Abstract
We consider a family of associative algebras, defined as the quotient of a free algebra with the ideal generated by a set of multi-parameter deformed commutation relations between four generators consisting of five quantum plane relations between pairs of generators and one sub-quadratic relation inter-linking all four generators. For generic parameter vectors, the center and the commutants of the two of the generators are described and conditions on the parameters for these commutants to be itself commutative or non-commutative are obtained.
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Keywords
Classification
1 Introduction
Commuting elements in non-commutative algebra are important for representation theory, classifications, interplay with harmonic analysis and spectral theory, topology and algebraic geometry, operator algebras and applications in Physics and Engineering. For example, commutants or centralisers, maximal commutative subalgebras of crossed product \(C^*\)-algebras and von Neumann algebras play a central role in investigation of representations, classifications and in structure of state space [1–6]. In particular, maximal commutative subalgebras are essential objects for the famous Kadison-Singer conjecture stated in a pioneering 1959—paper by Kadison and Singer [7], equivalent to the paving conjecture [8, 9] and several conjectures important for wavelets and frames analysis and applications in signal and image processing, one of them the well-known Feichtinger conjecture [10] in frame theory. For the key role of maximal commutative subalgebras for establishing interplay between Kadison-Singer conjecture, properties of projections, topological dynamical systems and compactifications of topological spaces see for example [11]. Commutants and maximal commutative subalgebras in generalized crossed product algebras arising from non-invertible dynamics and actions are used in the important ways in the general operator and spectral theory approach to wavelets analysis and investigation of wavelets on fractals [12–16]. The description of commuting elements and of corresponding commuting operators in the representing operator algebra, or in other words the problem of explicit description of commutative subalgebras is important in description and classifications of operator representations and applications of non-commutative algebras [17–27]. The commuting operators and commuting elements in rings and algebras also are important in study of integrable systems and non-linear equations. Further discussions in connection to this topic and numerous references can be found for instance in the book [28] devoted to commuting elements in the algebra defined by the \(q\)-deformed Heisenberg relations (see also [29, 30]).
The centers and commutants of elements or subsets in non-commutative algebras are fundamentally important subsets of an algebra or a ring in this context (see for example [31–39] and references therein). The center consists of elements commuting with all elements in the algebra, is the intersection of the commutants of all elements in the algebra and so is always a commutative subalgebra. The commutants of elements or subsets of elements in an associative algebra are subalgebras which contain the center of the whole algebra as its subalgebra, but may be commutative or may be not depending on the structure of the algebra and the subset for which the commutant is considered.
In this article we consider the centers and commutants for an interesting multiparameter family of associative algebras generated by four generators and six sub-quadratic relations involving six deformation parameters. The five of these relations are the famous quantum plane relations playing important role in quantum groups, \(q\)-calculus and quantum mechanics, operator algebras and non-commutative geometry (rotation algebras, non-commutative tori, etc.). The sixth relation is interconnecting the four generators by a special \(q\)-deformed quadratic relation expressing the sum of two generators as \(q\)-commutator of the other two of the generators:
where \(\mathbf {q}=(q_0, q_1, q_2, q_3, q_4, q_5) \in \mathbb {C} ^6\).
All of (1b)–(1f) are of the type \(\textit{XY}\,-\,q\textit{YX} = 0\), which is the so called quantum plane relation studied in non-commutative geometry. Equation (1a) resembles the Sylvester equation \(AX\) \(-\) \(XB = C\) and the Lyapunov equation \(AX + XA^* = -Q\), both of which are encountered in control theory. Specializing \(S = \lambda I\) and \(T = (1-\lambda ) I\) (where \(I\) denotes the multiplicative identity) and \(q_1,\,\ldots ,\,q_5 = 1\), the relations (b)–(f) become trivial and (a) becomes \(\textit{AB}-q_0\textit{BA} = I\). This is a generalization of the Heisenberg canonical commutation (\(q_0 = 1\)) and anti-commutation (\(q_0 = -1\)) relations, which are used in quantum mechanics to describe systems with one degree of freedom. More on the algebras defined by \(q\)-deformed Heisenberg relations (called also \(q\)-Weil relations) and commuting elements in such algebras can be found in the monograph [28] and references there.
It is a well known interesting issue whether it is possible to realize a given family of commutation relations in one or another way using matrices or differential operators or other types of linear operators, or any objects for which (1) makes sense, for example elements of some associative algebra. When the realization by the operators of a specific type is possible, further description and classifications of the representations of the relations by the operators of such type arise and often becomes a problem of great interest. It often requires insights both in the algebraic structure of the commutation relations and in the properties of the involved classes of operators. In algebraic contexts it often leads to interesting combinatorial identities and problems, while in the context of \(*\)-representations (involutive representations) and operator algebras it involves also spectral theory of possibly unbounded operators in the finite-dimensional or infinite-dimensional spaces.
The relations (1) provide an interesting example in this respect. For a first taste of what can happen in (1a)–(1c) when \(A, B, S, T\) are complex \((n \times n)\)-matrices, consider the case when \(A\) and \(B\) are hermitian and \(q_0\) lies on the unit circle. Note that \(\Vert X \Vert _F^2 = {{\mathrm{tr}}}(X^* X)\) defines a norm \(\Vert X \Vert _F\) on \(\mathbb {C} ^{n \times n}\) (this is the so called Frobenius norm). Since \(A, B\) are hermitian and \(q_0q_0^* = 1\), \((AB - q_0BA)^* = -q_0^*(AB - q_0BA)\), and thus
Using (1b,c) and the fact that \({{\mathrm{tr}}}(XYZ) = {{\mathrm{tr}}}(ZXY)\) for all \((n \times n)\)-matrices \(X, Y, Z\), this implies that
Thus, if \(q_2 = q_0\) and \(q_0q_1 = 1\), \(A, B\) must satisfy \(AB - q_0BA = 0\), and \(S, T\) must satisfy \(S = -T\). In particular, if \(q_0 = q_1 = q_2 = 1\), \(A\) and \(B\) must commute. It is not difficult to see that for many other conditions on the parameters this argument breaks down. This could be interpreted as an indication that the algebraic structures defined by these relations and their representations might have rich dependence on the interplay between the values of the six deformation parameters.
