Frobenius–Rieffel norms on finite-dimensional C*-algebras
Abstract.
In 2014, Rieffel introduced norms on certain unital C*-algebras built from conditional expectations onto unital C*-subalgebras. We begin by showing that these norms generalize the Frobenius norm, and we provide explicit formulas for certain conditional expectations onto unital C*-subalgebras of finite-dimensional C*-algebras. This allows us compare these norms to the operator norm by finding explicit equivalence constants. In particular, we find equivalence constants for the standard finite-dimensional C*-subalgebras of the Effros–Shen algebras that vary continuously with respect to their given irrational parameters.
Key words and phrases:
C*-algebras, matrix algebras, Frobenius norms, equivalence constants, conditional expectations, Effros–Shen algebras, quantum metric spaces, continued fractions2000 Mathematics Subject Classification:
Primary: 46L89, 46L30, 58B34.1. Introduction
A main goal of noncommutative metric geometry is to establish the convergence of spaces arising in the physics or operator-algebra literature [24, 25, 14, 11, 12, 17]. To accomplish this, one must equip operator algebras with compact quantum metrics, which were introduced by Rieffel [22, 23] and motivated by work of Connes [4, 5]. Then, convergence of compact quantum metric spaces is proven with quantum analogues of the Gromov–Hausdorff distance [24, 16, 15, 13, 18, 28].
In [2], the first author and Latrémolière recently exhibited the convergence of quantum metric spaces built from approximately finite-dimensional C*-algebras (AF algebras) and, in particular, convergence of the Effros–Shen algebras [8] with respect to their irrational parameters. Quantum metric spaces are obtained by endowing unital C*-algebras with a type of seminorm whose properties are inspired by the Lipschitz seminorm. A property, which is not needed in [2], but appears desirable in other context [26], is called the strongly Leibniz property. A seminorm satisfies the strongly Leibniz property on an operator algebra if
for all invertible , in which is the operator norm. This can be seen as a noncommutative analogue of the quotient rule for derivatives. Although the authors of [2] were able to prove their results without this property, Rieffel’s work on module convergence over the sphere [26] uses the strong Leibniz property, and it can be expected to play a role in the study of module convergence in general.
Let be a topological space and let . The reason that the seminorms in [2] do not likely satisfy the strongly Leibniz rule is because the seminorms are of the form
where is an element of the C*-algebra , is a C*-subalgebra of , and is a certain surjective linear map called a faithful conditional expectation. But conditional expectations are rarely multiplicative (otherwise, the strongly Leibniz property of this seminorm would come for free). Rather than replace , which provides crucial estimates, Rieffel provided another option in [27, Section 5] following his previous work in [21]: replace the operator norm with one induced by and the subalgebra . For , the Frobenius–Rieffel norm is
where is the adjoint of . If we define
then is a seminorm that is strongly Leibniz [27, Theorem 5.5].
However, this replacement comes at a cost. Following [2], we want the family of maps to vary continuously (pointwise) on a particular subset of with respect to . Thankfully, in the setting of [2], one need only verify this continuity when is finite dimensional. In this case, and are equivalent on , meaning there exist constants such that
for each . Therefore, we can replace with
which is strongly Leibniz. However, the constants need not change continuously with respect to . Therefore, our aim in this paper is to find explicit equivalence constants for the operator norm and Frobenius–Rieffel norms on finite-dimensional C*-algebras, so that we may prove the continuity of the constants with respect to . In fact, one of our main results (Theorem 5.2) shows that there exist explicit equivalence constants for the finite-dimensional C*-algebras that form the Effros–Shen algebras which vary continuously with respect to the irrational parameters that determine these algebras.
After some background on C*-algebras and the construction of the Frobenius–Rieffel norms, we provide some basic facts in the next section. Then, we find equivalence constants when is the space of complex -matrices. This provides a framework for the general case of finite-dimensional C*-algebras, which we tackle next. Our main method is to represent the conditional expectations as means of unitary conjugates for some standard subalgebras, and then extend these results to all unital C*-subalgebras by showing that although the Frobenius–Rieffel norms are not unitarily invariant, their equivalence constants are.
