))πππ‘ , and the ππ are unital diagonal. Suppose that each projection π1π‘ is Murray-von Neumann equivalent to some constant projection in π΄ 1 . Then π΄ has the LP property provided that π΄ has small eigenvalue variation in the sense of Bratteli and Elliott. Proof. We can assume that π΄ π = ππ πππ (πΆ(ππ ))ππ , for all π. It is easy to see that π1 is Murray-von Neumann equivalent to π1 = π11 + π22 + ⋅ ⋅ ⋅ + ππ1 , where π1 is the rank of π1 . For π > 1, define ππ = ππ−1 (ππ−1 ). Then ππ = π1π (π1 ) is constant, since π1 is constant and π1π is diagonal. Let us denote by ππ the rank of ππ , then ππ+1 | ππ . By Lemma 7, there are ∗-isomorphisms Θπ from ππ πππ (πΆ(ππ ))ππ to ππ πππ (πΆ(ππ ))ππ = πππ (πΆ(π)) such that Θπ (π) = π£π ππ£π∗ , π£1∗ π£1 and so (33) π£1 π£1∗ (36) ∼ = π1 and π£π = π1π (π£1 ). Since where π1 = ππ is diagonal, there exists its extension πΜπ which is a diagonal ∗-homomorphism from πππ (πΆ(ππ )) to πππ+1 (πΆ(ππ+1 )). 6 Abstract and Applied Analysis Let ππ be the restriction of πΜπ on ππ πππ (πΆ(ππ ))ππ . Then ππ (ππ ) = ππ+1 . Therefore, the map ππ can be viewed as the map from ππ πππ (πΆ(ππ ))ππ to ππ+1 πππ+1 (πΆ(ππ+1 ))ππ+1 and so lim(πππ (πΆ(ππ )), ππ ) is a diagonal AH-algebra. σ³¨→ On the other hand, it is straightforward to check that Θπ+1 β ππ = ππ β Θπ and hence π΄ = lim(πππ (πΆ(ππ )), ππ ). By σ³¨→ Theorem 6, π΄ has the LP property. and ππ,∞ the homomorphisms from ππ and π΄ π to πΎ and π΄ in the inductive limit of πΎ and π΄, respectively. Then 2.6. Examples. In some special cases, small eigenvalue variation in the sense of Bratteli and Elliott and the LP property are equivalent. Φ β (ππ ⊗ ππ ) = (ππ,∞ ⊗ ππ,∞ ) . Example 9. Let π΄ = lim(ππ(π) (πΆ(π)), ππ ) be a Goodearl σ³¨→ algebra [6] and ππ‘,1 the weighted identity ratio for ππ‘,1 . Suppose that π is not totally disconnected and has finitely many connected components, then the following statements are equivalent. (i) π΄ has real rank zero. (ii) limπ‘ → ∞ ππ‘,1 = 0. (iii) π΄ has small eigenvalue variation in the sense of Bratteli and Elliott. (iv) π΄ has the LP property. Proof. Indeed, (i) and (ii) are equivalent by [6, Theorem 9]. The implication (i) ⇒ (iii) follows from [2, Theorem 1.3]. By [14, Theorem 2.6], (i) implies (iv). Using Theorem 6 we get the implication (iii) ⇒ (iv). Finally, (iv) implies (ii) by [6, Theorem 6]. In general, the LP property cannot imply small eigenvalue variation in the sense of Bratteli and Elliott nor real rank zero. For example, let π΄ be a simple AH algebra with slow dimension growth and π» be a simple hereditary πΆ∗ subalgebra of π΄. By [5, Theorem 3.5], π» has nontrivial projections. Hence, π»⊗πΎ has the LP property by [1, Corollary 5]. However, π΄ has real rank zero if and only if it has small eigenvalue variation in the sense of Bratteli and Elliott [3]. This means that we can choose π» with real rank nonzero such that π» ⊗ πΎ has the LP property and does not have small eigenvalue variation in the sense of Bratteli and Elliott. Looking for examples in the class of diagonal AH algebras, we need the following lemma. Lemma 10. Let π΄ be a diagonal AH algebra and πΎ be the πΆ∗ algebra of compact