
TL;DR
This paper characterizes the kernel of the bounded transform in unbounded $KK$-theory, introduces an equivalence relation on unbounded Kasparov modules, and establishes a topological unbounded $KK$-theory isomorphic to $KK$-theory.
Contribution
It defines an equivalence relation on unbounded Kasparov modules and introduces topological unbounded $KK$-theory, clarifying the structure of the kernel of the bounded transform.
Findings
The kernel of the bounded transform is described via an equivalence relation.
A new notion of topological unbounded $KK$-theory is introduced.
The topological unbounded $KK$-theory is shown to be isomorphic to $KK$-theory.
Abstract
In the founding paper on unbounded -theory it was established by Baaj and Julg that the bounded transform, which associates a class in -theory to any unbounded Kasparov module, is a surjective homomorphism (under a separability assumption). In this paper, we provide an equivalence relation on unbounded Kasparov modules and we thereby describe the kernel of the bounded transform. This allows us to introduce a notion of topological unbounded -theory, which becomes isomorphic to -theory via the bounded transform. The equivalence relation is formulated entirely at the level of unbounded Kasparov modules and consists of homotopies together with an extra degeneracy condition. Our degenerate unbounded Kasparov modules are called spectrally decomposable since they admit a decomposition into a part with positive spectrum and a part with negative spectrum.
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\FirstPageHeading
\ShortArticleName
On the Unbounded Picture of -Theory
\ArticleName
On the Unbounded Picture of -Theory††This paper is a contribution to the Special Issue on Noncommutative Manifolds and their Symmetries in honour of Giovanni Landi. The full collection is available at https://www.emis.de/journals/SIGMA/Landi.html
\Author
Jens KAAD
\AuthorNameForHeading
J. Kaad
\Address
Department of Mathematics and Computer Science, The University of Southern Denmark,
Campusvej 55, DK-5230 Odense M, Denmark \Email[email protected] \URLaddresshttps://portal.findresearcher.sdu.dk/en/persons/kaad
\ArticleDates
Received October 22, 2019, in final form August 05, 2020; Published online August 22, 2020
\Abstract
In the founding paper on unbounded -theory it was established by Baaj and Julg that the bounded transform, which associates a class in -theory to any unbounded Kasparov module, is a surjective homomorphism (under a separability assumption). In this paper, we provide an equivalence relation on unbounded Kasparov modules and we thereby describe the kernel of the bounded transform. This allows us to introduce a notion of topological unbounded -theory, which becomes isomorphic to -theory via the bounded transform. The equivalence relation is formulated entirely at the level of unbounded Kasparov modules and consists of homotopies together with an extra degeneracy condition. Our degenerate unbounded Kasparov modules are called spectrally decomposable since they admit a decomposition into a part with positive spectrum and a part with negative spectrum.
\Keywords
-theory; unbounded -theory; equivalence relations; bounded transform
\Classification
19K35; 58B34
*Dedicated to Gianni Landi on the occasion
of his 60th birthday*
1 Introduction
-theory, as introduced by Kasparov in [16, 18], has its roots in the Brown–Douglas–Fillmore extension theory of commutative -algebras [5], and in Atiyah’s axiomatization of properties of elliptic operators on manifolds, [1]. But -theory extends far beyond the context of commutative -algebras and has become an important tool for accessing the algebraic topology of -algebras with applications ranging from Elliott’s classification program to key aspects of index theory.
In practice, explicit classes in -theory often come from unbounded operators acting on Hilbert -modules and these unbounded operators constitute the main ingredient in the unbounded picture of -theory. The cycles in the unbounded picture are called unbounded Kasparov modules and are often of a differential geometric origin with prototypical examples being Dirac operators (in the case of -homology) or multiplication operators by symbols of Dirac operator (in the case of -theory). In the unbounded picture, the relationship between -theory and the program of Connes on noncommutative geometry is in fact immediate: spectral triples are, without any further modifications, examples of unbounded Kasparov modules [6, 7].
The passage from the unbounded picture to the more commonly encountered bounded picture of -theory is furnished by the bounded transform which turns an unbounded Kasparov module into a class in -theory via the smooth approximation of the sign function given by t\mapsto t\big{(}1+t^{2}\big{)}^{-1/2} (and the functional calculus on Hilbert -modules). The richness of the unbounded picture is witnessed by a fundamental theorem of Baaj and Julg stating that any class in -theory comes from an unbounded Kasparov module so that the bounded transform is in fact a surjection (under a mild separability condition) [2]. See also [20, 24] for other interesting and related lifting results.
In this paper, we construct an equivalence relation on unbounded Kasparov modules which captures the kernel of the bounded transform and this equivalence relation is “geometric” in the sense that it can be formulated without any reference to the bounded picture of -theory. Our equivalence relation relies on an extra degeneracy condition on unbounded Kasparov modules together with a notion of homotopies using families of unbounded Kasparov modules parametrized by the unit interval. Our degeneracy condition on an unbounded Kasparov module is formulated in terms of a spectral decomposition of the unbounded operator in question building on the simple observation that the phase of an unbounded selfadjoint and regular operator with strictly positive spectrum is equal to the identity operator. It was pointed out to us by the referee that spectral decomposability is related to the concept of weak degeneracy from [8, Definition 3.1] and that it can be formulated alternatively as a condition on the bounded transform. We are of course grateful for these comments.