2. Preliminaries
The facts we state about C*-algebras in this section can be found in standard texts such as [7, 19, 20]. A C*-algebra is a Banach algebra over equipped with a conjugate-linear anti-multiplicative involution called the adjoint satisfying the C*-identity (i.e., for all ). We say that is unital if it has a multiplicative identity. If two C*-algebras are *-isomorphic, then we denote this by . Let . We denote the space of complex matrices by and its C*-norm by , the operator norm induced by the 2-norm on . We denote the identity matrix by . For , we let denote the -entry of for all , where .
Example 2.1.
Let and let . The space
is a unital C*-algebra with coordinate-wise operations; the norm is the maximum of the operator norms in each coordinate. If we set , then is the unit, which we frequently denote by . Every finite-dimensional C*-algebra is of this form up to *-isomorphism [7, Theorem III.1.1].
We denote by , so that for each and is the -entry of for all .
The following maps are needed for the construction of Frobenius–Rieffel norms.
Definition 2.2.
Let be a unital C*-algebra and let be a unital C*-subalgebra. A linear function is a conditional expectation if
-
(1)
, , and
-
(2)
, .
We say that is faithful if .
We can now define norms induced by faithful conditional expectations.
Theorem 2.3 ([21][27, Section 5]).
Let be a unital C*-algebra and be a unital C*-subalgebra. Let be a faithful conditional expectation. For all , set
This defines a norm on called the Frobenius–Rieffel norm associated to and .
The terminology for these norms is due to two facts: Rieffel introduced these norms [27, Section 5] using his work that introduced spaces called Hilbert C*-modules [21] and we show in Theorem 3.16 that one can recover the Frobenius norm using a particular C*-subalgebra.
One of the main results that makes our work in this paper possible is the fact that we can express our conditional expectations as orthogonal projections. The key property that allows this is the preservation of faithful tracial states. A state on a C*-algebra is a positive linear functional of norm . We say that is faithful if and tracial if for all . If is a unital C*-subalgebra and is a conditional expectation onto , then we say that is -preserving if .
Example 2.4.
Let and . Let such that . For every , define
where is the trace of a matrix. Then is a faithful tracial state on . In fact, all faithful tracial states on are of this form [7, Example IV.5.4]. For , we have . Thus, , and we simply denote by in this case.
A faithful tracial state allows us to define an inner product on .
Theorem 2.5 ([6, Proposition VIII.5.11]).
Let be a unital C*-algebra and let be a faithful state. Then
is an inner product on .
The following fact is well known.
Theorem 2.6 ([2, Expression (4.1)]).
Let be a unital C*-algebra, let be a unital C*-subalgebra, and let be a faithful tracial state. If is finite dimensional, then there exists a unique -preserving conditional expectation onto such that given any basis of which is orthogonal with respect to , we have
for all .
In this case, we denote the associated Frobenius–Rieffel norm on by . Now, let , let be a unital C*-subalgebra, and let such that .
- (1)
-
(2)
If , then is the unique faithful tracial state on , and we denote the conditional expectation of Theorem 2.6 induced by by . We denote the associated Frobenius–Rieffel norm by .
3. Some properties of Frobenius–Rieffel norms
In this section, we detail the subalgebras of that we will be working with and the conditional expectations given by Theorem 2.6. We also explain why we use “Frobenius” in the name of the norms of Theorem 2.3.
A partition of , denoted is a tuple , where depends on and . We need the following refinement to describe certain subalgebras of .
Definition 3.1.
Let . A formal expression in which for and
(3.1) |
is a refined partition of , denoted . Write and so that . The vectors and are the multiplicity vector and dimension vector of , respectively. We drop the subscript unless needed for clarity. In the formal expression for , we suppress if . The number of summands in (3.1) is the length of .
For example, are refined partitions of with, respectively, lengths ; multiplicity vectors ; and dimension vectors .
In what follows, we use Kronecker products and direct sums. For example, by , we mean the subalgebra
of , where is the block-diagonal matrix
with s in the entries not occupied by the s and .
Definition 3.2.
Let and let be a refined partition of . The subalgebra of corresponding to is
(3.2) |
We sometimes write instead of when the context is clear.
Example 3.3.
For each , we have and
where -copies of are in the subscript of and denotes *-isomorphism.
Example 3.4.
Observe that
Thus,
is a unital C*-subalgebra of which is not of the form (3.2), but is *-isomorphic to .