operators on an infinite dimensional Hilbert space. Then the tensor product π΄ ⊗ πΎ is again diagonal. Proof. Let π΄ = lim(π΄ π , ππ ) and πΎ = lim(ππ , ππ ), where π΄ π is a σ³¨→ σ³¨→ homogeneous algebra, ππ is an injective diagonal homomorphism from π΄ π to π΄ π+1 , and ππ is the embedding from ππ to ππ+1 which associates each π ∈ ππ to diag(π, 0) ∈ ππ+1 for each positive integer π. Let us consider the inductive limit lim(π΄ π ⊗ ππ , ππ ⊗ ππ ). For each integer π ≥ 1, denote by ππ,∞ σ³¨→ (ππ+1,∞ ⊗ ππ+1,∞ ) β (ππ ⊗ ππ ) = ππ,∞ ⊗ ππ,∞ . (37) Hence, by the universal property of inductive limit, there exists a unique homomorphism Φ from lim(π΄ π ⊗ ππ , ππ ⊗ ππ ) σ³¨→ to π΄ ⊗ πΎ such that (38) It is straightforward to check that the image of Φ is dense in π΄ ⊗ πΎ and since all the maps ππ and ππ are injective, we have lim(π΄ π ⊗ ππ , ππ ⊗ ππ ) is π΄ ⊗ πΎ. Furthermore, for each σ³¨→ π, we identify an element π ⊗ π in π΄ π ⊗ ππ with the matrix (πππ π) in ππ (π΄ π ), where π = (πππ ) ∈ ππ and π ∈ π΄ π . By interchanging rows and columns (independent of π ⊗ π) of (ππ ⊗ ππ ) (π ⊗ π), we obtain diag(π ⊗ π β π 1 , . . . , π ⊗ π β π π , 0), where π 1 , . . . , π π are the eigenvalue maps of ππ . This means that there is a permutation matrix π’π ∈ ππ+1 (π΄ π+1 ) such that π’π ππ ⊗ ππ π’π∗ is diagonal. The fact is that the inductive limit is unchanged under unitary equivalence; that is, lim (π΄ π ⊗ ππ , ππ ⊗ ππ ) = lim (π΄ π ⊗ ππ , π’π ππ ⊗ ππ π’π∗ ) . σ³¨→ σ³¨→ (39) Hence, lim(π΄ π ⊗ ππ , ππ ⊗ ππ ) is diagonal. σ³¨→ Example 11. Let π΅ be a simple unital diagonal AH algebra with real rank one without the LP property (e.g., take a Goodearl algebra, see Example 9), then π΅ ⊗ πΎ is a diagonal AH algebra of real rank one with the LP property. Proof. By Lemma 10, π΅ ⊗ πΎ is a diagonal AH algebra. The real rank of π΅ ⊗ πΎ is one since that of π΅ is nonzero. Since π΅ is unital, π΅ ⊗ πΎ has a nontrivial projection. By [1, Corollary 5], π΅ ⊗ πΎ has the LP property. 3. The LP Property for an Inclusion of Unital πΆ∗ -Algebras 3.1. Examples. In this subsection, we will show that the LP property is not stable under the fixed point operation via the given examples. Firstly, we could observe the following example which shows that the LP property is not stable under the hereditary subalgebra. Lemma 12. Let π΄ be a projectionless simple unital πΆ∗ -algebra with a unique tracial state. Then for any π ∈ N with π > 1, ππ (π΄) has the LP property. Proof. Note that ππ (π΄) has also a unique tracial state. Since π΄ is unital, ππ (π΄) has a nontrivial projection. Then by [1, Corollary 5], ππ (π΄) has the LP property. Remark 13. Let π΄ be the Jiang-Su algebra. Then we know that π π (π΄) = 1 [14]. Since ππ (π΄) is an AH algebra without real rank zero, π π (ππ (π΄)) = 1. But from Lemma 12, ππ (π΄) has the LP property. Abstract and Applied Analysis 7 Using this observation, we can construct a πΆ∗ -algebra with the LP property such that the fixed point algebra does not have the LP property. Example 14. A simple unital AI algebra π΄ in [15, Example 9], which comes from Thomsen’s construction, has two extremal tracial states; so by [16, Theorem 4.4], π΄ does not have the LP property. There is a symmetry πΌ on π΄ constructed by Elliott such that π΄βπΌ Z/2Z is a UHF algebra. Since the fixed point algebra (π΄βπΌ Z/2Z)π½ = π΄, where π½ is the dual action of πΌ. This shows that there is a simple unital πΆ∗ -algebra π΅ with the LP property such that the fixed point algebra π΅π½ does not have the LP property. 