In summary, we introduce a notion of topological unbounded -theory and show that topological unbounded -theory is isomorphic to -theory via the bounded transform. We hereby give an affirmative answer to the question raised by Deeley, Goffeng, and Mesland on page in [8]. In fact, it turns out that our topological unbounded -theory is independent of the choice of a dense -subalgebra of a -algebra as long as this -subalgebra is countably generated. It would thus be interesting to investigate the relationship between topological unbounded -theory and the bordism group introduced in [8], where the equivalence relation comes from Hilsum’s notion of bordisms of unbounded Kasparov modules [9].
The idea for proving the injectivity of the bounded transform is to apply the lifting procedure introduced by Baaj and Julg to a homotopy at the bounded level, where the homotopic elements are bounded transforms of some given unbounded Kasparov modules. The problem with this idea is that it might very well happen that the unbounded homotopy achieved from this process connects two unbounded Kasparov module that are very different from the original ones. To see what might happen, notice that an unbounded Kasparov module could satisfy that commutators extend to bounded operators for all elements in a dense subalgebra whereas a Baaj–Julg lift can always be chosen such that commutators extend to compact operators for all elements in a (perhaps different) dense subalgebra. In this paper, we resolve this problem by studying the concept of a spectrally decomposable unbounded Kasparov module which provides a type of degenerate elements at the unbounded level, related to the idea that a strictly positive unbounded operator should not contain any topological information.
After this paper was written and made available on the arXiv a strengthening of our results was obtained by van den Dungen and Mesland [26]. Among other things these authors were able to prove that a spectrally decomposable unbounded Kasparov module is in fact null-homotopic at the unbounded level, see [26, Corollary 4.9]. Notably, using ideas related to [2, 20, 24], van den Dungen and Mesland also establish a lifting result regarding homotopies of Kasparov modules which is stronger than the lifting results applied in the present text, see [26, Theorem 2.9].
We emphasize that the word topological is a keyword in connection with our definition of unbounded -theory. In other approaches to unbounded -theory, the aim is to find an interesting equivalence relation which captures geometric content at the level of unbounded Kasparov modules while still admitting explicit formulae for the interior Kasparov product. The geometric content which could be valuable in this respect relates to the asymptotic behaviour of eigenvalues and the spectral metric aspects of noncommutative geometry. Certainly, this geometric content is invisible from a topological point of view and thus in particular from the point of view of topological unbounded -theory. The delicate questions on the geometric nature of unbounded -theory are part of ongoing research on the unbounded Kasparov product and the interested reader can consult the following (incomplete list of) references: [4, 11, 14, 15, 19, 20, 23, 24].
1.1 Standing assumptions
Throughout this text and will be -graded -algebras with separable and -unital (meaning that has a countable approximate identity). We moreover fix a norm-dense -graded -subalgebra , which we require to be generated as a -algebra by some countable subset . Remark that the grading on is compatible with the grading on meaning that the -grading operator (being on and on ) induces the -grading operator .
2 Kasparov modules and -theory
In this section we give a brief summary of the main definitions concerning Kasparov modules and -theory. For more details the reader can consult the following references: [3, 10, 18]. The commutators appearing in this section are all graded commutators. For a -graded -correspondence from to we usually suppress the even -homomorphism , which determines the left action of on (where denotes the -graded -algebra of bounded adjointable operators on ).
Definition 2.1**.**
A Kasparov module from to is a pair where is a countably generated -graded -correspondence from to and is an odd bounded adjointable operator such that
[TABLE]
are compact operators for all .
A Kasparov module from to is degenerate when
[TABLE]
Definition 2.2**.**
Two Kasparov modules and from to are unitarily equivalent when there exists an even unitary isomorphism of -graded -correspondences such that . In this case we write . Remark that (by definition) has to intertwine the left actions as well so that for all .
When given a -graded -algebra and an even -homomorphism we may “change the base” of a -graded -correspondence from to . Indeed, we may consider as a -graded -correspondence from to and form the interior tensor product which is a -graded -correspondence from to . Any bounded adjointable operator then induces a bounded adjointable operator and this operation yields an even -homomorphism \mathbb{L}(X)\to\mathbb{L}\big{(}X\widehat{\otimes}_{\beta}C\big{)}, see for example [21, Chapter 4].
Definition 2.3**.**
Two Kasparov modules and both from to are homotopic when there exists a Kasparov module from to such that
[TABLE]
where denotes the even -homomorphism given by evaluation at . In this case we write .
It is a non-trivial fact that the above homotopy relation is an equivalence relation and it can be difficult to find a record of this result in the standard literature on -theory. We state the result as a proposition here and notice that the proof is very similar to the proof given in the unbounded setting later on, see Proposition 4.7 and in particular Lemma 4.6 which can be applied to prove the transitivity of the relation .
Proposition 2.4**.**
Homotopy of Kasparov modules is an equivalence relation.
Definition 2.5**.**
-theory from to consists of Kasparov modules from to modulo homotopies. -theory from to is denoted by .
We may form the direct sum of two Kasparov modules and from to and this is the Kasparov module from to given by
[TABLE]
The zero module is the Kasparov module from to .