The algebra of circulant matrices provides another example of a unital C*-subalgebra of that is not of the form (3.2).
Example 3.5.
A matrix of the form
is a circulant matrix [10, 0.9.6 and 2.2.P10]. The *-algebra of circulant matrices is a unital commutative C*-subalgebra of that is *-isomorphic to . Indeed, they are simultaneously unitarily diagonalizable normal matrices.
The next definition serves as a vital intermediate step in finding equivalence constants associated to all unital C*-subalgebras and faithful tracial states of .
Definition 3.6.
Consider . For each , let
be the canonical projection onto the th summand. We say that is a standard unital C*-subalgebra if it is a unital C*-subalgebra such that for each
where . Then is a unital C*-subalgebra of
which is a unital C*-subalgebra of .
Example 3.7.
Observe that
is a standard unital C*-subalgebra of and
We note that the unital C*-subalgebra of given by
is not standard, but it is *-isomorphic to . Thus, whether a subalgebra is standard or not depends upon the larger ambient algebra.
Example 3.8.
Observe that
is not a standard unital C*-subalgebra of since is not of the form (3.2). But it is *-isomorphic to the standard unital C*-subalgebra
of . Note and .
Up to unitary equivalence, standard unital C*-subalgebras comprise all unital C*-subalgebras of . To be clear, let be two unital C*-subalgebras. We say that and are unitarily equivalent (with respect to ) if there exists a unitary such that is a bijection from onto , in which case we write . Sometimes the term spatially isomorphic is used for unitary equivalence, but spatially isomorphic is also sometimes used in a more general sense.
Unitary equivalence is stronger than *-isomorphism. For example, the unital C*-subalgebras
of are *-isomorphic but not unitarily equivalent in (they are unitarily equivalent in , but we are viewing them as subalgebras of ). We now state the following well-known result.
Theorem 3.9 ([7, Theorem III.1.1, Corollary III.1.2, and Lemma III.2.1]).
Every unital C*-subalgebra is unitarily equivalent with respect to to for some refined partition of , and
Furthermore, any unital C*-subalgebra of is unitarily equivalent, with respect to , to a standard unital C*-subalgebra.
For example, the *-algebra of circulant matrices of Example 3.5 is unitarily equivalent with respect to to , not just *-isomorphic to it [10, 2.2.P10]. Also, the subalgebras and of Example 3.8 are unitarily equivalent, not just *-isomorphic.
We use Theorem 3.9 to generalize our results to all unital C*-subalgebras once we verify our results for the standard subalgebras. One of the advantages of working with standard unital C*-subalgebras is that they have canonical bases which are orthogonal with respect to the inner products induced by faithful tracial states.
Definition 3.10.
Consider . For each and , let have a in the -entry of the th summand and zeros in all other entries and all other summands. We call a matrix unit. If , then we suppress the superscript .
Any standard unital C*-subalgebra has a standard basis (up to ordering of terms) given by matrix units or sums of distinct matrix units, which we denote by .
Example 3.11.
For the subalgebra of Example 3.7, we have .
Example 3.12.
For , we have
For , we have
For , we have .
All cases in the example above can be recovered as follows.
Remark 3.13.
Let be a standard unital C*-subalgebra of Definition 3.6. Thus, there exists a refined partition of such that , and we have that
where we regard a sum over an empty set of indices as zero.
For these bases, although some of the elements are sums of distinct matrix units, we note that the summands are from distinct blocks. For example, for , no element of the form appears in the standard basis. This easily verified fact and more are summarized in the following.
Theorem 3.14.
Let be a standard unital C*-subalgebra. For each , let (i.e., ). The following hold:
-
(1)
for every with .
-
(2)
If , then if and only if and ( or ).
-
(3)
If , then is an orthogonal basis of with respect to .
We now provide an explicit way of calculating the conditional expectations associated with standard unital C*-subalgebras. This is a complete generalization of [1, Proposition 2.8].
Theorem 3.15.
Let be a standard unital C*-subalgebra. For each and , let , and let denote the cardinality of . Let satisfy . If , then
Proof.
Fix . Since is the set of indices for the nonzero entries of the basis element contained in the th summand, we know that
If , then for any and . We use this fact repeatedly in the following calculation. Let and observe that
We next show how the Frobenius–Rieffel norms recover the Frobenius norm.
