3.3 The reflector from correspondences to Hilbert bimodules
4.2.2 Relative Cuntz–Pimsner algebras
et(p)(T)et(q)(S)−et(p∨q)(ιp∨qp (T)ιp∨qq (S))|p, q∈P, p∨q <∞, T ∈K(Ep) andS∈K(Eq) with
et(p)(T)et(q)(S)|p, q∈P, p∨q=∞, T ∈K(Ep) andS∈K(Eq) .
Put N TE := TE/IN and let ¯π = {π¯p}p∈P be the representation of E in N TE obtained from the composition ofetwith the quotient map. So ¯πis Nica covariant. It is also injective because the Fock representation is Nica covariant. Hence the pair (N TE,π¯) satisfies all the required properties.
We callN TE theNica–Toeplitz algebraofE.
4.2.2 Relative Cuntz–Pimsner algebras
LetE = (Ep)p∈P be a product system. For eachp∈P, letJp/ Abe an ideal that acts by compact operators onEpand setJ ={Jp}p∈P. We say that a representation ψ={ψp}p∈P isCuntz–Pimsner covariant onJ if, for all p∈P and allainJp,
ψ(p)(ϕp(a)) =ψe(a).
Repeating the argument employed in the proof of Proposition 4.2.5, we obtain the following:
Proposition 4.2.6. Let (G, P) be a quasi-lattice ordered group and let E be a compactly aligned product system overP. LetJ ={Jp}p∈P be a family of ideals inAwithϕp(Jp)⊆K(Ep)for allp∈P.
Then there is aC∗-algebraOJ,E and a Nica covariant representation j={jp}p∈P ofE inOJ,E that is also Cuntz–Pimsner covariant on J and such that
(i) OJ,E is generated by j(E)as aC∗-algebra;
(ii) given a Nica covariant representationψ={ψp}p∈P ofEin aC∗-algebraB that is Cuntz–Pimsner covariant onJ, there is a unique∗-homomorphismψ¯J: OJ,E →B such thatψ¯J ◦jp=ψp for all p∈P.
Moreover, the pair(OJ,E, j)is unique up to canonical isomorphism.
Definition 4.2.7. GivenE andJ as above, we callOJ,E therelative Cuntz–Pimsner algebra deter-mined byJ.
We emphasize two particular cases. IfJp={0}for allp∈P, thenOJ,E =N TE. If (G, P) = (Z,N), Eis a product system of Hilbert bimodules andJp=hhEp| Epiifor allpinP, thenOJ,E is the C∗-algebra studied by Katsura in [29]. He proved that the canonical∗-homomorphism from A toOJ,E is an isomorphism onto the fixed-point algebra ofOJ,E. In this case,E extends to a semi-saturated Fell bundle overZ(see [1]). We will generalise this to a certain class of compactly aligned product systems of Hilbert bimodules over semigroups arising from quasi-lattice orders.
Remark 4.2.8. Fowler defined the Cuntz–Pimsner algebra of a product systemE to be the universal C∗-algebra for representations of E that are Cuntz–Pimsner covariant on J = {Jp}p∈P, where Jp =ϕ−1p (K(Ep)) for allp∈P (see [26]). Here we consider the class of compactly aligned product systems and define the relative Cuntz–Pimsner algebra with respect to a family of ideals as a quotient of the Nica–Toeplitz algebra ofE. This provides the construction of relative Cuntz–Pimsner algebras with a special feature and will allow us to generalise most of the results obtained in Chapter 3 to quasi-lattice ordered groups. Our approach applies to Fowler’s Cuntz–Pimsner algebras of proper product systemsE= (Ep)p∈P if (G, P) is a quasi-lattice ordered group andP is directed. This is so because, in this case, a Cuntz–Pimsner covariant representation ofE in the sense of Fowler is also Nica covariant [26, Proposition 5.4].
A product system of Hilbert bimodulesE = (Ep)p∈P gives rise to a product systemE∗ overPop by settingE∗:= (Ep∗)p∈P,whereEp∗is the Hilbert bimodule adjoint toEp. We will identifyAwith its adjoint Hilbert bimoduleA∗through the isomorphisma7→ae∗implemented by the involution operation onA, whereae∗ is the image ofa∗ inA∗ under the canonical conjugate-linear map. The multiplication mapEp∗⊗AEq∗∼=Eqp∗ is given by the isomorphismEp∗⊗AEq∗∼= (Eq⊗AEp)∗,ξ∗⊗η∗7→(η⊗ξ)∗, followed by the multiplication mapµq,p. In addition,E∗∗ =E. Before providing more concrete examples of relative Cuntz–Pimsner algebras, we need the following lemma.