We quote the following two results from [3, Chapter 17]:
Proposition 2.6**.**
Any degenerate Kasparov module from to is homotopic to the zero module.
Theorem 2.7**.**
The direct sum operation and the zero module provide -theory from to with the structure of an abelian group.
3 Unbounded Kasparov modules
In this section we review the main results of the paper [2], which can be regarded as the founding paper on unbounded -theory. We recall that a symmetric unbounded operator acting on a Hilbert -module over is selfadjoint and regular when the operators are surjective, see [21, Lemmas 9.7 and 9.8]. Unbounded selfadjoint and regular operators admit a continuous functional calculus as developed in [27, 28], see also [21, Theorem 10.9]. Notice that in our convention all unbounded operators are densely defined.
Definition 3.1**.**
An unbounded Kasparov module from to is a pair , where is a countably generated -graded -correspondence from to and is an odd unbounded selfadjoint and regular operator such that
each preserves the domain of and the graded commutator extends to a bounded operator ; 2. 2)
the operator is compact for all .
An unbounded Kasparov module from to is Lipschitz regular when the graded commutator
[TABLE]
extends to a bounded operator on for all .
For an unbounded Kasparov module it follows automatically that is adjointable for all and we have the formulae
[TABLE]
Definition 3.2**.**
The direct sum of two unbounded Kasparov modules and from to is the unbounded Kasparov module
[TABLE]
from to . The zero module from to is the unbounded Kasparov module .
It was proved in [2] that every unbounded Kasparov module represents a class in -theory:
Theorem 3.3**.**
Suppose that is an unbounded Kasparov module from to . Then the pair \big{(}X,D\big{(}1+D^{2}\big{)}^{-1/2}\big{)} is a Kasparov module from to . In particular, we have an associated class \big{[}X,D\big{(}1+D^{2}\big{)}^{-1/2}\big{]}\in KK(A,B) in -theory.
We refer to the assignment (X,D)\mapsto\big{[}X,D\big{(}1+D^{2}\big{)}^{-1/2}\big{]} which sends an unbounded Kasparov module from to to its associated class in as the Baaj–Julg bounded transform.
It turns out that every class in -theory can be represented by an unbounded Kasparov module. This result is also due to Baaj and Julg [2]. The standing hypothesis that is countably generated as a -algebra plays a crucial role in the proof.
Notice that a bounded positive operator is strictly positive precisely when the image of is dense in and in this case is an unbounded positive and regular operator, see [21, Lemma 10.1]. In particular, \operatorname{Dom}\big{(}\Delta^{-1}\big{)}:=\operatorname{Im}(\Delta).
Theorem 3.4**.**
Suppose that is a norm-dense and countably generated -graded -subalgebra. Suppose moreover that is a Kasparov module from to with and . Then there exists an even strictly positive compact operator such that
the operator preserves the domain of and \big{[}F,\Delta^{-1}\big{]}=0 on \operatorname{Dom}\big{(}\Delta^{-1}\big{)}; 2.
each preserves the domain of and \big{[}a,\Delta^{-1}\big{]}\colon\operatorname{Dom}\big{(}\Delta^{-1}\big{)}\to X extends to a compact operator on ; 3.
for each , the image of the graded commutator is contained in \operatorname{Dom}\big{(}\Delta^{-1}\big{)} and is a compact operator.
Moreover, with D:=\Delta^{-1}F\colon\operatorname{Dom}\big{(}\Delta^{-1}\big{)}\to X we have that is an unbounded Kasparov module from to satisfying that
[TABLE]
in . In particular, it holds that the Baaj–Julg bounded transform is surjective.
In the context of the above theorem, it is worthwhile to notice that the graded commutator \big{[}\Delta^{-1}F,a\big{]}\colon\operatorname{Dom}\big{(}\Delta^{-1}\big{)}\to X does in fact extend to a compact operator for all and that \big{(}i+\Delta^{-1}F\big{)}^{-1}\colon X\to X is compact even though the separable -algebra need not be unital.
4 Equivalence relations on unbounded Kasparov modules
In this section we introduce an equivalence relation on unbounded Kasparov modules and use this equivalence relation to construct the topological unbounded -theory. A key ingredient in our approach is the following notion of a degenerate cycle:
Definition 4.1**.**
An unbounded Kasparov module from to is spectrally decomposable when there exists an orthogonal projection such that
preserves the domain of and on ; 2. 2)
and are unbounded positive operators; 3. 3)
for all even elements and for all odd elements ; 4. 4)
, where is the -grading operator on .
Notice that it follows from Definition 4.1 and the regularity and selfadjointness of that and are selfadjoint and regular as well.
For a spectrally decomposable unbounded Kasparov module with spectral decomposition given by an orthogonal projection , we apply the notation
[TABLE]
for the associated unbounded positive and regular operators.
We remark that and so that we obtain the decomposition:
[TABLE]
We refer to [12, Section 6] for more information on products of unbounded selfadjoint and regular operators with bounded adjointable operators.
Lemma 4.2**.**
Suppose that an unbounded Kasparov module from to is spectrally decomposable. Then the class \big{[}X,D\big{(}1+D^{2}\big{)}^{-1/2}\big{]}\in KK(A,B) is equal to zero.