Theorem 3.16.
For all ,
where is the Frobenius norm normalized with respect to .
Proof.
The next two examples show that Frobenius–Rieffel norms are not generally sub-multiplicative or unitarily invariant.
Example 3.17.
Example 3.18.
Consider
and the unitary
Following similar calculations as the last example, we conclude
4. Equivalence constants for the operator norm
As discussed in the introduction, it is important to be able to compare the Frobenius–Rieffel norms with the operator norm. Theorem 2.3 says that
for all , any unital C*-subalgebra , and any conditional expectation onto . This equality is achieved by the identity matrix. Thus, the nontrivial task is to find a constant such that
for all
We begin with some general results and then focus on the case of . Then, we move to the general case, which is more involved since the Frobenius–Rieffel norms depend on the underlying subalgebra and faithful tracial state. We begin with an inequality that allows us to avoid dealing with .
Lemma 4.1.
Let be a unital C*-subalgebra, let be a faithful tracial state on , and let The following are equivalent.
-
(1)
for all positive .
-
(2)
for all .
Proof.
We begin with . Suppose for all positive . Then for all . Since , we see that
For , suppose that
for all . Then . Thus, for all positive . ∎
The next lemma allows us to extend our results from standard unital C*-subalgebras to all unital C*-subalgebras. The following fact is surprising since, at the end of the last section, we showed that the Frobenius–Rieffel norms are not unitarily invariant in general. Also, it can be the case that for certain , but the equivalence constants are the same for uniatrily equivalent subalgebras .
Lemma 4.2.
Let be a faithful tracial state on , let be unitarily equivalent (with respect to ) unital C*-subalgebras , and let The following are equivalent.
-
(1)
for all .
-
(2)
for all .
Proof.
The argument is symmetric, so we prove only . Fix an orthogonal basis for with respect to . Since is a linear bijection, is a basis for . Furthermore, if , we have
Hence, is an orthogonal basis for with respect to .
We next present a basic lemma about positive matrices.
Lemma 4.3.
If for some positive , then .
Proof.
Since , it follows that is invertible if or . Thus, the spectrum of the self-adjoint matrix is contained in the interval . ∎
Lemma 4.4 is our main tool in providing equivalence constants. It is motivated by the notion of “pinching” in matrix analysis (see [3]).
Lemma 4.4.
Let be positive. If is a mean of unitary conjugates of , (the transpose of ), or , one of which is itself, then
Proof.
Since is positive, a unitary conjugate of , , or is also positive (and has the same operator norm as ). Suppose that
is a mean of unitary conjugates of , , or and that itself. Since is positive, the previous lemma ensures that
Consequently,
which completes the proof. ∎
We first apply this lemma to the following family of unital C*-subalgebras.
Theorem 4.5.
Let where and .
If is positive, then
Moreover,
for all .
Proof.
Consider the unitary , where is a primitive th root of unity. Let . We may write as blocks in the following way
where with for each and , and and denote the remaining entries of . By Theorem 3.15, it follows that
On the other hand, a direct computation shows that
Hence, . By Lemma 4.4, we have that .
We can now use the ideas from Theorem 4.5 to calculate equivalence constants for a subalgebra of the form for arbitrary (Definition 3.2). The idea of the proof is as follows. Assume we want to project a matrix of the form
onto the subalgebra of matrices of the form
We can do this in two steps. First project onto
which is the setting of Theorem 4.5. Then project onto
The proof of the next theorem shows how we can represent this final projection using a mean of unitary conjugates, which allows us to utilize Lemma 4.4 as done in the proof of Theorem 4.5. The reason for this two-step approach is that it does not seem feasible to represent the projection directly onto the desired subaglebra as a mean of unitary conjugates.
Theorem 4.6.
Consider such that , where . Set and . If is positive, then
Moreover,
for all
Proof.
We write as the composition of two maps. For each , set
(4.1) |
that is, , and
etc. Now set and note that . By Theorem 4.5, we have for all positive .
For each let to be the circulant matrix with all zeros in the first row, except for a in the th position for Then we define for where For any positive , define
Example 4.7.
We calculate the values of for the following subalgebras of
For , we have and . Thus .
For , we have and . Thus .
For , we have and . Thus .
For , we have and . Thus .