In this article, we provide further indication of richness of the structure of this family of algebras depending on the values of the deformation parameters, by considering some important properties of the algebra with generators and relations (1), especially focussing on centers and commutants. As these algebras are defined as the quotient algebra \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \) of a free algebra on six generators by the ideal associated to the commutation relations (1), in order to be able to compute in this algebra it is particularly important to be able to decide the equality of the elements in the algebra, since using the relations (1), the same element can be expressed in many ways, and it is not obvious whether or not two given expressions are equal. To handle this, one needs a normal form for elements in \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \), which for the relations of the type (1) amounts to finding a basis for \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \) for various choices of parameters. In Sect. 2, we indicate that relations are more subtle than it may seem on the first sight as there are more relations than generators, and for many values of parameters these relations imply some further much more special relations between generators bringing significant restrictions on the size or the structure of the bases and thus on various further properties and computations in the algebra. Finding in a systematic way bases for the algebras for various choices of parameters becomes an elaborate task requiring non-trivial use of the Bergman’s diamond lemma and relations (1) as well as some symmetries of the relations and their consequences for case reductions of various subtle parameter subsets. It appears in the course of this analysis, that the basis takes a somewhat simpler form for a large subset of parameters given by a system of certain inequalities. This set of “generic” parameters, as we call it, and the bases yield useful grading structures, used in Sect. 3 to describe the commutants of the main generators \(A\) and \(B\) by describing the spanning sets. In Sect. 4, the results from the preceding sections combined with further computations are used to describe explicitly the center by providing its basis depending on the deformation parameters. While the center of an algebra is always a commutative subalgebra, as an intersection of commutants of all elements of the algebra, the commutants of elements or non-trivial subsets of a non-commutative algebra are subalgebras which are not necessarily themselves commutative. For some classes of algebras it is possible to prove that commutants of the elements are commutative. Investigating whether this is a case and finding examples and counterexamples for such commutativity property for a particular family of algebras defined by generators and specific relations is an important problem which is often highly non-trivial, especially so when the defining relations are dependent on parameters. In Sect. 5, we provide necessary and sufficient conditions on \(\mathbf {q}\) within the set of “generic” parameters, for \(\fancyscript{C}(A)\) and \(\fancyscript{C}(B)\) to be commutative, thus also providing necessary and sufficient conditions on “generic” parameters for when these commutants are not-commutative. The results of these paper suggest that the description and further in-depth analysis of the structure of the commutants of these and other elements and subsets for the family of algebras considered in this paper both for “generic” as well as for non-generic parameters is an interesting and rich open problem.
2 First Steps: Reordering and Basis
Let \(\fancyscript{F}\) be the free unital associative algebra over \(\mathbb {C}\) generated by the set \(\{ A, B, S, T\}\). For \(\mathbf {q} = (q_0, q_1, q_2, q_3, q_4, q_5) \in \mathbb {C} ^6\) let \(\fancyscript{J}(\mathbf {q}) \) be the ideal generated by the set
or equivalently the ideal in \(\fancyscript{F}\) generated by the relations
where \(\equiv \) denotes equivalence modulo \(\fancyscript{J}(\mathbf {q}) \).
From (3) it is not too hard to derive the additional relations
The implications of these relations depend on which of the involved scalar expressions are zero and which are non-zero. There are also a few more expressions in the parameters that change the situation if they are zero. Only the generic case will be considered here.
Definition 2.1
A parameter vector \(\mathbf {q} = (q_0, q_1, q_2, q_3, q_4, q_5) \in \mathbb {C} ^6\) is generic if
For generic \(\mathbf {q}\) it follows from (3), (4) and (5) that
Since (3) can be used to put the symbols in the monomials in the order \(T, S, B, A\), this means that any monomial that has two symbols from \(\{ S, T \}\) and additionally one symbol from \(\{ A, B, S, T \}\) is \(\equiv 0\). Thus it seems plausible that the set
is a basis for \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \). This can be shown using the Diamond Lemma for ring theory [40].
Sums of the form \(\sum _{i = 0}^{n - 1} q^i\) will often appear in what follows, so it is convenient to have a more compact notation for them.
Definition 2.2
For \(q \in \mathbb {C} \) and \(n \in \mathbb {N}\), let
\(\left\{ n \right\} _{q}\) is called the n:th q-natural number.
To express the product of two general elements in the basis \(\fancyscript{B}\), it is necessary to be able to rewrite monomials of the form \(A^mB^n\) so that the \(B\):s are moved to the left of the \(A\):s.
Lemma 2.1
Let \(\mathbf {q} = (q_0,\,\ldots ,\,q_5) \in \mathbb {C} ^6\) be generic. Then the following formula holds in \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \) for \(m, n \ge 1, (m, n) \ne (2, 2)\).
The formula can be proved for most \((m, n)\) by induction first on \(m\) and then on \(n\), or by induction first on \(n\) and then on \(m\). The exceptional point \((m, n) = (2, 2)\) makes it necessary to use both orders of induction to cover all \((m, n) \ne (2, 2)\). We omit the elaborate details of the proof.
Equation (7) does not hold for \((m, n) = (2, 2)\). The reordering formula for \((m, n) = (2, 2)\) is instead
This formula agrees with (7) except for the extra \(TS\)-term on the right side.
Let \(\fancyscript{M}\) be the set of monomials in \(\fancyscript{F}\) and define for \(Y \in \fancyscript{M} \)
Then \(\fancyscript{F}\) has an \(\mathbb {N}^2\)-gradation \(\{ A_{(m, n)} \}_{(m, n) \in \mathbb {N}^2}\) given by
All elements in the generating set of \(\fancyscript{J}(\mathbf {q}) \) are homogeneous in this gradation and thus the induced gradation of \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \) is well defined. If \(m, n \ge 1\) and \((m, n) \ne (2, 2)\) then a basis for the homogeneous component of degree \((m, n)\) is given by
3 Commutants of \(A\) and \(B\)
The commutant of an element \(X \in \fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \) is the set of all elements that commute with \(X\). It will be denoted by \(\fancyscript{C}(X)\). In this section, spanning sets for \(\fancyscript{C}(A)\) and \(\fancyscript{C}(B)\) are described for generic \(\mathbf {q}\).