Lemma 4.2.9. Let E= (Ep)p∈P be a product system of Hilbert bimodules. For eachp∈P, let IEp:=
hhEp| Epii and set IE = {IEp}p∈P. A representation ψ = {ψp}p∈P of E in a C∗-algebra B that is Cuntz–Pimsner covariant on IE naturally induces a representation of E∗ = (Ep∗)p∈P that is Cuntz–
Pimsner covariant onIE∗, where IE∗={IE∗p}p∈P and IEp∗=hhEp∗| Ep∗ii=hEp| Epi. As a consequence, representations ofE that are Cuntz–Pimsner covariant on IE are in one-to-one correspondence with representations ofE∗ that are Cuntz–Pimsner covariant on IE∗.
Proof. For p= e, put ψ∗e := ψe. Given p∈ P \ {e}, define ψp∗: Ep∗ → B by ψ∗p(ξ∗) :=ψp(ξ)∗ and setψ∗={ψp∗}p∈P. Then, for allξ∈ Ep andη∈ Eq,
ψ∗p(ξ∗)ψ∗q(η∗) =ψp(ξ)∗ψq(η)∗=ψqp(µq,p(η⊗ξ))∗=ψqp∗ (µq,p(η⊗ξ)∗). Sinceψis Cuntz–Pimsner covariant onIE, it follows that
ψ∗p(ξ∗)∗ψp∗(η∗) =ψp(ξ)ψp(η)∗=ψ(p)(|ξihη|) =ψe(hhξ|ηii) =ψ∗e(hhξ|ηii)
for all ξ, η ∈ Ep. That ψ∗ is Cuntz–Pimsner covariant on IE∗ follows from the fact that ψ is a representation ofE. So the last statement is obtained from the identityE =E∗∗.
Example 4.2.10. Let α: P → End(A) be an action by injective extendible endomorphisms with hereditary range. LetAα= (Aαp)p∈P be the product system of Hilbert bimodules built out ofαas in Example 4.1.3. Although it is not clear whenAαis compactly aligned,αAalways is so. The idealIp/ A given by the left inner product ofAαpis preciselyAαp(1)A. Given a nondegenerate representationψ= {ψp}p∈P ofAαin a C∗-algebraB, we obtain a strictly continuous unital∗-homomorphism ¯ψe:M(A)→ M(B) by nondegeneracy ofψe. In addition, we define a semigroup homomorphism from P to the semigroup of isometries inM(B) by setting
vp:= lim
λ ψp(uλαp(1)).
Here the limit is taken in the strict topology ofM(B). It indeed exists becausekψp(uλαp(1))k ≤1 for eachλand, fora∈Aandb∈B,
limλ ψp(uλαp(1))(ψe(a)b) = lim
λ ψp(uλαp(a))b=ψp(αp(a))b
and lim
λ (bψe(a))ψp(uλαp(1)) = lim
λ bψp(auλαp(1)) =bψp(aαp(1)). To see thatv∗pvp = 1, observe that
vp∗vp(ψe(a)b) = lim
λ ψp(uλαp(1))∗ψp(αp(a))b= lim
λ ψe α−1p (αp(1)uλαp(a))
b=ψe(a)b.
The semigroup of isometries{vp|p∈P} and the∗-homomorphism ¯ψe:M(A)→M(B) satisfy the relation
vp·ψ¯e(c) = ¯ψe(αp(c))vp
for allc∈M(A) andp∈P. Hence
ψ¯e(αp(c))vpv∗p=vpψ¯e(c)v∗p. (4.2.11) In addition, ψp(aαp(1)) = ψe(a)vp for all a∈ A and p∈ P. Ifψ is Cuntz–Pimsner covariant on IAα={Ip}p∈P,it follows that for allc∈M(A) andp∈P,
ψ¯e(αp(c)) = ¯ψe(αp(c))vpvp∗. Indeed, forc inAandaαp(1) inAαp, we compute
αp(c∗c)aαp(1) =αp(c∗)αp(αp−1(αp(c)aαp(1)))
=αp(c∗)αp(hαp(c∗)αp(1)|aαp(1)i)
=αp(c∗)· hαp(c∗)αp(1)|aαp(1)i
=|αp(c∗)ihαp(c∗)|(aαp(1)). Hence Cuntz–Pimsner covariance gives us
ψe(αp(c∗c)) =ψp(αp(c∗))ψp(αp(c∗))∗=ψe(αp(c∗))vpvp∗ψe(αp(c))
=ψe(αp(c∗))vpψe(c)vp∗=ψe(αp(c∗c))vpv∗p.