We also note that for the subalgebra , we have , , and
Thus, combining Theorem 4.6 with Lemma 4.2 and Theorem 3.9, we have found equivalence constants for Frobenius–Rieffel norms constructed from any unital C*-subalgebra of built from natural structure (the dimensions of the terms of the block diagonals of the given subalgebra).
Table 1 outlines the equivalence constants for all unital *-subalgebras of for . The second column contains equivalence constants suggested by brute force using software (this was done by making software calculate the operator and Frobenius–Rieffel norms of many matrices, and then making a guess), which we think might be the sharp equivalence constants. The third column contains the theoretical equivalence constant found in Theorems 4.5, 4.6. Our goal in this paper is not to find the sharp equivalence constants, but just explicit ones that afford us some continuity results as mentioned in the first section. It remains an open question to find the sharp constants, and this table suggests that we may have found the sharpest constants in some cases.
Algebra | Guess of Sharp Equiv. Const. | Theorem 4.6 Equiv. Const. |
---|---|---|
4.1. The general case
We now study the case of , which is much more involved for two main reasons. First, as seen in Example 3.11, the canonical basis elements for standard unital C*-subalgebras of can have non-zero terms in multiple summands, which requires more bookkeeping than the previous section. Second, the Frobenius–Rieffel norms now vary on an extra parameter: the faithful tracial state. In the case, the only faithful tracial state is , so this was not an issue. For instance, consider and the subalgebra
To build a Frobenius–Rieffel norm on with respect to , we also need a faithful tracial state on . We could take on (see Example 2.4). Hence, taking into account the expression for the associated conditional expectation of Theorem 3.15, we need to keep track of how the coefficients and impact the construction of the Frobenius–Rieffel norm since appears in both summands. Thus, we cannot simply view as a subalgebra of and proceed to use the previous section since we would lose track of the weights since has a unique faithful tracial state. The following definition environment allows us to collect all the terms that we use to find our equivalence constants in this much more involved setting. We note that we generalize the constants from Theorem 4.6.
Definition 4.8.
Let be a standard unital C*-subalgebra, where for each , we have with . We denote and .
Next, we collect the data we need associated to a given faithful tracial state. Let such that , and let be the canonical orthogonal basis for given by matrix units.
Define:
-
(1)
,
-
(2)
, where is the number of blocks of in the th summand of for each ,
-
(3)
, where is the number of nonzero entries of the basis element for each ,
-
(4)
and
-
(5)
, where is the number of times there is a nonzero entry of in the th summand of for each and
Theorem 4.9.
Consider . For each , consider such that . Set
Let such that . If is positive, then
and, moreover,
for all .
Proof.
We recover using a mean of unitary conjugates in two steps. Let . Suppose the th block of has dimension (see Expression (4.1)). Set and note that . Then, let
where is a primitive th root of unity.
Using the convention for in Notation 4.8, we then define, for , the matrix to be the circulant matrix with all zeros in the first row, except for a in the th position for . Set for , and let
Then define by
Since , we know by Lemma 4.4. We also have that by construction. Hence
which completes the proof by Lemma 4.1. ∎
The values of do not appear in the calculations above. This makes sense because the case of Theorem 4.9 is essentially the case when since the non-zero entries of a basis element do not appear in multiple summands, and so the different coordinates of do not appear and we simply work with . Thus, we now move towards the case when the non-zero entries of our basis elements can appear in multiple summands, such as in Example 3.7 and as in the subalgebras defined before Theorem 5.2. To provide intuition for the following proof, we revisit the example at the beginning of the section. Consider and the C*-subalgebra
The first step of the following proof is to project an onto an element of the form . Next, in order to project into , we view as and we view elements of as . Then we use a mean of unitary conjugates in to project to an element of the form , which is an element in . To form the unitaries, begin with . Next, since the -entry in repeats in the -entry and -entry, we permute the first, third, and fourth column of two times to get two more unitaries
If we permute these columns one more time, then we obtain . Note that
Using Definition 4.8, note that since the standard basis elements of are and .
Theorem 4.10.
Let such that . Let be a standard unital C*-subalgebra of . If is positive, then
and, moreover,
for all .
Proof.
We then define
which gives us for all positive .