In general, a commutant of a homogeneous element is spanned by the homogeneous elements of the commutant. This means that it is enough to find all homogeneous elements that commute with \(A\) or \(B\). Let \(X_{m, n}\) denote a general homogeneous element of degree \((m, n)\). For \(m, n \ge 1\), \((m, n) \ne (2, 2)\), such an element can be uniquely written as
with \(c_1, c_2, c_3 \in \mathbb {C} \). Since \(TS\) commutes with every \(Y \in \{ A, \, B, \, S, \, T \}\) (in fact \(YTS \equiv TSY \equiv 0\) by (6)), it is general enough to consider \(X_{m, n}\) of the form (9) when \((m, n) = (2, 2)\) as well. When \(m = 0\) or \(n = 0\), the homogeneous elements of degree \((m, n)\) are of the form \(X_{0, n} = c_1B^n\) and \(X_{m, 0} = c_1A^m\) respectively.
Using the defining relations (3) and the reordering formula (7), the commutators of \(X_{m, n}\) with \(A\) and \(B\) can be computed. For \(m, n \ge 1, (m, n) \ne (1, 2)\), the commutator of \(X_{m, n}\) with \(A\) is
If \((m, n) = (1, 2)\) then there is an additional term
on the right side. For \(m = 0\), the commutator is
and \([X_{m, 0}, A] \equiv 0\) for all \(m\).
For \(m, n \ge 1, (m, n) \ne (2, 1)\), the commutator of \(X_{m, n}\) with \(B\) is
If \((m, n) = (2, 1)\) then there is an additional term
on the right side. For \(n = 0\), the commutator is
and \([X_{0, n}, B] \equiv 0\) for all \(n\).
The computations are summarised in the following lemma.
Lemma 3.1
Let \(\mathbf {q} = (q_0,\,\ldots ,\,q_5) \in \mathbb {C} ^6\) be generic.
\(\fancyscript{C}(A)\) is the linear subspace of \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \) spanned by the elements listed in the following table.
Element (\(m, n\) range over \(\mathbf {N}^+\)) | Conditions |
---|---|
\(I\) | — |
\(TS\) | — |
\(A^m\) | — |
\(B^n\) | \(1 - q_0^n = \left\{ n \right\} _{q_0q_2} = \left\{ n \right\} _{q_0q_4} = 0\) |
\(c_1B^nA^m + (c_2 S + c_3 T)B^{n - 1}A^{m - 1}\) | \(K_{(m, n)} \begin{bmatrix} c_1&c_2&c_3 \\ \end{bmatrix}^T = 0\) |
Here,
for \((m, n) \ne (1, 2)\) and
\(\fancyscript{C}(B)\) is the linear subspace of \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \) spanned by the elements listed in the following table.
Element (\(m, n\) range over \(\mathbf {N}^+\)) | Conditions |
---|---|
\(I\) | — |
\(TS\) | — |
\(A^m\) | \(q_0^m - 1 = \left\{ m \right\} _{q_1 / q_0} = \left\{ m \right\} _{q_3 / q_0} = 0\) |
\(B^n\) | — |
\(c_1 B^nA^m + (c_2 S + c_3 T) B^{n - 1}A^{m - 1}\) | \(L_{(m, n)} \begin{bmatrix} c_1&c_2&c_3 \\ \end{bmatrix}^T = 0\) |
Here,
for \((m, n) \ne (2, 1)\) and
4 The Center of \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \)
The center of \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \) is the set of elements that commute with every element of \(\fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \). It will be denoted by \(\fancyscript{Z}\). In this section, \(\fancyscript{Z}\) is described for generic \(\mathbf {q}\).
Lemma 4.1
Let \(\mathbf {q} = (q_0,\,\ldots ,\,q_5) \in \mathbb {C} ^6\) be generic. Then \(\fancyscript{Z} = \fancyscript{C}(A) \cap \fancyscript{C}(B)\).
Proof
Let \(X\) be a general homogeneous element that commutes with both \(A\) and \(B\). Then \(X\) commutes with \(S + T\) by (3a). It will be shown that \(X\) commutes with \(S\) and \(T\) as well. There are four cases depending on the degree of \(X\).
If \(X\) has degree \((0, n)\), then \(X \equiv c_1B^n\) for some \(c_1 \in \mathbb {C} \). Then
If \(X\) has degree \((m, 0)\), then \(X \equiv c_1A^m\) for some \(c_1 \in \mathbb {C} \). Then
If \(X\) has degree \((1, 1)\), then \(X \equiv c_1BA + c_2S + c_3T\) for some \(c_1, c_2, c_3 \in \mathbb {C} \). Then
The right side can be zero only if \(c_1 = c_3 - c_2 = 0\) since \(\mathbf {q}\) is generic. But then \(X \equiv c_3 (S + T)\), so
Since \(X\) is assumed to commute with \(A\) and \(B\), the right side must be zero, which implies that \(c_3 = 0\) since \(\mathbf {q}\) is generic. Thus \(X \equiv 0\), and so \(X\) commutes with \(S\) and \(T\).
Finally, if \(X\) has degree \((m, n)\) with \(m, n \ne 0\) and \((m, n) \ne (1, 1)\) then
for some \(c_1, c_2, c_3, c_4 \in \mathbb {C} \) (with \(c_4 = 0\) unless \((m, n) = (2, 2)\)). Then
Theorem 4.1
Let \(\mathbf {q} = (q_0,\,\ldots ,\,q_5) \in \mathbb {C} ^6\) be generic and suppose that \(q_0\) is not a root of unity. Then a basis for \(\fancyscript{Z}\) is given by the elements listed in the following table.