Proof.
By and in Definition 4.1, the pair is a degenerate Kasparov module from to and by Proposition 2.6 it therefore suffices to show that \big{(}X,D\big{(}1+D^{2}\big{)}^{-1/2}\big{)} is homotopic to . We let and show that D\big{(}1+D^{2}\big{)}^{-1/2}Pa-Pa and D\big{(}1+D^{2}\big{)}^{-1/2}(1-P)a-(P-1)a are compact operators on . By in Definition 4.1, it holds that
[TABLE]
implying the identities
[TABLE]
We thus conclude that
[TABLE]
Using in Definition 4.1, we see that D_{+}-\big{(}1+D_{+}^{2}\big{)}^{1/2}\colon\operatorname{Dom}(D_{+})\to X and D_{-}-\big{(}1+D_{-}^{2}\big{)}^{1/2}\colon\operatorname{Dom}(D_{-})\to X extend to bounded adjointable operators on . But this implies that
[TABLE]
and
[TABLE]
are compact operators on . ∎
Remark 4.3**.**
As pointed out to us by the referee, an alternative proof of Lemma 4.2 can be given using a result of Skandalis [25, Lemma 11]. Indeed, with notation as in Lemma 4.2 we obtain that
[TABLE]
It then follows from [25, Lemma 11] that the Kasparov modules \big{(}X,D\big{(}1+D^{2}\big{)}^{-1/2}\big{)} and are operator homotopic and hence also homotopic.
In fact, as was also remarked by the referee, even more is true: an unbounded Kasparov module from to is spectrally decomposable if and only if there exists a selfadjoint unitary operator satisfying that is a degenerate Kasparov module together with the conditions FD\big{(}1+D^{2}\big{)}^{-1/2}-D\big{(}1+D^{2}\big{)}^{-1/2}F=0 and FD\big{(}1+D^{2}\big{)}^{-1/2}+D\big{(}1+D^{2}\big{)}^{-1/2}F\geq 0. As such, spectral decomposability can be viewed as a condition on the bounded transform of .
Definition 4.4**.**
Two unbounded Kasparov modules and are unitarily equivalent when there exists an even unitary isomorphism of -correspondences such that .
Unitary equivalence of unbounded Kasparov modules is indeed an equivalence relation and we denote it by .
Suppose now that is an extra -graded -unital -algebra and that is an even -homomorphism. As in Section 2 we have the change of base operation given by the interior tensor product of -graded -correspondences: . Moreover, any unbounded selfadjoint and regular operator induces an unbounded selfadjoint and regular operator D\widehat{\otimes}_{\beta}1\colon\operatorname{Dom}\big{(}D\widehat{\otimes}_{\beta}1\big{)}\to X\widehat{\otimes}_{\beta}C, which has resolvents given by
[TABLE]
In particular, if is a compact operator for some , then
[TABLE]
is a compact operator as well, see [21, Proposition 4.7]. These observations allow us to formulate our notion of homotopy at the level of unbounded Kasparov modules:
Definition 4.5**.**
Two unbounded Kasparov modules and both from to are homotopic when there exists an unbounded Kasparov module from to such that
[TABLE]
where denotes the even -homomorphism given by evaluation at . In this case we write .
Before proving that homotopies of unbounded Kasparov modules yields an equivalence relation it is worthwhile to spend a little time on a glueing construction for -graded -correspondences. Consider two countably generated -graded -correspondences and both from to and suppose that
[TABLE]
is an even unitary isomorphism of -correspondences. This data gives rise to a -graded -correspondence from to obtained by glueing and using the unitary to identify the fibres sitting at and [math], respectively. Indeed, we may define
[TABLE]
and endow this set with the vector space structure, left action of and -grading inherited from the direct sum . To construct the right action of and the inner product on , we introduce the even -endomorphisms by and for all and . We put
[TABLE]
for all , and .
Lemma 4.6**.**
The -graded -correspondence from to is countably generated. Moreover, if and are compact operators such that , then the direct sum restricts to a compact operator .
Proof.
We start by constructing an adjointable isometry , where denotes the standard module over . Since is -unital by our standing assumptions this will imply that is countably generated.
Since and are countably generated over it follows by Kasparov’s stabilization theorem, [17, Theorem 2], that we may find unitary isomorphisms of Hilbert -modules
[TABLE]
We let denote the unique unitary isomorphism of Hilbert -modules, which makes the diagram here below commute:
[TABLE]
We specify that the lower vertical isomorphisms are induced by , for , and the top vertical unitary isomorphisms come from the distributivity of the interior tensor product together with the lower vertical isomorphisms.
The notation and refers to the standard inclusions given on matrix form as . We define our adjointable isometry by the formula
[TABLE]
for all and . We leave it to the reader to verify that is well-defined (in particular that ). The adjoint of is given explicitly by
[TABLE]
where and for all and .
The compactness of is equivalent to the compactness of . The compact operators on the standard module can be identified with the operator norm continuous maps from to the compact operators on . Using this identification, we compute that
[TABLE]
where and . Since and are compact by assumption this proves the compactness of . ∎
Proposition 4.7**.**
Homotopy of unbounded Kasparov modules is an equivalence relation.
Proof.
