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Matrix representation of Toeplitz operators on Newton spaces
Journal of Inequalities and Applications volume 2024, Article number: 43 (2024)
Abstract
In this paper, we study several properties of an orthonormal basis \(\{N_{n}(z)\}\) for the Newton space \(N^{2}({\mathbb{P}})\). In particular, we investigate the product of \(N_{m}\) and \(N_{m}\) and the orthogonal projection P of \(\overline{N_{n}}N_{m}\) that maps from \(L^{2}(\mathbb{P})\) onto \(N^{2}(\mathbb{P})\). Moreover, we find the matrix representation of Toeplitz operators with respect to such an orthonormal basis on the Newton space \(N^{2}({\mathbb{P}})\).
1 Introduction
For any \(n\in \mathbb{N} \cup {0}\), let \(N_{n}(z)\) denote the nth Newton polynomial, which is determined by the coefficients in the expansion:
where \(|w|<1\) and z is any complex number in the complex plane \(\mathbb{C}\). Using the notations in [1, 12–14], \(N_{n}(z)\) has the following expression
where \(\binom{z}{n}= \frac{z(z-1)(z-2)\cdots (z-(n-1))}{n!}\text{ for }n \geq 1\) and \(\binom{z}{0}=1\).
Consider a probability measure μ defined on \(\mathbb{C}\) such that
Let \(\gamma (x)\) denote the discrete measure on \(\mathbb{R}\) with unit masses at \(\{-\frac{1}{2}+\frac{n}{2}:n\in{\mathbb{N}}\}\) and \({\mathbb{P}}:=\{ z\in{\mathbb{C}}:Re(z)>-\frac{1}{2}\}\). Set
where Γ denotes the usual gamma function.
Let \(N^{2}({\mathbb{P}})\) be a Newton space as the closure of the set of polynomials in \(L^{2}({\mathbb{C}},\mu )\) (see [3]). In [11], Markett, Rosenblum, and Rovnyak verified that \(N^{2}({\mathbb{P}})\) is a Hilbert space and the Newton polynomials \(\{N_{n}(z)\}_{n=0}^{\infty}\) form an orthonormal basis for \(N^{2}({\mathbb{P}})\). Note that
On the positive real line define a measure μ by \(d\mu (t)=e^{-t}\,dt\). The measure μ is finite and has total mass \(\Gamma (1)=1\). Consider the weighted Lebesgue space denoted by \(L^{2}(\mu )\), which comprises measurable complex-valued functions f defined with
and let \({L^{\infty}({\mu})}\) be the set of all essentially bounded measurable functions in \(\mathbb{P}\). For \(f \in {L^{2}({\mu})}\), the weighted Mellin transform F on \(N^{2}({\mathbb{P}})\) of f is defined by
For \(f, g\in {L^{\infty}({\mu})}\), an inner product on \(N^{2}(\mathbb{P})\) is defined by
where F and G are weighted Mellin transforms of f and g, respectively, (see [11]).
Let P denote the orthogonal projection that maps \(L^{2}({\mu})\) onto \(N^{2}({\mathbb{P}})\) defined by
where dA is an area measure on \({\mathbb{P}}\). The reproducing kernel of \(N^{2}({\mathbb{P}})\) has the following form:
For \(\varphi \in {L^{\infty}({\mu})}\), the Toeplitz operator \(T_{\varphi}\) on \(N^{2}(\mathbb{P})\) is defined by
From [9], it is known that the following properties of the Toeplitz operators \(T_{\varphi}\) on \(N^{2}(\mathbb{P})\) hold:
(i) \(T_{\alpha \varphi +\beta \psi}=\alpha T_{\varphi}+\beta T_{\psi}\) for \(\varphi ,\psi \in L^{\infty}({\mu})\).
(ii) \(T_{\varphi}^{\ast}=T_{\overline{\varphi}}\) for \(\varphi \in L^{\infty}({\mu})\).
(iii) \(T_{\varphi}=0\) if and only if \(\varphi =0\) a.e.
(iv) \(T_{\varphi}T_{\psi}=T_{\varphi \psi}\) and \(T_{\overline{\psi}}T_{\varphi}=T_{\overline{\psi}{\varphi}}\) for \(\varphi \in L^{\infty}({\mu})\) and \(\psi \in H^{\infty}({\mu})\).
In [6, 10], the authors studied the properties of composition operators on Newton space \(N^{2}({\mathbb{P}})\). Recently, Han [3] focused on the complex symmetric composition operators on Newton space \(N^{2}({\mathbb{P}})\) with respect to the specific conjugation. Furthermore, in [7, 8], we considered the properties of Toeplitz operators on Newton space. From the above research point of view, we further investigate the properties of Newton space and Newton basis and study the matrix of Toeplitz operators on Newton space in this paper.