Element (\(m, n\) range over \(\mathbb {N}^+\)) | Conditions |
---|---|
\(I\) | — |
\(TS\) | — |
\(SB^{n - 1} A^{m - 1}\) | \(1 - q_0^{n - 1}q_3 = q_0^{m - 1} - q_2 = 0\) |
\(TB^{n - 1}A^{m - 1}\) | \(1 - q_0^{n - 1}q_1 = q_0^{m - 1} - q_4 = 0\) |
Moreover, this basis contains at most one element of the form \(SB^{n - 1} A^{m - 1}\) and at most one element of the form \(TB^{n - 1} A^{m - 1}\). Thus, \(\fancyscript{Z}\) has dimension at most four.
Proof
By Lemma 4.1, it is enough to show that the listed elements form a basis for \(\fancyscript{C}(A) \cap \fancyscript{C}(B)\). Spanning sets for \(\fancyscript{C}(A)\) and \(\fancyscript{C}(B)\) are given by Lemma 3.1; denote them by \(\fancyscript{B}(A)\) and \(\fancyscript{B}(B)\) respectively. Then \(\fancyscript{C}(A) \cap \fancyscript{C}(B)\) is the linear space spanned by \(\fancyscript{B}(A) \cap \fancyscript{B}(A)\). Now, \(I, TS \in \fancyscript{B}(A) \cap \fancyscript{B}(B)\) always. For \(m, n \ge 1\), \(A^m \notin \fancyscript{B}(B)\) and \(B^n \notin \fancyscript{B}(A)\) since \(q_0\) is not a root of unity, and thus \(A^m, B^n \notin \fancyscript{B}(A) \cap \fancyscript{B}(B)\). An element in \(\fancyscript{B}(A) \cap \fancyscript{B}(B)\) of the form \(c_1B^nA^m + c_2SB^{n - 1}A^{m - 1} + c_3TB^{n - 1}A^{m - 1}\) with \(m, n \ge 1\) must have \(c_1 = 0\) since \(q_0\) is not a root of unity. The coefficient \(c_2\) may be non-zero if and only if \(1 - q_0^{n - 1}q_3 = q_0^{m - 1} - q_2 = 0\). Since \(q_0\) is not a root of unity, this can happen for at most one value of \((m, n)\). Similarly, \(c_3\) may be non-zero if and only if \(1 - q_0^{n - 1}q_1 = q_0^{m - 1} - q_4 = 0\), and this can happen for at most one value of \((m, n)\). Thus the listed elements span \(\fancyscript{C}(A) \cap \fancyscript{C}(B)\), and since they are linearly independent they form a basis.
Theorem 4.2
Let \(\mathbf {q} = (q_0,\,\ldots ,\,q_5) \in \mathbb {C} ^6\) be generic and suppose that \(q_0\) is a root of unity. Let \(d\) be the smallest positive integer such that \(q_0^d = 1\). Then a basis for \(\fancyscript{Z}\) is given by the elements listed in the following table.
Element (\(m, n\) range over \(\mathbb {N}^+\)) | Conditions |
---|---|
\(I\) | — |
\(TS\) | — |
\(A^m\) | \(d | m, q_1^m = q_3^m = 1, q_1 / q_0, q_3 / q_0 \ne 1\) |
\(B^n\) | \(d | n, q_2^n = q_4^n = 1, q_0q_2, q_0q_4 \ne 1\) |
\(SB^{n - 1}A^{m - 1}\) | \(d | m - 1 - r_2, d | n - 1 + r_3, q_2 = q_0^{r_2}, q_3 = q_0^{r_3}\) |
\(TB^{n - 1}A^{m - 1}\) | \(d | n - 1 + r_1, d | m - 1 - r_4, q_1 = q_0^{r_1}, q_4 = q_0^{r_4}\) |
\(B^nA^m + (c_S S + c_T T) B^{n - 1}A^{m - 1}\) | \(d | m, d | n, q_1^mq_4^n = q_2^nq_3^m = 1\) |
and in addition | |
\(\begin{array}{l} q_2 + 1 / q_2 = q_4 + 1 / q_4 \text { if } (m, n) = (1, 2) \\ q_1 + 1 / q_1 = q_3 + 1 / q_3 \text { if } (m, n) = (2, 1) \\ \end{array}\) |
Here,
and
Proof
By Lemma 4.1, it is enough to show that the listed elements form a basis for \(\fancyscript{C}(A) \cap \fancyscript{C}(B)\). Spanning sets for \(\fancyscript{C}(A)\) and \(\fancyscript{C}(B)\) are given by Lemma 3.1; denote them by \(\fancyscript{B}(A)\) and \(\fancyscript{B}(B)\) respectively. Then \(\fancyscript{C}(A) \cap \fancyscript{C}(B)\) is the linear space spanned by \(\fancyscript{B}(A) \cap \fancyscript{B}(B)\). Now, \(I, TS \in \fancyscript{B}(A) \cap \fancyscript{B}(B)\) always, and
and
Assume now that \(m, n \ge 1, (m, n) \ne (1, 2)\) and \((m, n) \ne (2, 1)\). An element of the form \(c_1B^nA^m + c_2SB^{n - 1}A^{m - 1} + c_3TB^{n - 1}A^{m - 1}\) lies in \(\fancyscript{B}(A) \cap \fancyscript{B}(B)\) if and only if \(K_{(m, n)} [c_1 \, c_2 \,c_3]^T = 0\) and \(L_{(m, n)} [c_1 \, c_2 \, c_3]^T = 0\), where \(K_{(m, n)}\) and \(L_{(m, n)}\) are defined as in Lemma 3.1. Regrouping these equations gives the equivalent equation system
where
There are two types of possible solutions to (10): Those with \(c_1 = 0\) and those with \(c_1 \ne 0\). Note that \([0 \, c_2 \, c_3]^T\) satisfies (10) if and only if \([0 \, c_2 \, 0]^T\) and \([0 \, 0 \, c_3]^T\) do. Thus for the case \(c_1 = 0\), it is enough to consider elements of the forms \(SB^{n - 1}A^{m - 1}\) and \(TB^{n - 1}A^{m - 1}\) separately, rather that a general linear combination \(c_2SB^{n - 1}A^{m - 1} + c_3TB^{n - 1}A^{m - 1}\).