3.2. πΆ∗ -Index Theory. According to Example 14, there is a faithful conditional expectation πΈ : π΅ → π΅π½ . We extend this observation to an inclusion of unital πΆ∗ -algebras with a finite Watatani index as follows. In this section we recall the πΆ∗ -basic construction defined by Watatani. Definition 15. Let π΄ ⊃ π be an inclusion of unital πΆ∗ -algebras with a conditional expectation πΈ from π΄ to π. (1) A quasi-basis for πΈ is a finite set {(π’π , π£π )}ππ=1 ⊂ π΄ × π΄ such that for every π ∈ π΄, π π π=1 π=1 π = ∑π’π πΈ (π£π π) = ∑πΈ (ππ’π ) π£π . (40) (2) When {(π’π , π£π )}ππ=1 is a quasi-basis for πΈ, we define index πΈ by π Index πΈ = ∑π’π π£π . (41) π=1 When there is no quasi-basis, we write Index πΈ = ∞. index πΈ is called the Watatani index of πΈ. Remark 16. We give several remarks about the above definitions. (1) Index πΈ does not depend on the choice of the quasibasis in the above formula, and it is a central element of π΄ [17, Proposition 1.2.8]. (2) Once we know that there exists a quasi-basis, we can choose one of the form {(π€π , π€π∗ )}π π=1 , which shows that Index πΈ is a positive element [17, Lemma 2.1.6]. (3) By the above statements, if π΄ is a simple πΆ∗ -algebra, then Index πΈ is a positive scalar. (4) If Index πΈ < ∞, then πΈ is faithful; that is, πΈ(π₯∗ π₯) = 0 implies π₯ = 0 for π₯ ∈ π΄. Next we recall the πΆ∗ -basic construction defined by Watatani. Let πΈ : π΄ → π be a faithful conditional expectation. Then π΄ π (= π΄) is a pre-Hilbert module over π with a π valued inner product β¨π₯, π¦β©π = πΈ (π₯∗ π¦) , π₯, π¦ ∈ π΄ π . (42) We denote by EπΈ and ππΈ the Hilbert π module completion of π΄ by the norm βπ₯βπ = ββ¨π₯, π₯β©π β1/2 for π₯ in π΄ and the natural inclusion map from π΄ to EπΈ . Then EπΈ is a Hilbert πΆ∗ -module over π. Since πΈ is faithful, the inclusion map ππΈ from π΄ to EπΈ is injective. Let πΏ π (EπΈ ) be the set of all (right) π module homomorphisms π : EπΈ → EπΈ with an adjoint right π module homomorphism π∗ : EπΈ → EπΈ such that β¨ππ, πβ© = β¨π, π∗ πβ© , π, π ∈ EπΈ . (43) Then πΏ π (EπΈ ) is a πΆ∗ -algebra with the operator norm βπβ = sup{βππβ : βπβ = 1}. There is an injective ∗-homomorphism π : π΄ → πΏ π (EπΈ ) defined by π (π) ππΈ (π₯) = ππΈ (ππ₯) (44) for π₯ ∈ π΄ π and π ∈ π΄, so that π΄ can be viewed as a πΆ∗ subalgebra of πΏ π (EπΈ ). Note that the map ππ : π΄ π → π΄ π defined by ππ ππΈ (π₯) = ππΈ (πΈ (π₯)) , π₯ ∈ π΄π (45) is bounded and thus it can be extended to a bounded linear operator, denoted by ππ again, on EπΈ . Then ππ ∈ πΏ π (EπΈ ) and ππ = ππ2 = ππ∗ ; that is, ππ is a projection in πΏ π (EπΈ ). A projection ππ is called the Jones projection of πΈ. The (reduced) πΆ∗ -basic construction is a πΆ∗ -subalgebra of πΏ π (EπΈ ), defined as β⋅β πΆπ∗ β¨π΄, ππ β© = span {π (π₯) ππ π (π¦) ∈ πΏ π (EπΈ ) : π₯, π¦ ∈ π΄ } . (46) Remark 17. Watatani proved the following in [17]. (1) Index πΈ is finite if and only if πΆπ∗ β¨π΄, ππ β© has the identity (equivalently πΆπ∗ β¨π΄, ππ β© = πΏ π (EπΈ )) and there exists a constant π > 0 such that πΈ(π₯∗ π₯) ≥ ππ₯∗ π₯ for π₯ ∈ π΄; that is, βπ₯β2π ≥ πβπ₯β2 for π₯ in π΄ by [17, Proposition 2.1.5]. Since βπ₯β ≥ βπ₯βπ for π₯ in π΄, if index πΈ is finite, then EπΈ = π΄. (2) If index πΈ is finite, then each element π§ in πΆπ∗ β¨π΄, ππ β© has a form π π§ = ∑π (π₯π ) ππ π (π¦π ) (47) π=1 for some π₯π and π¦π in π΄. ∗ β¨π΄, ππ β© be the unreduced πΆ∗ -basic construc(3) Let πΆmax tion defined in Definition 2.2.5 of [17], which has the certain universality (cf.(5) below). If index πΈ is finite, then there exists an isomorphism from πΆπ∗ β¨π΄, ππ β© ∗ β¨π΄, ππ β© [17, Proposition 2.2.9]. Therefore, we to πΆmax ∗ β¨π΄, ππ β©. So we call can identify πΆπ∗ β¨π΄, ππ β© with πΆmax ∗ ∗ πΆπ β¨π΄, ππ β© the πΆ -basic construction and denote it by πΆ∗ β¨π΄, ππ β©. Moreover, we identify π(π΄) with π΄ in πΆ∗ β¨π΄, ππ β©(= πΆπ∗ β¨π΄, ππ β©), and we define it as π πΆ∗ β¨π΄, ππ β© = {∑π₯π ππ π¦π : π₯π , π¦π ∈ π΄, π ∈ N}. π=1 (48) 8 Abstract and Applied Analysis (4) The πΆ∗ -basic construction πΆ∗ β¨π΄, ππ β© is isomorphic to πππ (π)π for some π ∈ N and projection π ∈ ππ (π) [17, Lemma 3.3.4]. If index πΈ is finite, then index πΈ is a central invertible element of π΄ and there is the dual conditional expectation πΈΜ from πΆ∗ β¨π΄, ππ β© to π΄ such that πΈΜ (π₯ππ π¦) = (Index πΈ)−1 π₯π¦ for π₯, π¦ ∈ π΄ (49) by [17, Proposition 2.3.2]. Moreover, πΈΜ has a finite index and faithfulness. If π΄ is simple unital πΆ∗ algebra, index πΈ ∈ π΄ by Remark 16(4). Hence index πΈ = index πΈΜ by [17, Proposition 2.3.4]. (5) Suppose that index πΈ is finite and π΄ acts on a Hilbert space H faithfully and π is a projection on H such that πππ = πΈ(π)π for π ∈ π΄. If a map π ∋ π₯ σ³¨→ π₯π ∈ π΅(H) is injective, then there exists an isomorphism π from the norm closure of a linear span of π΄ππ΄ to πΆ∗ β¨π΄, ππ β© such that π(π) = ππ and π(π) = π for π ∈ π΄ [17, Proposition 2.2.11]. 3.3. Rokhlin Property for an Inclusion of Unital πΆ∗ -Algebras. For a πΆ∗ -algebra π΄, we set σ΅© σ΅© π0 (π΄) = {(ππ ) ∈ π∞ (N, π΄) : lim σ΅©σ΅©σ΅©ππ σ΅©σ΅©σ΅© = 0} , π→∞ ∞ π΄ π∞ (N, π΄) . = π0 (π΄) (50) We identify π΄ with the πΆ∗ -subalgebra of π΄∞ consisting of the equivalence classes of constant sequences and set π΄ ∞ = π΄∞ ∩ π΄σΈ . (51) For an automorphism πΌ ∈ Aut(π΄), we denote by πΌ∞ and πΌ∞ the automorphisms of π΄∞ and π΄ ∞ induced by πΌ, respectively. Izumi defined the Rokhlin property for a finite group action in [18, Definition 3.1] as follows. Definition 18. Let πΌ be an action of a finite group πΊ on a unital πΆ∗ -algebra π΄. πΌ is said to have the Rokhlin property if there exists a partition of unity {ππ }π∈πΊ ⊂ π΄ ∞ consisting of projections satisfying (πΌπ )∞ (πβ ) = ππβ for π, β ∈ πΊ. (52) We call {ππ }π∈πΊ the Rokhlin projections. Let π΄ ⊃ π be an inclusion of unital πΆ∗ -algebras. For a conditional expectation πΈ from π΄ to π, we denote by πΈ∞ the natural conditional expectation from π΄∞ to π∞ induced by πΈ. If πΈ has a finite index with