SinceAis spanned by positive elements, the same relation holds for allc∈Aand thus for allc∈M(A) if we replaceψeby its extension ¯ψe. So combining this with (4.2.11), we deduce the relation
ψe(αp(c)) =vpψe(c)vp∗ for allc∈A. The same holds for ¯ψeandc inM(A).
Conversely, we claim that a nondegenerate∗-homomorphismπ: A→B together with a semigroup of isometries{vp|p∈P}satisfying the relation
π(αp(a)) =vpπ(a)v∗p (4.2.12)
yields a representation ofAα that is Cuntz–Pimsner covariant onIAα. First, notice that the projec-tionvpvp∗coincides with ¯π(αp(1)), where ¯πis the strictly continuous∗-homomorphism M(A)→M(B) extendingπ. For each p∈ P anda ∈ A, we set ψp(aαp(1)) := π(a)vp. Putψ = {ψp}p∈P. Then
¯
π(αp(1)) =vpvp∗ implies thatψis Cuntz–Pimsner covariant onIp=Aαp(1)Afor allp∈P, since ψe(aαp(1)b) =π(aαp(1)b) =π(a)¯π(1)π(b) =π(a)vpv∗pπ(b) =π(a)vp(π(b∗)vp)∗
=ψp(aαp(1))ψp(b∗αp(1))∗=ψ(p)(|aαp(1)ihb∗αp(1)|)
for allaandbinA. Moreover, (4.2.12) tells us thatψe(αp(a))vp =vpψe(a) for alla∈Aandp∈P. This also gives
ψp(aαp(1))ψq(bαq(1)) =ψpq(aαp(b)αpq(1)) =ψpq µp,q(aαp(1)⊗bαq(1)) . Again by (4.2.12),
ψe αp−1(αp(1)a∗bαp(1))=vp∗vpψe αp−1(αp(1)a∗bαp(1)) vp∗vp
=vp∗ψe(αp(1)a∗bαp(1))vp
=vp∗ψe(a∗b)vp.
This shows thatψ is a representation ofAα that is Cuntz–Pimsner covariant onIAα.
As a result, the crossed productAoαP ofAby the semigroup of endomorphisms provided byαhas a description as the universal C∗-algebra of representations ofAα that are Cuntz–Pimsner covariant onIAα. By Lemma 4.2.9,AoαP may also be described as the universal C∗-algebra for representations ofαA that are Cuntz–Pimsner covariant onI A
α . IfPopis the positive cone of a quasi-lattice order and is also directed, a representation ofαA that is Cuntz–Pimsner covariant onIαA is also Nica covariant by [26, Proposition 5.4]. In this caseOI A
α , Aα ∼=AoαP. In general,AoαP is the Cuntz–Pimsner algebra ofαA as defined by Fowler [26]. See, for instance, [35] and [37] for constructions of crossed products by semigroups of endomorphisms. We also refer the reader to [38] for this and further constructions of crossed products out of product systems.
Example4.2.13. We may attach a C∗-algebra to a quasi-lattice ordered group (G, P) by considering the trivial product system overP. TheToeplitz algebra of (G, P) as introduced by Nica [47], denoted by C∗(G, P), is the Nica–Toeplitz algebra of the trivial product system overP. This is the relative Cuntz–Pimsner algebra with respect to the trivial family of idealsJp={0}for allp∈P. In fact, there is also a description of C∗(G, P) as a semigroup crossed product as in the previous example (see [35]
and also Subsection 6.3.3). This is the universal C∗-algebra generated by a family of isometries{vp}p∈P
subject to the relation
vpvp∗vqv∗q =
(vp∨qv∗p∨q ifp∨q <∞,
0 otherwise.
The Fock representation in this case is the canonical representation ofP by isometries on`2(P). The image of C∗(G, P) in B(`2(P)) under the Fock representation is calledWiener–Hopf algebra [47].