Now, \(SB^{n - 1}A^{m - 1} \in \fancyscript{B}(A) \cap \fancyscript{B}(B)\) if and only if \(M_S [0 \, 1]^T = 0\), that is, iff
This implies (by raising both sides of the equations to the power of \(d\)) that \(q_2^d = q_3^d = 1\), so \(q_2\) and \(q_3\) are \(d\):th roots of unity and thus \(q_2 = q_0^{r_2}\) and \(q_3 = q_0^{r_3}\) for some \(r_2, r_3 \in \{ 0,\,\ldots ,\,d-1 \}\) (since \(q_0\) generates the group of \(d\):th roots of unity). Then (11) holds if and only if \(q_0^{n - 1 + r_3} = q_0^{m - 1 - r_2} = 1\), that is, \(d\) divides both \(n - 1 + r_3\) and \(m - 1 - r_2\).
Similarly, \(TB^{n - 1}A^{m - 1} \in \fancyscript{B}(A) \cap \fancyscript{B}(B)\) if and only if \(M_T [0 \, 1]^T = 0\), that is, iff
This implies that \(q_1^d = q_4^d = 1\) and thus that \(q_1 = q_0^{r_1}\) and \(q_4 = q_0^{r_4}\) for some \(r_1, r_4 \in \{ 0,\,\ldots ,\,d - 1 \}\). Then (12) holds if and only if \(q_0^{n - 1 + r_1} = q_0^{m - 1 - r_4} = 1\), that is, \(d\) divides both \(n - 1 + r_1\) and \(m - 1 - r_4\).
If there is a solution of (10) with \(c_1 \ne 0\) then \(q_0^m = q_0^n = 1\) so \(d | m\) and \(d | n\). In addition, \(\det (M_S) = \det (M_T) = 0\), which is equivalent (using \(q_0^m = q_0^n = 1\) and \(\left\{ k \right\} _{q}(1 - q) = 1 - q^k\)) to \(q_2^nq_3^m = q_1^mq_4^n = 1\). When \(M_S\) is singular, either of the equations of the system \(M_S [c_1 \, c_2]^T = 0\) can be used to solve for \(c_2\). One gets
(the case \(1 - q_0q_2 = 1 - q_3 / q_0 = 0\) is excluded since \(q_2q_3 \ne 1\) when \(\mathbf {q}\) is generic). Similarly, when \(M_T\) is singular, one can use either of the equations of the system \(M_T [c_1 \, c_3]^T = 0\) to solve for \(c_3\). One gets
(the case \(1 - q_0q_4 = 1 - q_1 / q_0 = 0\) is excluded since \(q_1q_4 \ne 1\) when \(\mathbf {q}\) is generic).
When \((m, n) = (1, 2)\) or \((m, n) = (2, 1)\) then (10) is still a necessary condition for \(c_1B^nA^m + c_2SB^{n - 1}A^{m - 1} + c_3TB^{n - 1}A^{m - 1}\) to lie in \(\fancyscript{C}(A, B)\), but \(c_2, c_3\) must also satisfy
If \(c_1 = 0\) in any of these cases then either \(c_2 = 0\) or \(c_3 = 0\), since if \(c_2, c_3 \ne 0\) then (10) would imply \(q_1 = q_3 \, (= 1 / q_0^{n - 1})\) and \(q_2 = q_4 \, (= q_0^{m - 1})\). But if one of \(c_2, c_3\) is \( = 0\), then so is the other by (15). Thus, there are no non-trivial solutions with \(c_0 = 0\) when \((m, n) = (1, 2)\) or \((m, n) = (2, 1)\). The element \(B^nA^m + c_2SB^{n - 1}A^{m - 1} + c_3TB^{n - 1}A^{m - 1}\) lies in \(\fancyscript{C}(A, B)\) if and only if \([1 \, c_2 \, c_3]^T\) satisfies both (10) and (15). Using the expressions (13) and (14) for \(c_2\) and \(c_3\) together with \(q_0 = q_1^mq_4^n = q_2^nq_3^m = 1\) (that is, using the conditions that have just been shown to be equivalent to (10); note that when \(m = 1\) or \(n = 1\), \(d | m\) and \(d | n\) iff \(q_0 = 1\). Also note that \(q_1^mq_4^n = q_2^nq_3^m = 1\) implies \(q_2, q_4 \ne 1\) when \((m, n) = (1, 2)\) and \(q_1, q_3 \ne 1\) when \((m, n) = (2, 1)\) since \(\mathbf {q}\) is generic), (15) can be simplified to
Thus, the elements listed in the theorem form a spanning set for \(\fancyscript{C}(A) \cap \fancyscript{C}(B)\). To see that they are linearly independent, note that for a fixed \((m, n)\) it is impossible that both \(B^nA^m\,+\, c_2SB^{n - 1}A^{m - 1}\, + \, c_3TB^{n - 1}A^{m - 1}\) and \(SB^{n - 1}A^{m - 1}\) lie in \(\fancyscript{C}(A) \cap \fancyscript{C}(B)\), for that would imply
Similarly, it is impossible that both \(B^nA^m + c_2SB^{n - 1}A^{m - 1} + c_3TB^{n - 1}A^{m - 1}\) and \(TB^{n - 1}A^{m - 1}\) lie in \(\fancyscript{C}(A) \cap \fancyscript{C}(B)\), for that would imply \(q_1q_4 = 1\). Thus, the listed elements are linearly independent, and so they form a basis for \(\fancyscript{C}(A) \cap \fancyscript{C}(B)\).