a quasi-basis {(π’π , π£π )}ππ=1 , then πΈ∞ also has a finite index with a quasi-basis {(π’π , π£π )}ππ=1 and Index (πΈ∞ ) = Index πΈ. Motivated by Definition 18, Kodaka et al. introduced the Rokhlin property for an inclusion of unital πΆ∗ -algebras with a finite index [19]. Definition 19. A conditional expectation πΈ of a unital πΆ∗ algebra π΄ with a finite index is said to have the Rokhlin property if there exists a projection π ∈ π΄ ∞ satisfying πΈ∞ (π) = (Index πΈ)−1 ⋅ 1 (53) and a map π΄ ∋ π₯ σ³¨→ π₯π is injective. We call π a Rokhlin projection. The following result states that the Rokhlin property of an action in the sense of Izumi implies that the canonical conditional expectation from a given simple πΆ∗ -algebra to its fixed point algebra has the Rokhlin property in the sense of Definition 19. Proposition 20 (see [19]). Let πΌ be an action of a finite group πΊ on a unital πΆ∗ -algebra π΄ and πΈ the canonical conditional expectation from π΄ to the fixed point algebra π = π΄πΌ defined by πΈ (π₯) = 1 ∑ πΌ (π₯) , #πΊ π∈πΊ π for π₯ ∈ π΄, (54) where #πΊ is the order of πΊ. Then πΌ has the Rokhlin property if and only if there is a projection π ∈ π΄ ∞ such that πΈ∞ (π) = (1/#πΊ) ⋅ 1, where πΈ∞ is the conditional expectation from π΄∞ to π∞ induced by πΈ. The following is the key one in the next section. Proposition 21 (see [19] and [20, Lemma 2.5]). Let π ⊂ π΄ be an inclusion of unital πΆ∗ -algebras and πΈ a conditional expectation from π΄ to π with a finite index. If πΈ has the Rokhlin property with a Rokhlin projection π ∈ π΄ ∞ , then there is a unital linear map π½ : π΄∞ → π∞ such that for any π₯ ∈ π΄∞ there exists the unique element π¦ of π∞ such that π₯π = π¦π = π½(π₯)π and π½(π΄σΈ ∩ π΄∞ ) ⊂ πσΈ ∩ π∞ . In particular, π½|π΄ is a unital injective ∗-homomorphism and π½(π₯) = π₯ for all π₯ ∈ π. The following is contained in [19, Proposition 3.4]. But we give it for self-contained. Proposition 22. Let π ⊂ π΄ be an inclusion of unital πΆ∗ algebras and πΈ conditional expectation from π΄ to π with a finite index. Suppose that π΄ is simple. Consider the basic construction π ⊂ π΄ ⊂ πΆ∗ β¨π΄, ππ β© (:= π΅) ⊂ πΆ∗ β¨π΅, ππ΄ β© (:= π΅1 ) . (55) If πΈ : π΄ → π has the Rokhlin property with a Rokhlin projection π ∈ π΄ ∞ , then the double dual conditional ΜΜ πΈπ΅ ) : πΆ∗ β¨π΅, ππ΄ β© → π΅ has the Rokhlin expectation πΈ(:= property. Proof. Note that from Remark 17(4) and [19, Corollary 3.8], πΆ∗ -algebras πΆ∗ β¨π΄, ππ β© and πΆ∗ β¨π΅, ππ΄ β© are simple. Abstract and Applied Analysis 9 Since ππ πππ = πΈ∞ (π)ππ = (Index πΈ)−1 ππ , (Index πΈ)πππ π ≤ π, and Moreover, for any π§ ∈ πΆ∗ β¨π΄, ππ β©, we have ππ§ = ∑π€π πππ΄ π€π∗ π§ ∞ ∞ πΈΜ (π − (Index πΈ) πππ π) = π − (Index πΈ) ππΈΜ (ππ ) π π (56) = π − π = 0, = ∑π€π πππ΄ (∑πΈΜ (π€π∗ π§π€π ) π€π∗ ) π = ∑π€π ∑πΈΜ (π€π∗ π₯π§π€π ) πππ΄ π€π∗ we have π = (Index πΈ)πππ π. Then, for any π₯, π¦ ∈ π΄ π π (π₯ππ π¦) π = ππ₯πππ ππ¦π = (Index πΈ)−1 ππ₯π¦π π π (60) = ∑ (∑π€π πΈΜ (π€π∗ π§π€π )) πππ΄ π€π∗ π (57) = πΈΜ (π₯ππ π¦) π. π = ∑π§π€π πππ΄ π€π∗ = π§∑π€π πππ΄ π€π∗ π π = π§π. Μ Hence, from Remark 17(3), we have ππ§π = πΈ(π§)π for any π§ ∈ πΆ∗ β¨π΄, ππ β©. Μ πΈπ΄) and ππ΄ Let {(π€π , π€π∗ )} ⊂ π΅ × π΅ be a quasi-basis for πΈ(= Μ be the Jones projection of πΈ. Set π = ∑π π€π πππ΄ π€π∗ ∈ π΅1∞ . Then π is a projection and π ∈ π΅1σΈ . Indeed, since 2 π = Since π΅1 = πΆ∗ β¨πΆ∗ β¨π΄, ππ β©, ππ΄ β©, π ∈ π΅1σΈ ∩ π΅1∞ . To prove that the double dual conditional expectation Μ πΈΜ has the Rokhlin property, we will show that π is the Μ for any π§ ∈ Rokhlin projection of πΈ.