Reflexivity: For an unbounded Kasparov module from to , we have that via the unbounded Kasparov module from to , where is the unbounded selfadjoint and regular operator defined by
[TABLE]
Symmetry: Suppose that two unbounded Kasparov modules and from to are homotopic via the unbounded Kasparov module from to . Define the even -automorphism by for all and . Then it holds that and are homotopic via the unbounded Kasparov module from to .
Transitivity: Suppose that , and are unbounded Kasparov modules from to such that and via the unbounded Kasparov modules and , respectively. Let us choose an even unitary isomorphism of -correspondences
[TABLE]
such that . We study the associated -graded -correspondence from to and notice that is countably generated by Lemma 4.6. We define the odd unbounded selfadjoint and regular operator by
[TABLE]
To see that is indeed selfadjoint and regular, we notice that is symmetric and that the resolvents are given by
[TABLE]
for all and all .
We claim that is an unbounded Kasparov module from to . It is indeed clear that each preserves the domain of and that the graded commutator extends to a bounded adjointable operator on . Moreover, it follows from Lemma 4.6 that is a compact operator for all .
The unbounded Kasparov module from to implements the homotopy from to and this ends the proof of the proposition. ∎
Let us shortly discuss the notion of bounded perturbations of unbounded Kasparov modules:
Definition and Proposition 4.8**.**
Let be an unbounded Kasparov module from to and let be an odd bounded selfadjoint operator. Then the pair is an unbounded Kasparov module from to and and are homotopic. We say that is a bounded perturbation of .
Proof.
The domain of agrees with the domain of and is selfadjoint and regular by [27, Example 1]. The commutator condition in Definition 3.1 is immediately verified and the resolvent condition in Definition 3.1 follows from the resolvent identity:
[TABLE]
We thus have that is an unbounded Kasparov module from to . To see that and are homotopic we apply the unbounded Kasparov module from to given by where the corresponding odd unbounded selfadjoint and regular operator is defined by
[TABLE]
We remark that the above notion of bounded perturbations yields an equivalence relation on unbounded Kasparov modules. We will not discuss this equivalence relation any further at this point but refer the reader to [11] for more details.
In this paper the relevant equivalence relation on unbounded Kasparov modules is a stabilized version of homotopies of unbounded Kasparov modules, where we are using spectrally decomposable unbounded Kasparov modules in the stabilization procedure:
Definition 4.9**.**
Two unbounded Kasparov modules and from to are stably homotopic when there exist two spectrally decomposable unbounded Kasparov modules and from to such that
[TABLE]
In this case we write .
We remark that the relation is indeed an equivalence relation and that this can be verified using Proposition 4.7 together with the fact that the direct sum of two spectrally decomposable unbounded Kasparov modules is again spectrally decomposable.
Definition 4.10**.**
The topological unbounded -theory from to consists of the unbounded Kasparov modules from to modulo stable homotopies, thus modulo the equivalence relation . The topological unbounded -theory from to is denoted by .
We may equip the topological unbounded -theory from to with the structure of a commutative monoid, where the addition is induced by the direct sum operation from Definition 3.2 and the neutral element is the class of the zero module . We shall see in Section 6 that is in fact an abelian group.
The next result is a combination of Theorem 3.4 and Lemma 4.2 together with the observation that the Baaj–Julg bounded transform is compatible with direct sums and homotopies of unbounded Kasparov modules.
Theorem 4.11**.**
The Baaj–Julg bounded transform (X,D)\mapsto\big{[}X,D\big{(}1+D^{2}\big{)}^{-1/2}\big{]} induces a well-defined surjective homomorphism
[TABLE]
which we also refer to as the Baaj–Julg bounded transform.
The main result of this paper is that the surjective homomorphism is in fact an isomorphism. In particular, it holds that is independent of the norm-dense -graded -subalgebra as long as is countably generated. This will be proved in Section 7.
5 Lipschitz regularity and invertibility
We shall now see that given a class in topological unbounded -theory one may always choose a Lipschitz regular representative with the extra property that the unbounded selfadjoint and regular operator is invertible (so that is a bounded adjointable operator with image equal to the domain of ).
We start with Lipschitz regularity:
Proposition 5.1**.**
Let and suppose that is an unbounded Kasparov module from to . Then \big{(}X,D\big{(}1+D^{2}\big{)}^{-r}\big{)} is a Lipschitz regular unbounded Kasparov module from to and it holds that
[TABLE]
Proof.
For each , define the functions
[TABLE]
We remark that and that the maps given by are continuous with respect to the supremum norm on . Notice in this respect that we have the estimates whenever and .
For each , we thus have that
[TABLE]
are compact operators for all and that the maps given by t\mapsto\big{(}i\pm D\big{(}1+D^{2}\big{)}^{-tr}\big{)}^{-1} are continuous in operator norm.
For , we are going to apply the integral formula
[TABLE]
where the integrand is continuous in operator norm and the integral converges absolutely in operator norm.