5 Commutativity of \(\fancyscript{C}(A)\) and \(\fancyscript{C}(B)\)
This section gives, for generic \(\mathbf {q}\), necessary and sufficient conditions on \(\mathbf {q}\) for \(\fancyscript{C}(A)\) and \(\fancyscript{C}(B)\) to be commutative. As before, it is enough to consider homogeneous elements of \(\fancyscript{C}(A)\) and \(\fancyscript{C}(B)\), and the \(TS\)-components of the homogeneous elements of degree \((2, 2)\) can be disregarded since \(TS \in \fancyscript{Z} \). Thus, \(\fancyscript{C}(A)\) is commutative if and only if the set
is, and \(\fancyscript{C}(B)\) is commutative if and only if the set
is. Define further the sets
Then \(\fancyscript{H}_A = \fancyscript{X}_A \cup \fancyscript{Y}_A\) and \(\fancyscript{H}_B = \fancyscript{X}_B \cup \fancyscript{Y}_B\), and \(\fancyscript{X}_A \cap \fancyscript{Y}_A = \fancyscript{X}_B \cap \fancyscript{Y}_B = \{ 0 \}\), since \(0\) is homogeneous of all degrees. (The reason for explicitly including \(0\) in \(\fancyscript{Y}_A\) and \(\fancyscript{Y}_B\) is to make sure that they always contain \(0\): If \(0\) were not explicitly included then the case \(q_0 = 1\) would be exceptional.) These sets do, of course, depend on \(\mathbf {q}\); when this dependence needs to be emphasised the notation will be \(\fancyscript{X}_A(\mathbf {q})\), \(\fancyscript{Y}_A(\mathbf {q})\) and so on.
Consider two general homogeneous elements
of degrees \((k, l)\) and \((m, n)\) respectively. A somewhat lengthy calculation using the reordering formula (7) and Eq. (6) shows that
This holds for all \(k, l, m, n \ge 1\) except for \(k = l = m = n = 1\) (if \((k, l) = (2, 2)\) or \((m, n) = (2, 2)\) then there is an additional \(TS\)-term in the expression for \(X_{k, l}\) or \(X_{m, n}\), but that makes no difference for the product because of (6)). The commutator of \(X_{k, l}\) and \(X_{m, n}\) then is
The switch \(A \leftrightarrow B\) will be used in the proofs below. Assume that \(q_0 \ne 0\) (as is the case when \(\mathbf {q}\) is generic) and let \(f_{AB}: \fancyscript{F} \rightarrow \fancyscript{F} \) be the isomorphism defined by
The image under \(f_{AB}\) of \(G(\mathbf {q}) \), defined in (2), is
Thus \(f_{AB}(G(\mathbf {q}) )\) generates the ideal \(\fancyscript{J}(\hat{\mathbf {q}})\) where \(\hat{\mathbf {q}} = (\frac{1}{q_0}, q_4, q_3, q_2, q_1, q_5)\), and consequently \(f_{AB}(\fancyscript{J}(\mathbf {q}) ) = \fancyscript{J}(\hat{\mathbf {q}}) \). This makes it possible to define an isomorphism \(h_{AB}: \fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \rightarrow \fancyscript{F}/ \fancyscript{J}(\hat{\mathbf {q}}) \) by
It is easily checked that \(\hat{\mathbf {q}}\) is generic whenever \(\mathbf {q}\) is.
Also the switch \(S \leftrightarrow T\) will be used below. Let \(f_{ST}: \fancyscript{F} \rightarrow \fancyscript{F} \) be the isomorphism defined by
The image under \(f_{ST}\) of \(G(\mathbf {q}) \) is (assuming that \(q_5 \ne 0\))
Thus \(f_{ST}(G(\mathbf {q}) )\) generates the ideal \(\fancyscript{J}(\tilde{\mathbf {q}})\), where \(\tilde{\mathbf {q}} = (q_0, q_3, q_4, q_1, q_2, \frac{1}{q_5})\), so \(f_{ST}(\fancyscript{J}(\mathbf {q}) ) = \fancyscript{J}(\tilde{\mathbf {q}}) \) and an isomorphism \(h_{ST}: \fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \rightarrow \fancyscript{F}/ \fancyscript{J}(\tilde{\mathbf {q}}) \) can be defined by
Again, it is easily checked that \(\tilde{\mathbf {q}}\) is generic whenever \(\mathbf {q}\) is.
Lemma 5.1
Let \(\mathbf {q} = (q_0,\,\ldots ,\,q_5) \in \mathbb {C} ^6\) be generic. Then the sets \(\fancyscript{X}_A\) and \(\fancyscript{X}_B\) are commutative.
Proof
Pick any \(X_1, X_2 \in \fancyscript{X}_A\). Then \(X_1, X_2 \in \fancyscript{C}(A)\) and they are homogeneous, say of degrees \((k, l)\) and \((m, n)\) respectively with \(q_0^l = q_0^n = 1\). If \(k = 0\) then \(X_1 \equiv b_1B^l\) and Lemma 3.1 implies that \(X_1 \equiv 0\) or \(q_2^l = q_4^l = 1\). In either case, \(X_1 \in \fancyscript{Z} \), so in particular \(X_1\) commutes with \(X_2\). Similarly, if \(m = 0\) then \(X_2 \in \fancyscript{Z} \) and thus commutes with \(X_1\). If \(l = 0\) then \(X_1 = b_1A^k\) and if \(n = 0\) then \(X_2 = c_1A^m\); in both cases \(X_1\) and \(X_2\) commute. Thus it may be assumed that \(k, l, m, n \ge 1\), so that \(X_1\) and \(X_2\) can be written as
with coefficients that satisfy
where \(K_{(k, l)}\), \(K_{(m, n)}\) are defined as in Lemma 3.1. If \(k = l = m = n = 1\) then \(X_1\) and \(X_2\) are parallel, because \(K_{(1, 1)}\) has rank at least two (using that \(q_1 \ne q_3\) since \(\mathbf {q}\) is generic). Hence it may be assumed that at least one of \(k, l, m, n\) is \(\ge 2\), so that the commutator \([X_1, X_2]\) is given by (16). Since \(q_0^l = q_0^n = 1\), the coefficient of \(B^{l + n}A^{k + m}\) in (16) is \(0\)—it has to be shown that the coefficients of \(SB^{l + n - 1}A^{k + m - 1}\) and \(TB^{l + n - 1}A^{k + m - 1}\) are \(0\) as well.
If \(q_3 \ne q_0\) then (19) implies that
and the \(SB^{l + n - 1}A^{k + m - 1}\)-coefficient in (16) can be simplified to
The last equality holds by the identity \(\left\{ a \right\} _{q} + q^a \left\{ b \right\} _{q} = \left\{ a + b \right\} _{q}\) for \(q\)-natural numbers, since \(q_2^l = (q_0q_2)^l\), \(q_2^n = (q_0q_2)^n\). Similarly if \(q_1 \ne q_0\) then
and the \(TB^{l + n - 1}A^{k + m - 1}\)-coefficient in (16) can be simplified to
Now there are three cases to consider (\(q_1 = q_3 = q_0\) is impossible since \(\mathbf {q}\) is generic).