ΜΜ Since ππ§π = πΈ(π§)π πΆ∗ β¨π΄, π€π β©, by Remark 17(5), there exists an isomorphism π : πΆ∗ β¨πΆ∗ β¨π΄, ππ β©, ππ΄ β© → πΆ∗ β¨πΆ∗ β¨π΄, ππ β©, πβ© such that π(ππ΄ ) = π and π(π§) = π§ for π§ ∈ πΆ∗ β¨π΄, ππ β©. Then ∑π€π πππ΄ π€π∗ π€π πππ΄ π€π∗ π,π = ∑π€π πππ΄ πΈΜ (π€π∗ π€π ) π€π∗ π,π (58) πΈΜΜ ∞ (π) = ∑π€π ππΈΜΜ ∞ (ππ΄ ) π€π∗ π = ∑π€π (Index πΈ)−1 ππ€π∗ = ∑π€π πππ΄ (∑πΈΜ (π€π∗ π€π ) π€π∗ ) π π π = (Index πΈ)−1 ∑π€π π (ππ΄ ) π€π∗ = ∑π€π πππ΄ π€π∗ = π, π π = (Index πΈ)−1 π (∑π€π ππ΄ π€π∗ ) π π is a projection. Consider the following: πππ΄ = ∑π€π πππ΄ π€π∗ ππ΄ π = (Index πΈ)−1 1 ΜΜ −1 1, = (Index πΈ) = ∑π€π πΈΜ (π€π∗ ) πππ΄ π = πππ΄ , hence πΈΜΜ has the Rokhlin property. ππ΄ π = ππ΄ ∑π€π πππ΄ π€π∗ = ∑πΈΜ (π€π ) ππ΄ ππ€π∗ π = ππ΄ π∑πΈΜ (π€π ) π€π∗ π = πππ΄ = πππ΄ . (61) π (59) 3.4. Main Results Theorem 23. Let 1 ∈ π ⊂ π΄ be an inclusion of unital πΆ∗ algebras with a finite Watatani index and πΈ : π΄ → π a faithful conditional expectation. Suppose that π΄ has the LP property and πΈ has the Rokhlin property. Then π has the LP property. 10 Abstract and Applied Analysis Proof. Let π₯ ∈ π and π > 0. Since π΄ has the LP property, π₯ can be approximated by a line sum of projection ∑ππ=1 π π ππ (ππ ∈ π΄) such that βπ₯ − ∑ππ=1 π π ππ β < π. Since π½ : π΄∞ → π∞ is an injective ∗-homomorphism by Proposition 21, we have σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© π π σ΅© σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©π½ (π₯ − ∑π π π)σ΅©σ΅©σ΅© = σ΅©σ΅©σ΅©π½ (π₯) − ∑π π π½ (ππ )σ΅©σ΅©σ΅© < π. σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© π=1 π=1 π΄ βπΌ πΊ ∗ (62) Since π½|π = ππ, we have βπ₯−∑ππ=1 π π π½(ππ )β < π. Each projection in π∞ can be lifted to a projection in β∞ (N, π), so we can find a set of projections {ππ }ππ=1 ⊂ π such that σ΅©σ΅© σ΅©σ΅© π σ΅© σ΅©σ΅© σ΅©σ΅©π₯ − ∑π π ππ σ΅©σ΅©σ΅© < π. σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© π=1 Proof. At first we prove condition (3). Since πΌ is outer, πΌ is saturated by [21, Proposition 4.9]; that is, (63) = linear span of { ∑ (πΌπ (π₯) π’π ) ( ∑ πΌπ (π¦) π’π ) | π₯, π¦ ∈ π΄} π∈πΊ = linear span of { 1 ∑ π₯∗ πΌπ (π¦) π’π | π₯, π¦ ∈ π΄}. |πΊ| π∈πΊ (66) On the contrary, for any π₯, π¦ ∈ π΄, we have π₯ππ¦ = π₯ Therefore, π has the LP property. Theorem 24. Let πΌ be an action of a finite group πΊ on a simple unital πΆ∗ -algebra π΄ and πΈ be canonical conditional expectation from π΄ to the fixed point algebra π = π΄πΌ defined by πΈ (π₯) = 1 ∑ πΌ (π₯) , #πΊ π∈πΊ π for π₯ ∈ π΄, (64) where #πΊ is the order of πΊ. Suppose that πΌ has the Rokhlin property. We have, then, that if π΄ has the LP property, the fixed point algebra and the crossed product π΄ βπΌ πΊ have the LP property. Before giving the proof, we need the following two lemmas, which must be well known. Lemma 