Let be homogeneous. For each , the domain of is a core for D\big{(}1+D^{2}\big{)}^{-tr} and for each , we compute the graded commutator
[TABLE]
The first term extends to the bounded adjointable operator \big{(}1+D^{2}\big{)}^{-tr}d(a)\colon X\to X and we remark that the map defined by t\mapsto\big{(}1+D^{2}\big{)}^{-tr}d(a) is continuous with respect to the strict operator topology on . The second term in equation (5.2) is more complicated and, using the integral formula in equation (5.1), we obtain the expression
[TABLE]
for all , where the left hand side only makes sense on . The right hand side does however make sense as a bounded adjointable operator on and the operator norm is dominated by
[TABLE]
For each we denote the bounded adjointable extension of \big{[}\big{(}1+D^{2}\big{)}^{-tr},a\big{]}D\colon\operatorname{Dom}(D)\allowbreak\to X by . Notice that and that is given explicitly by the right hand side of equation (5.3) for . In particular, it holds that for all . Using the identity in equation (5.2) one may also verify that
[TABLE]
for all . We claim that the map given by is strictly continuous. Since is a -algebra and since the right hand side of the identity in equation (5.4) defines a strictly continuous map on we only need to show that the map is norm continuous for every . In fact, because of the uniform bound on the operator norm of for and the density of in , we may restrict our attention to elements . But for the norm continuity of the map follows since t\mapsto\big{[}\big{(}1+D^{2}\big{)}^{-tr},a\big{]} is strictly continuous and since G_{t}(a)\xi=\big{[}\big{(}1+D^{2}\big{)}^{-tr},a\big{]}D\xi for all .
Our efforts so far can be summarized as follows: we have an unbounded Kasparov module from to , where the unbounded selfadjoint and regular operator is defined by
[TABLE]
In particular, we have that the unbounded Kasparov modules and \big{(}X,D\big{(}1+D^{2}\big{)}^{-r}\big{)} are homotopic.
To finish the proof of the proposition we only need to argue that the unbounded Kasparov module \big{(}X,D\big{(}1+D^{2}\big{)}^{-r}\big{)} is Lipschitz regular. Let be homogeneous. Since the function x\mapsto|x|-x^{2}\big{(}1+x^{2}\big{)}^{-1/2} is bounded on , we just have to prove that the graded commutator
[TABLE]
extends to a bounded operator on . Notice in this respect that
[TABLE]
agrees with
[TABLE]
up to a bounded selfadjoint operator and moreover that is a core for \big{|}D\big{(}1+D^{2}\big{)}^{-r}\big{|}. Since we already know that
[TABLE]
extend to bounded operators on we are left with proving that
[TABLE]
extends to a bounded operator on . But this follows since the integral formula in equation (5.1) implies that
[TABLE]
where the left hand side only makes sense on \operatorname{Dom}\big{(}|D|^{1-2r}\big{)}, but the right hand side makes sense as a bounded operator on . Indeed, both of the integrals in equation (5.5) have operator norm continuous integrands and converge absolutely because of the operator norm estimates
[TABLE]
which are valid for all . ∎
We continue with invertibility:
Proposition 5.2**.**
Suppose that is an unbounded Kasparov module from to . Then is homotopic to a Lipschitz regular unbounded Kasparov module with invertible.
Proof.
By Proposition 5.1 we may assume that is already Lipschitz regular. Let us denote the -grading operator on by . Define the -graded -correspondence from to which agrees with as a Hilbert -module over , but has grading operator and the left action of is trivial. Then the unbounded Kasparov module \big{(}\widetilde{X},-D\big{)} is homotopic to the zero module . Indeed, we may consider the -graded -correspondence C_{0}\big{(}(0,1],\widetilde{X}\big{)} from to equipped with the odd unbounded selfadjoint and regular operator E\colon\operatorname{Dom}(E)\to C_{0}\big{(}(0,1],\widetilde{X}\big{)} defined by
[TABLE]
Since the left action of on C_{0}\big{(}(0,1],\widetilde{X}\big{)} is trivial we have that \big{(}C_{0}\big{(}(0,1],\widetilde{X}\big{)},E\big{)} is an unbounded Kasparov module from to thus realizing the homotopy from \big{(}\widetilde{X},-D\big{)} to . The result of the proposition now follows from Proposition 4.8 by noting that (X,D)+\big{(}\widetilde{X},-D\big{)}=\big{(}X\oplus\widetilde{X},D\oplus(-D)\big{)} is a bounded perturbation of the Lipschitz regular unbounded Kasparov module
[TABLE]
from to . Remark in this respect that the square of is given by
[TABLE]
which is indeed an invertible operator. ∎
6 Group structure
We show in this section that the commutative monoid is in fact an abelian group. This result relies on a more general proposition stating (at least roughly speaking) that two unbounded Kasparov modules and from to are stably homotopic when the odd unbounded selfadjoint and regular operators and have the same phase. This proposition will also be of key importance later on when we prove the injectivity of the Baaj–Julg bounded transform.
Definition 6.1**.**
The inverse of an unbounded Kasparov modules from to is the unbounded Kasparov module from to given by
[TABLE]
where agrees with as a Hilbert -module over , but is equipped with the opposite -grading and with left action \pi_{X^{{\rm op}}}\colon A\to\mathbb{L}\big{(}X^{{\rm op}}\big{)} defined by
[TABLE]
Proposition 6.2**.**
Let and be two unbounded Kasparov modules from to and suppose there exists an odd selfadjoint unitary operator such that
the operator preserves the domain of and of and the commutators and have bounded extensions to ; 2.
the unbounded operators and are bounded perturbations of even unbounded positive and regular operators and ; 3.
for each , the image of the graded commutator is contained in and the operators are bounded.