Suppose is the dimension of the th block of and is the total number of blocks of . For the following, we view and as subalgebras of , where . Let
We construct by permuting the blocks of in the following way. If the th block of is not repeated, then fix . Next, assume that the th block of is repeated and that the th block is the first position this repeated block appears. Assume that the th block is the next block to the right that the the th block is repeated. Then stays in the same rows it occupied in , but its columns permute to the columns (in ) of the th block in . If the th block is repeated, then repeat this process with . However, if the th block is not repeated, then permute the columns to the columns of the th block. Continue in this way until all blocks are either permuted or fixed depending on repetition or lack thereof, which gives us . Repeat this process to make , where is defined in (3) of Definition 4.8 (see the example before the statement of the theorem). Note that . Define by
which satisfies
for all positive by Lemma 4.4.
We can use the previous theorem to find equivalence constants for all unital *-subalgebras by Lemma 4.2.
5. An application to Effros–Shen algebras
To finish, we now apply our main result to the finite-dimensional C*-algebras in the inductive sequence used by Effros and Shen in the construction of their AF algebras from the continued fraction expansion of irrational numbers [7, Section VI.3], [8]. These algebras provide a suitable example to test our results. Indeed, in [2], it was shown that the Effros–Shen algebras vary continuously with respect to their irrational parameters in a noncommutative analogue to the Gromov–Hausdorff distance, called the dual Gromov–Hausdorff propinquity [15]. A crucial part of this result is the fact that each Effros–Shen algebra comes equipped with a unique faithful tracial state and that the faithful tracial states themselves vary continuously with respect to the irrational parameters. Therefore, to test our results in the previous section, we will see that for the Frobenius–Rieffel norms that are built from these faithful tracial states, this continuity passes through to the equivalence constants. This further displays how far-reaching the information of the irrational parameters appears in structures related to the Effros–Shen algebras.
First, given an irrational , the Effros–Shen algebras are built using the continued fraction expansion of . The continuity results in [2] were established using the Baire space, a metric space that is homeomorphic to with its usual topology. The Baire space is the set of positive integer sequences, which is in one-to-one correspondence with via the continued fraction expansion, equipped with the Baire metric. We begin reviewing continued fractions and the Baire space. Background on continued fractions can be found in many introductory number theory texts, such as [9].
Let be irrational. There exists a unique sequence of integers (where ) with for all such that
When , we have that . The sequence is called the continued fraction expansion of .
To define the Baire space, first let denote the set of positive integer sequences. The Baire metric on is defined by
The metric space is the Baire space. In particular, the distance in the Baire metric between two positive integer sequences is less than if and only if their terms agree up to . We now state the following well-known result in the descriptive set theory literature.
Proposition 5.1 ([2, Proposition 5.10]).
The map
is a homeomorphism with respect to the usual topology on and the Baire metric.
Thus, convergence of a sequence of irrationals to an irrational in the usual topology on can be expressed in terms of their continued fraction expansions using the topology induced by the Baire metric.
Next, we define the finite-dimensional C*-subalgebras of the Effros–Shen algebras. For each , define
and set
and
The sequence of convergents converges to . In fact, for each ,
We now define the C*-algebras with which we endow Frobenius–Rieffel norms. We set and, for each , we set
For the subalgebras, define
(5.1) |
where there are copies of on the diagonal in the first summand of . This is a unital *-monomorphism by construction. For ,
For each , set
which is a standard unital C*-subalgebra of .
To complete the construction of the Frobenius–Rieffel norm, we need to define a faithful tracial state. We begin with
Then set
so for all , we have
For each , the Frobenius–Rieffel norm on associated to and to the unital C*-subalgebra is denoted by
We conclude the paper with the following theorem, which shows that the equivalence constants we found in this paper are natural in the sense that they reflect the established continuity of the Effros-Shen algebras with respect to their irrational parameters.
Theorem 5.2.
Let and . Then
for all . If is a sequence in converging to some , then
Proof.
First, we gather the necessary information from the canonical basis of given by matrix units. Let
be the set of basis elements that span elements of the form . Let
be the set of basis elements that span elements of the form . Note for , we have . Thus, the canonical basis for is
Using Definition 4.8, we have
and
Next
and
where the second term is given at the end of the proof of [2, Lemma 5.5], and finally
Thus, we conclude that the equivalence constant of Theorem 4.10 is
(5.2) |
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