25. Under the same conditions in Theorem 24 consider the following two basic constructions: π΄πΌ ⊂ π΄ ⊂ πΆ∗ β¨π΄, ππ β© ⊂ πΆ∗ β¨π΅, ππ΄ β© π∈πΊ (π΅ = πΆ∗ β¨π΄, ππ β©) (π΄πΌ ) ⊂ π΄ ⊂ π΄ βπΌ πΊ ⊂ πΆ∗ β¨π΄βπΌ πΊ, ππΉ β© , (65) where πΉ : π΄ βπΌ πΊ → π΄ is a canonical conditional expectation. Then there is an isomorphism π : πΆ∗ β¨π΄, ππ β© → π΄ βπΌ πΊ and Μ : πΆ∗ β¨π΅, ππ΄ β© → πΆ∗ β¨π΄ βπΌ πΊ, ππΉ β© such that π (1) π(π) = π for all π ∈ π΄, 1 ∑π’ π¦ |πΊ| π∈πΊ π = 1 π₯ ∑ π’ π¦π’∗ π’ |πΊ| π∈πΊ π π π = 1 ∑ π₯πΌ (π¦) π’π , |πΊ| π∈πΊ π hence π΄ βπΌ πΊ = πΆ∗ β¨π΄, πβ©. Since for any π ∈ π΄ πππ = 1 ∑ π’π π ∑ π’β |πΊ|2 π∈πΊ β∈πΊ = 1 ∑ π’π ππ’π∗ π’π β |πΊ|2 π,β∈πΊ = 1 ∑ πΌπ (π) π’πβ |πΊ|2 π,β∈πΊ = 1 1 ∑ πΌ (π) ∑π’ |πΊ| π∈πΊ π |πΊ| β∈πΊ πβ by Remark 17(5) there is an isomorphism π : πΆ∗ β¨π΄, ππ β© → πΆ∗ β¨π΄, πβ© = π΄ βπΌ πΊ such that π(π) = π for any π ∈ π΄ and π(ππ ) = π. Hence conditions (1) and (2) are proved. By the similar steps we will show conditions (4) and (5). Since for any π₯, π¦, π, π ∈ π΄ (ππΉ π (π₯ππ π¦) ππΉ ) (πππ) = (ππΉ π₯ππ¦) πΉ ( Μ (π) = π(π) for all π ∈ π΅, (4) π Μ (ππ΄ ) = ππΉ . (5) π Moreover, we have Μ. (6) πΉ β π = πΈΜ and π β πΈΜΜ = πΉΜ β π (68) = πΈ (π) π, (2) π(ππ ) = π, where π = (1/|πΊ|) ∑π∈πΊ π’π , (3) π΄βπΌ πΊ = πΆ∗ β¨π΄, πβ©, (67) 1 ∑ ππΌ (π) π’π ) |πΊ| π∈πΊ π = 1 (π π₯ππ¦ππ) |πΊ| πΉ = 1 π₯π¦ππ. |πΊ|2 (69) Abstract and Applied Analysis 11 On the contrary, π (πΈΜ (π₯ππ π¦)) ππΉ (πππ) = π ( 1 1 π₯π¦) ππ |πΊ| |πΊ| 1 π₯π¦ππ. = |πΊ|2 (70) Μ π π¦)). By Remark 17(5), Hence, we have ππΉ π(π₯ππ π¦)ππΉ = π(πΈ(π₯π ∗ Μ : πΆ β¨π΅, ππ΄ β© → πΆ∗ β¨π΄ βπΌ πΊ, ππΉ β© there is an isomorphism π Μ (π) = π(π) for any π ∈ π΅ and π Μ (ππ΄ ) = ππΉ . such that π The condition (6) comes from the direct computation. Lemma 26. Under the same conditions Lemma 25 πΆ∗ β¨π΄ βπΌ πΊ, ππΉ β© is isomorphic to π|πΊ| (π΄). in Proof. Note that {(π’π∗ , π’π )}π∈πΊ is a quasi-basis for πΉ. By [17, Lemma 3.3.4], there is an isomorphism from πΆ∗ β¨π΄ βπΌ πΊ, ππΉ β© to ππ|πΊ| (π΄)π, where π = [πΈ(π’π∗ π’β )]π,β∈πΊ = πΌ|πΊ| . Hence πΆ∗ β¨π΄ βπΌ πΊ, ππΉ β© is isomorphic to π|πΊ| (π΄). Proof of Theorem 24. Let {ππ }π∈πΊ be the Rokhlin projection of πΈ. From Proposition 20, πΈ : π΄ → π΄πΊ is of index finite and has a projection π ∈ π΄σΈ ∩ π΄∞ such that πΈ∞ (π) = (1/|πΊ|)1. Note that index πΈ = |πΊ| and π = π1 . Consider the basic construction π΄πΊ ⊂ π΄ ⊂ πΆ∗ β¨π΄, ππ β© ⊂ πΆ∗ β¨π΅, ππ΄ β© (π΅ = πΆ∗ β¨π΄, ππ β©) . (71) Since π΄ is simple, the map π΄ ∋ π₯ σ³¨→ π₯π is injective, hence we know that πΈ has the Rokhlin property. Therefore, π΄πΊ has the LP property by Theorem 23. Since πΆ∗ β¨π΄ βπΌ πΊ, ππΉ β© is isomorphic to π|πΊ| (π΄) by Lemma 26 and π΄ has the LP property, πΆ∗ β¨π΄ βπΌ πΊ, ππΉ β© has the LP property. Hence, πΆ∗ β¨π΅, ππ΄ β© has the LP property, because that πΆ∗ β¨π΄ βπΌ πΊ, ππΉ β© is isomorphic to πΆ∗ β¨π΅, ππ΄ β© from Lemma 25. From Proposition 22, πΈΜΜ : πΆ∗ β¨π΅, ππ΄ β© → πΆ∗ β¨π΄, ππ β© has the Rokhlin property, hence we conclude that πΆ∗ β¨π΄, ππ β© has the LP property by Theorem 23. Since πΆ∗ β¨π΄, ππ β© is isomorphic to π΄ βπΌ πΊ by Lemma 25, we conclude that π΄ βπΌ πΊ has the LP property. Remark 27. (1) When