1. If \(q_1, q_3 \ne q_0\) then the coefficients of \(SB^{l + n - 1}A^{k + m - 1}\) and \(TB^{l + n - 1}A^{k + m - 1}\) in (16) are \(0\) by (20) and (21).
2. If \(q_1 = q_0\), \(q_3 \ne q_0\), then the computation (20) is still valid, that is, the coefficient of \(SB^{l + n - 1}A^{k + m - 1}\) in (16) is \(0\). Further, (19) implies that
and thus also
Then the \(TB^{l + n - 1}A^{k + m - 1}\)-coefficient in (16) can be simplified to
3. If \(q_1 \ne q_0\), \(q_3 = q_0\) then the computation (21) is still valid, that is, the coefficient of \(TB^{l + n - 1}A^{k + m - 1}\) in (16) is \(0\). The condition (19) implies that
and the \(SB^{l + n - 1}A^{k + m - 1}\)-coefficient becomes
Thus it has been shown that \(\fancyscript{X}_A\) is commutative.
In order to see that \(\fancyscript{X}_B = \fancyscript{X}_B(\mathbf {q})\) is commutative, let \(h_{AB}: \fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \rightarrow \fancyscript{F}/ \fancyscript{J}(\hat{\mathbf {q}}) \) be the isomorphism defined as in (17). Then \(\fancyscript{X}_A (\hat{\mathbf {q}})\) is commutative by the above proof, so \(\fancyscript{X}_B(\mathbf {q}) = h_{AB}^{-1} (\fancyscript{X}_A (\hat{\mathbf {q}}))\) is commutative as well.
Lemma 5.2
Let \(\mathbf {q} = (q_0,\,\ldots ,\,q_5) \in \mathbb {C} ^6\) be generic. Then the sets \(\fancyscript{Y}_A\) and \(\fancyscript{Y}_B\) are commutative.
Proof
Pick any \(Y_1, Y_2 \in \fancyscript{Y}_A\). Then \(Y_1, Y_2 \in \fancyscript{C}(A)\) and they are homogeneous, say of degrees \((k, l)\) and \((m, n)\) respectively with \(q_0^l, q_0^n \ne 1\). It is then impossible that \(l = 0\) or \(n = 0\), and by Lemma 3.1 it cannot be that \(Y_1 = b_1B^l\) or \(Y_2 = c_1B^n\) with \(b_1, c_1 \ne 0\). Thus it may be assumed that \(k, l, m, n \ge 1\), and \(Y_1, Y_2\) can be written as
with coefficients that satisfy
where \(K_{(k, l)}\), \(K_{(m, n)}\) are defined as in Lemma 3.1. If \(k = l = m = n = 1\) then \(Y_1\) and \(Y_2\) are parallel, because \(K_{(1, 1)}\) has rank at least two (using that \(q_1 \ne q_3\) since \(\mathbf {q}\) is generic). Hence it may be assumed that at least one of \(k, l, m, n\) is \(\ge 2\). Since \(q_0^l, q_0^n \ne 1\), (22) implies that \(b_1 = c_1 = 0\). But then \(Y_1Y_2 \equiv Y_2Y_1 \equiv 0\) by (6), so \(Y_1, Y_2\) commute.
To see that \(\fancyscript{Y}_B = \fancyscript{Y}_B(\mathbf {q})\) is commutative, let \(h_{AB}: \fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \rightarrow \fancyscript{F}/ \fancyscript{J}(\hat{\mathbf {q}}) \) be the isomorphism defined as in (17). Then \(\fancyscript{Y}_A (\hat{\mathbf {q}})\) is commutative by the above proof, so \(\fancyscript{Y}_B(\mathbf {q}) = h_{AB}^{-1} (\fancyscript{Y}_A (\hat{\mathbf {q}}))\) is commutative as well.
Because of Lemma 5.1 and Lemma 5.2, it is enough to check whether the elements of \(\fancyscript{X}_A\) commute with the elements of \(\fancyscript{Y}_A\) to see if \(\fancyscript{C}(A)\) is commutative, and to check whether the elements of \(\fancyscript{X}_B\) commute with the elements of \(\fancyscript{Y}_B\) to see if \(\fancyscript{C}(B)\) is commutative.
Theorem 5.1
Let \(\mathbf {q} = (q_0,\,\ldots ,\,q_5) \in \mathbb {C} ^6\) be generic and suppose that \(q_0\) is not a root of unity. Then \(\fancyscript{C}(A)\) and \(\fancyscript{C}(B)\) are commutative.
Proof
Since \(q_0\) is not a root of unity,
Thus, every element of \(\fancyscript{X}_A\) commutes with every element of \(\fancyscript{Y}_A\), and it follows from Lemma 5.1 and Lemma 5.2 that \(\fancyscript{C}(A)\) is commutative. Similarly,
thus every element of \(\fancyscript{X}_B\) commutes with every element of \(\fancyscript{Y}_B\) and thus \(\fancyscript{C}(B)\) is commutative.