This paper is organized as follows. First, we study several properties of an orthonormal basis \(\{N_{n}(z)\}\) for Newton space \(N^{2}({\mathbb{P}})\). In particular, we investigate the product of \(N_{m}\) and \(N_{m}\) and the orthogonal projection P of \(\overline{N_{n}}N_{m}\) that maps from \(L^{2}(\mathbb{P})\) onto \(N^{2}(\mathbb{P})\). Next, we consider the matrix representation of Toeplitz operators with respect to such an orthonormal basis on Newton space \(N^{2}({\mathbb{P}})\).
2 Main results
In this section, we first study an orthonormal basis for the Newton space \(N^{2}({\mathbb{P}})\). We begin with the following lemma.
Lemma 2.1
([10]) Let the map \(\Delta : N^{2}({\mathbb{P}})\rightarrow N^{2}({\mathbb{P}})\) defined by
be the backwards unilateral shift on the orthonormal basis \(\{N_{n}(z)\}_{n=0}^{\infty}\). Then, \(\Delta ^{\ast}\) is the unilateral shift on the orthonormal basis \(\{N_{n}(z)\}_{n=0}^{\infty}\), i.e., \(\Delta ^{\ast}N_{n}(z)=N_{n+1}(z)\) holds.
Lemma 2.2
For any \(m,n\geq 0\), the following equation holds
Proof
Since \(N_{n}(z)=(-1)^{n}\frac{z(z-1)\cdots (z-(n-1))}{n!}\) for \(n\geq 1\), it follows that
Hence, we complete the proof. □
Lemma 2.3
Let \({\mathcal {N}}\) be an \((n+1)\times (n+1)\) matrix given by
Then, \({\mathcal {N}}^{-1}={\mathcal {N}}\).
Proof
Put
and
where \(A^{T}\) is the transpose of the matrix A. If \(j< k\), then \(x_{j}\cdot (y_{k})^{T}=0\). If \(j=k\), then
Let \(j> k\). Note that \(\sum_{i=0}^{j-k}(-1)^{i} \binom{j-k}{i} =0\). Since
we have
Hence, it means that \({\mathcal {N}}^{2}=I\) and so \({\mathcal {N}}^{-1}={\mathcal {N}}\). □
Let \(m,n\geq 0\) be nonnegative integers. Then, \(z^{m}z^{n}=z^{m+n}\) holds on the Hardy space \(H^{2}\). However, \(N_{m}N_{n}\) is not \(N_{m+n}\) on Newton space \(N^{2}(\mathbb{P})\), in general. We next show that the product of \(N_{m}\) and \(N_{n}\) is the linear combination of \(\{N_{j}\}_{j=\max\{m,n\}}^{(m+n)}\).
Theorem 2.4
For any \(m\geq n\geq 0\), it holds that
where
for \(b_{j}(m,n)\in{\mathbb{R}}\) and \({\mathcal {N}}\) is denoted as in Lemma 2.3.
Proof
By the definition of \(N_{n}(z)\), we have
Thus, we can write \(N_{m}(z)N_{n}(z)\) as follows:
for some \(b_{j}(m,n)\). Substituting 0 to \(m-1\) into (2.3), we obtain that \(b_{0}(m,n)=b_{1}(m,n)=\cdots =b_{m-1}(m,n)=0\). If we put m into (2.3), then we have
and so \(N_{n}(m)=b_{m}(m,n)\). Next, we put \(m+1\) into (2.3) and we have
Set
as in Lemma 2.3. By repeating this method, we deduce that
Therefore, we conclude that \(N_{m}(z)N_{n}(z)=\sum_{j=m}^{(m+n)}b_{j}(m,n) N_{j}(z)\), where
By Lemma 2.3, we have the results. □
From (2.2), we obtain the exact value of \(b_{j}(m,n)\) as follows for the given m, n. We obtain the specific value of \(b(m,n)\) through a simple calculation.
Remark 2.5
(a) If \(m=n=2\), then we have \(N_{2}(z)N_{2}(z)=\sum_{j=1}^{4}b_{j}(2,2) N_{j}(z)\) gives that
Take \(z=1\), then \(b_{1}(2,2)=0\) and so \(N_{2}(z)N_{2}(z)=\sum_{j=2}^{4}b_{j}(2,2) N_{j}(z)\). Thus,
Take \(z=2\), then \(b_{2}(2,2)=N_{2}(2)=1\) and hence
Therefore,
If \(z=3\) in (2.4), then \({b_{3}}(2,2)=-6\). If \(z=4\) in (2.4), then \(6=3+\frac{b_{4}(2,2)}{2}\) and so \(b_{4}(2,2)=6\). Hence, \(b_{1}(2,2)=0\), \(b_{2}(2,2)=1\), \(b_{4}(2,2)=-b_{3}(2,2)=6\). Hence,
From (2.2), for \(m=2\) and \(n=2\), we have
(b) From (2.2), for \(m=3\) and \(n=2\), we have
(c) From (2.2), for \(m=4\) and \(n=2\), we have
In the Hardy space \(H^{2}(\mathbb{T})\), \(\overline{z}^{n}z^{m}\) is equal to \(z^{m-n}\), but in the weighted Bergmann space \(A^{2}_{\alpha}(\mathbb{D})\), \(\overline{z}^{n}z^{m}\neq z^{m-n}\) since \(z\in \mathbb{D}\). In addition, \(\overline{N_{n}(z)}N_{m}(z)\) is not \(N_{m-n}(z)\) in the Newton space \(N^{2}(\mathbb{P})\).