an action πΌ of a finite group πΊ does not have the Rokhlin property, we have an example of simple unital πΆ∗ -algebra with the LP property such that the fixed point algebra π΄πΊ does not have the LP property by Example 14. Note that the action πΌ does not have the Rokhlin property. (2) When an action of a finite group πΊ on a unital πΆ∗ algebra π΄ has the Rokhlin property, the crossed product can be locally approximated by the class of matrix algebras over corners of π΄ [22, Theorem 3.2]. Many kinds of properties are preserved by this method such as AF algebras [23], AI algebras, AT algebras, simple AH algebras with slow dimension growth and real rank zero [22], D-absorbing separable unital πΆ∗ algebras for a strongly self-absorbing πΆ∗ -algebras D [24], simple unital separable strongly self-absorbing πΆ∗ -algebras [20], and unital Kirchberg πΆ∗ -algebras [22]. Like the ideal property [25], however, since the LP property is not preserved by passing to corners by Lemma 12, we cannot apply this method to determine the LP property of the crossed products. We could also have many examples which shows that the LP property is preserved under the formulation of crossed products from the following observation. Let π΄ be an infinite dimensional simple πΆ∗ -algebra and let πΌ be an action from a finite group πΊ on Aut(π΄). Recall that πΌ has the tracial Rokhlin property if for every finite set πΉ ⊂ π΄, every π > 0, and every positive element π₯ ∈ π΄ with βπ₯β = 1, there are mutually orthogonal projections ππ ∈ π΄ for π ∈ πΊ such that (1) βπΌπ (πβ ) − ππβ β < π for all π, β ∈ πΊ and all π ∈ πΉ, (2) βππ π − πππ β < π for all π ∈ πΊ and all π ∈ πΉ, (3) with π = ∑π∈πΊ ππ , the projection 1 − π is the Murray-von Neumann equivalent to a projection in the hereditary subalgebra of π΄ generated by π₯, (4) with π as in (3), we have βππ₯πβ > 1 − π. It is obvious that the tracial Rokhlin property is weaker than the Rokhlin property. Proposition 28. Let πΌ be an action of a finite group πΊ on a simple unital πΆ∗ -algebra π΄ with a unique tracial state. Suppose that πΌ has the tracial Rokhlin property. If π΄ has the LP property, then the crossed product π΄ βπΌ πΊ has the LP property. Proof. From [26, Proposition 5.7], the restriction map from tracial states on the crossed product π΄ βπΌ πΊ to πΌ-invariant tracial states on π΄ is isomorphism. Hence, π΄ βπΌ πΊ has a unique tracial state. Since πΌ is a pointwise outer (i.e., for any π ∈ πΊ \ {0} πΌπ is outer) by [23, Lemma 1.5], π΄ βπΌ πΊ is simple. Therefore, by [1, Corollary 4], π΄ βπΌ πΊ has the LP property. Remark 29. There are many examples of actions πΌ of finite groups on simple unital πΆ∗ -algebras with real rank zero and a unique tracial state such that πΌ has the tracial Rokhlin property, see [23, 26]. Acknowledgment The research of H. Osaka was partially supported by the JSPS grant for Scientific Research no. 23540256. 12 References [1] G. K. Pedersen, “The linear span of projections in simple πΆ∗ algebras,” Journal of Operator Theory, vol. 4, no. 2, pp. 289–296, 1980. [2] B. Blackadar, O. Bratteli, G. A. Elliott, and A. 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