Then is stably homotopic to the zero module .
Proof.
We are going to show that
[TABLE]
is homotopic to a spectrally decomposable unbounded Kasparov module. We denote the grading operator on by so that the grading operator on is given by .
We remark that the graded commutator is compact for all . Indeed, for any and , it follows from assumption and the fact that is an unbounded Kasparov module that
[TABLE]
is a compact operator.
Define the orthogonal projections
[TABLE]
and for each , define the unitary automorphisms of the Hilbert -module :
[TABLE]
We study the -graded -correspondence from to , which as a Hilbert -module over agrees with , but with left action defined by putting
[TABLE]
for all , and with grading operator defined by
[TABLE]
It is useful to notice that
[TABLE]
Using assumption , we define the unbounded selfadjoint and regular operators
[TABLE]
One may then verify directly that
[TABLE]
are unbounded selfadjoint and regular operators. The resolvent of is for example given by
[TABLE]
for all . Alternatively, we refer to [13, Section 7] or [22, Theorem 4.5] for much more general results on sums of unbounded selfadjoint and regular operators.
We claim that the pair is an unbounded Kasparov module from to (where it is understood that the unbounded selfadjoint and regular operator in question acts as in each fibre). For each we thus have the fibre where is the countably generated -graded -correspondence from to which agrees with as a Hilbert -module but with grading operator and with left action given by the even -homomorphism .
We let be given and compute for each even that
[TABLE]
and for each odd that
[TABLE]
Since the graded commutator is compact, this computation implies that is a compact operator for all and and moreover that the associated map is continuous in operator norm. Using assumption , the above computation also implies that preserves the domain of for all and (the image of is in fact contained in this domain) and moreover that the graded commutator
[TABLE]
extends to a bounded operator on (in fact each of the terms have this property). The associated map given by
[TABLE]
is continuous in operator norm. These observations imply that is an unbounded Kasparov module from to if and only if the fibre at is an unbounded Kasparov module from to .
The fibre at is given by the pair , where is unitarily isomorphic to as a -graded -correspondence via the unitary operator defined in equation (6.1). Moreover, we have that
[TABLE]
By assumption we know that the off-diagonal entries extend to bounded operators on and it follows that the fibre at agrees with the unbounded Kasparov module from to up to unitary equivalence and bounded perturbations. By Proposition 4.8 this implies in particular that is an unbounded Kasparov module from to which is homotopic to .
We may thus conclude that is an unbounded Kasparov module from to .
By what has been achieved so far, we have reduced the proof of the proposition to showing that the fibre of at is homotopic to a spectrally decomposable unbounded Kasparov module from to .
The unbounded Kasparov module sitting as the fibre at is given by the pair , where agrees with as a Hilbert -module over but with grading operator and left action given by
[TABLE]
By assumption we know that is a bounded perturbation of the unbounded selfadjoint and regular operator
[TABLE]
where the upper diagonal entry and minus the lower diagonal entry are both unbounded positive and regular operators. But this shows that the fibre at is a bounded perturbation of a spectrally decomposable unbounded Kasparov module. Indeed, the unbounded Kasparov module from to is spectrally decomposable (using the orthogonal projection when verifying the conditions in Definition 4.1). ∎
Remark 6.3**.**
It is worthwhile to understand the result of Proposition 6.2 in the light of Skandalis’ work in [25]. This relationship was communicated to us by the referee. Indeed, under the assumptions of Proposition 6.2 we obtain that is a Kasparov module from to (see the proof of the proposition). With some effort it can moreover be established that the assumptions imply that a\big{(}FD\big{(}1+D^{2}\big{)}^{-1/2}+D\big{(}1+D^{2}\big{)}^{-1/2}F\big{)}a^{*}\geq 0 modulo the compact operators on for all and a similar result applies to D^{\prime}\big{(}1+(D^{\prime})^{2}\big{)}^{-1/2}. Therefore, by [25, Lemma 11] we obtain that the bounded transforms \big{(}X,D\big{(}1+D^{2}\big{)}^{-1/2}\big{)} and \big{(}X,D^{\prime}\big{(}1+(D^{\prime})^{2}\big{)}^{-1/2}\big{)} are operator homotopic since they are both operator homotopic to .
Notice however that this argument does not yield an alternative proof of Proposition 6.2 since it only provides information on the bounded transforms of the unbounded Kasparov modules and .
Theorem 6.4**.**
The direct sum of unbounded Kasparov modules and the zero module provide the topological unbounded -theory, , with the structure of an abelian group.
Proof.
For an unbounded Kasparov module from to , we need to prove that is stably homotopic to the zero module . By Proposition 5.2 we may assume that is Lipschitz regular and that is invertible. The phase of is then a well-defined odd selfadjoint unitary operator . The result of the present proposition will now be a consequence of Proposition 6.2 applied to the case where : The conditions and are clearly satisfied and condition follows from the Lipschitz regularity of . Indeed, for each homogeneous and each it holds that
[TABLE]
so that for some bounded adjointable operator . ∎
7 Injectivity of the bounded transform
We are now ready to prove the main theorem of this paper:
Theorem 7.1**.**
Suppose that and are a -graded -algebras with separable and -unital. For any norm-dense countably generated -graded -subalgebra we have an isomorphism of abelian groups
[TABLE]
induced by the Baaj–Julg bounded transform (X,D)\mapsto\big{[}X,D\big{(}1+D^{2}\big{)}^{-1/2}\big{]}.