Theorem 5.2
Let \(\mathbf {q} = (q_0,\,\ldots ,\,q_5) \in \mathbb {C} ^6\) be generic, and suppose that \(q_0\) is a root of unity with \(d\) being the smallest positive integer such that \(q_0^d = 1\). Then \(\fancyscript{C}(A)\) is commutative if and only if
and
and \(\fancyscript{C}(B)\) is commutative if and only if
and
Proof
It follows from Lemma 5.1 and Lemma 5.2 that \(\fancyscript{C}(A)\) is commutative if and only if every element of \(\fancyscript{X}_A\) commutes with every element of \(\fancyscript{Y}_A\). A non-zero element of \(\fancyscript{Y}_A\) cannot have degree \((m, 0)\) since \(q_0^0 = 1\), and it cannot have degree \((0, n)\) by Lemma 3.1. Thus any non-zero \(Y \in \fancyscript{Y}_A\) is of the form
for some \(n\) with \(q_0^n \ne 1\) and with coefficients that satisfy
Since \(q_1 \ne q_3\) (because \(\mathbf {q}\) is generic), the matrix in (27) has one of the forms
where \(*\) indicates a non-zero element and \(?\) indicates an element that may or may not be zero. Thus the solutions to (27) are
Since it is impossible that both \(c_2\) and \(c_3\) are non-zero, \(Y\) must actually have the form \(c_2 SB^{n - 1}A^{m - 1}\) or \(c_3 TB^{n - 1}A^{m - 1}\). Thus \(\fancyscript{Y}_A\) can be decomposed as \(\fancyscript{Y}_A^S \cup \fancyscript{Y}_A^T \cup \{ 0 \}\), where
(here, \(c\) ranges over \(\mathbb {C}\) and \(m, n\) range over \(\mathbf {N}^+\)), and \(\fancyscript{C}(A)\) is commutative if and only if every element of \(\fancyscript{X}_A\) commutes with every element of \(\fancyscript{Y}_A^S\) and \(\fancyscript{Y}_A^T\).
Consider first \(\fancyscript{Y}_A^S\) and the conditions (23). If \(\left\{ d \right\} _{q_3 / q_0} \ne 0\) then \(q_3^d \ne 1\) or \(q_3 = q_0\) and it cannot be that \(q_0^n \ne 1\) and \(q_0^{n - 1}q_3 = 1\); thus \(\fancyscript{Y}_A^S = \emptyset \). Otherwise, there is an \(r_3 \in \{ 2,\,\ldots ,\,d \}\) such that \(q_3 = q_0^{r_3}\), and
is non-empty. Now pick any \(X \in \fancyscript{X}_A\). If \(X = b_1A^k\) then \(X\) obviously commutes with every element in \(\fancyscript{Y}_A^S\). Otherwise, \(X\) has one of the forms
with \(d | l\). Then the commutator of \(X\) with an element of \(\fancyscript{Y}_A^S\) is (note that \(l = n = 1\) is impossible and use (6))
Thus if \(\left\{ d \right\} _{q_3 / q_0} \ne 0, q_2^d = 1\) then \(X\) commutes with everything in \(\fancyscript{Y}_A^S\). Finally, if \(q_1 = q_0\) and \(q_4^d \ne 1\) then Lemma 3.1 implies that \(b_1 = 0\), so that the commutator (28) is \(0\), and again \(X\) commutes with everything in \(\fancyscript{Y}_A^S\).
On the other hand, if none of the conditions
is satisfied, then
where \(r_3 \in \{ 2,\,\ldots ,\,d \}\) is such that \(q_3 = q_0^{r_3}\), and
(\(b_T\) arbitrary if \(q_1 = q_0\) works because then \(q_4^d = 1\) and thus \(\left\{ d \right\} _{q_0q_4} = 0\) since \(\mathbf {q}\) generic implies \(q_4 \ne q_0^{-1}\)). This element of \(\fancyscript{X}_A\) does not commute with \(SB^{2d - r_3}\) in \(\fancyscript{Y}_A^S\); their commutator is \((q_2^d - 1) SB^{3d - r_3}A^{2}\). Thus it has been shown that every element of \(\fancyscript{X}_A\) commutes with every element of \(\fancyscript{Y}_A^S\) if and only if (23) is satisfied.
To see that every element of \(\fancyscript{X}_A\) commutes with every element of \(\fancyscript{Y}_A^T\) consider the isomorphism \(h_{ST}: \fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \rightarrow \fancyscript{F}/ \fancyscript{J}(\tilde{\mathbf {q}}) \), where \(\tilde{\mathbf {q}} = (q_0, q_3, q_4, q_1, q_2, \frac{1}{q_5})\), as defined in (18). Note that \(\tilde{\mathbf {q}}\) is generic, \(\tilde{q}_0\) is a root of unity with \(d\) being the smallest positive integer such that \((\tilde{q}_0)^d = 1\) and \(\tilde{\mathbf {q}}\) satisfies (23) if and only if \(\mathbf {q}\) satisfies (24). Furthermore, \(h_{ST}(\fancyscript{X}_A(\mathbf {q})) = \fancyscript{X}_A(\tilde{\mathbf {q}})\) and \(h_{ST}(\fancyscript{Y}_A^T(\mathbf {q})) = \fancyscript{Y}_A^S(\tilde{\mathbf {q}})\). Thus, using what has already been proved,
This concludes the proof of the first part of the theorem, namely that \(\fancyscript{C}(A)\) is commutative if and only if (23) and (24) are satisfied.
For the second part of the theorem, consider the isomorphism \(h_{AB}: \fancyscript{F}/ \fancyscript{J}(\mathbf {q}) \rightarrow \fancyscript{F}/ \fancyscript{J}(\hat{\mathbf {q}}) \), where \(\hat{\mathbf {q}} = (\frac{1}{q_0}, q_4, q_3, q_2, q_1, q_5)\), as defined in (17). Note that \(\hat{\mathbf {q}}\) is generic, \(\hat{q}_0\) is a root of unity with \(d\) being the smallest positive integer such that \((\hat{q}_0)^d = 1\) and \(\hat{\mathbf {q}}\) satisfies (23) and (24) if and only if \(\mathbf {q}\) satisfies (25) and (26). Moreover, \(h_{AB}(\fancyscript{C}(B)(\mathbf {q})) = \fancyscript{C}(A)(\hat{\mathbf {q}})\) and thus using what has already been proved,
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This research was supported in part by the Swedish Research Council (621-2007-6338), Swedish Foundation for International Cooperation in Research and Higher Education (STINT), Swedish Royal Academy of Sciences, Crafoord Foundation and the Nordforsk network “Operator algebra and dynamics” (grant # 11580).
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Ekström, F., Silvestrov, S.D. (2014). Commutants and Centers in a 6-Parameter Family of Quadratically Linked Quantum Plane Algebras. In: Makhlouf, A., Paal, E., Silvestrov, S., Stolin, A. (eds) Algebra, Geometry and Mathematical Physics. Springer Proceedings in Mathematics & Statistics, vol 85. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-55361-5_3
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