Proof.
By Theorems 6.4 and 4.11 we only need to show that is injective.
Suppose that two unbounded Kasparov modules and from to satisfy that their bounded transforms \big{(}X_{0},D_{0}\big{(}1+D_{0}^{2}\big{)}^{-1/2}\big{)} and \big{(}X_{1},D_{1}\big{(}1+D_{1}^{2}\big{)}^{-1/2}\big{)} are homotopic. We thus have a Kasparov module from to and two even unitary isomorphisms of -correspondences and implementing unitary equivalences
[TABLE]
By Proposition 5.1, we may assume without loss of generality that and are both Lipschitz regular and, using [3, Proposition 17.4.3], we may moreover assume that is a selfadjoint contraction. We let denote the -graded -correspondence from to which agrees with as a Hilbert -module over but with grading operator and with left action given by the even -homomorphism \pi_{X\oplus\widetilde{X}}:=\pi_{X}\oplus 0\colon A\to\mathbb{L}\big{(}X\oplus\widetilde{X}\big{)}. Define the odd bounded adjointable operator
[TABLE]
and notice that and . Moreover, it holds that \big{(}X\oplus\widetilde{X},G\big{)} is a Kasparov module from to which is homotopic to , see [3, Section 17.6]. A similar construction applies to the endpoints yielding Kasparov modules \big{(}X_{0}\oplus\widetilde{X_{0}},G_{0}\big{)} and \big{(}X_{1}\oplus\widetilde{X_{1}},G_{1}\big{)} from to . For each , we define the invertible unbounded selfadjoint and regular operator
[TABLE]
and remark that . We recall from Proposition 5.2 that \big{(}X_{i}\oplus\widetilde{X_{i}},E_{i}\big{)} is a Lipschitz regular unbounded Kasparov module from to and that
[TABLE]
in the topological unbounded -theory, .
Using the Kasparov module \big{(}X\oplus\widetilde{X},G\big{)} from to as input for Theorem 3.4, we may choose an even strictly positive compact operator such that , , and in Theorem 3.4 hold. In particular, we obtain an unbounded Kasparov module \big{(}X\oplus\widetilde{X},\Delta^{-1}G\big{)} from to which implements a homotopy between the unbounded Kasparov modules
[TABLE]
where by definition
[TABLE]
Let us fix an . Summarizing what has been obtained so far, we see that the proof of the theorem is finished provided that the identity
[TABLE]
holds in . We are going to apply Proposition 6.2 for our two unbounded Kasparov modules from to and the odd selfadjoint unitary operator . So we need to verify the three conditions in the statement of Proposition 6.2. For condition we have that preserves the domains of and and that both the non-graded commutators \big{[}G_{i},\Delta_{i}^{-1}G_{i}\big{]}\colon\operatorname{Dom}\big{(}\Delta_{i}^{-1}G_{i}\big{)}\to X_{i}\oplus\widetilde{X_{i}} and are in fact trivial. For condition we notice that
[TABLE]
are already even unbounded positive and regular operators (so no bounded perturbations are needed). To check the final condition , we let be homogeneous. The graded commutator has image contained in \operatorname{Dom}\big{(}\Delta_{i}^{-1}\big{)}=\operatorname{Dom}\big{(}\Delta_{i}^{-1}G_{i}\big{)} and
[TABLE]
is bounded since has image contained in \operatorname{Dom}\big{(}\Delta^{-1}\big{)} and : is bounded by construction, see Theorem 3.4. The graded commutator also has image contained in since
[TABLE]
for all and since \big{(}X_{i}\oplus\widetilde{X_{i}},E_{i}\big{)} is Lipschitz regular. Letting and denote the bounded extensions of the graded commutators and we moreover see that
[TABLE]
is bounded. It thus follows from Proposition 6.2 and Theorem 6.4 that \big{[}X_{i}\oplus\widetilde{X_{i}},\Delta_{i}^{-1}G_{i}\big{]}=\big{[}X_{i}\oplus\widetilde{X_{i}},E_{i}\big{]} in and this ends the proof of the theorem. ∎
Acknowledgements
The starting point for this paper was a couple of conversations with Bram Mesland during the thematic programme on “Bivariant -theory in Geometry and Physics” at the Erwin Schrödinger Institute in Vienna in November 2018. I would like to thank the ESI for their hospitality and support and the organizers of the thematic programme for this great opportunity to meet and discuss the unbounded approach to -theory and its applications in mathematical physics. As always, I am also grateful to my friends and collaborators Magnus Goffeng, Bram Mesland, and Adam Rennie for many good conversations on unbounded -theory and its relationship to -theory. Finally, I would like to thank the anonymous referee for her/his comments regarding spectral decomposability and its relationship to the work of Skandalis.
The author was partially supported by the DFF-Research Project 2 “Automorphisms and Invariants of Operator Algebras”, no. 7014-00145B.
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