Lemma 2.6
[10, Theorem 1.2] The \(N^{2}({\mathbb{P}})\) is a Hilbert space that includes the Newton polynomials as a complete orthogonal set.
Lemma 2.7
The set of functions \(\{ N_{n}(z)\}\cup \{\overline{N_{m}(z)}\}\) forms an orthonormal basis for \(L^{2}(\mathbb{P})\) for \({n\in{\mathbb{N}\cup \{0\}}}\) and \({m\in{\mathbb{N}}}\).
Proof
For positive integers m, n with \(m\neq n\),
and \(\langle \overline{N_{m}}, \overline{N_{m}}\rangle =\langle {N_{m}}, {N_{m}} \rangle =1\). Now, we want to show that Parseval’s identity
holds for every \(f\in L^{2}({\mathbb{P}})\). Let \(f(z)=\sum_{k=0}^{\infty}{a_{k}}N_{k}(z)+\sum_{k=1}^{\infty}{a_{-k}} \overline{N_{k}(z)}\). Then, \(\|f\|_{2}^{2}= \sum_{k=-\infty}^{\infty}|{a_{k}}|^{2}\) and for any \(n\ge 0\),
and for any \(n>0\),
Therefore,
Since Parseval’s identity holds, we obtain that \(\{ N_{n}(z)\}\cup \{\overline{N_{m}(z)}\}\) is complete (see [2]). Hence, for \({n\in{\mathbb{N}\cup \{0\}}}\) and \({m\in{\mathbb{N}}}\), \(\{N_{n}(z)\}\cup \{\overline{N_{m}(z)}\}\) forms an orthonormal basis for \(L^{2}(\mathbb{P})\). □
In [4], let P be an orthogonal projection of \(L^{2}(\mathbb{D})\) onto the Bergamm space \(A^{2}(\mathbb{D})\). Then, for nonnegative integers n, m,
Next, we investigate the orthogonal projection P of \(\overline{N_{n}}N_{m}\).
Theorem 2.8
For any nonnegative integers m, n,
where \(b_{m}(n,m-n+j)\) is the solution of the matrix equation as in Theorem 2.4for \(0\leq j\leq n\).
Proof
For any nonnegative integer k, we obtain from Theorem 2.4 that
(a) If \(m< n\), then (2.6) implies
for \(n\geq k\) and
for \(n < k\) since the Newton polynomials \(\{N_{n}(z)\}_{n=0}^{\infty}\) are orthonormal.
(b) If \(m\ge n\), then
Hence, if \(m\ge n\), then (2.6) becomes
and if \(m< n\), then \(P(\overline{N_{n}} N_{m})=0\). □
Remark 2.9
Note that \(b_{m}(m,n)=b_{m}(n,m)\) and \(b_{j}(m,0)=1\) for any nonnegative integer m, n, j.
(i) Since
and
by Theorem 2.4, we have \(b_{1}(1,1)=-1\), \(b_{2}(1,1)=2\), \(b_{2}(2,1)=-2\), and \(b_{3}(2,1)=3\). Then,
by Theorem 2.8.
(ii) By Theorem 2.8 and Remark 2.4, we also obtain that
and
As an application of Theorem 2.8, we obtain the following corollary.
Corollary 2.10
For any nonnegative integers m, k with \(m\geq k\),
holds, where P denotes an orthogonal projection of \(L^{2}(\mathbb{P})\) onto \(N^{2}({\mathbb{P}})\).
Proof
By Theorem 2.8, we obtain that
where \(b_{m}(n,m-k+j)\) denotes the solutions of the matrix equation as in Theorem 2.4 for \(0\leq j\leq n\). □
We finally find the matrices of Toeplitz operators \(T_{\varphi}\) with harmonic symbols φ on the Newton spaces by using Theorems 2.4 and 2.8. In Theorem 2.11, we explain the characteristics of the entries of the Toeplitz matrix in Newton space. Applying this, by specifically using the coefficient of \(b_{j}(m,n)\) in Corollary 2.14, it was found that the entries of the Toeplitz matrix in Newton space are expressed as a linear combination of the binomial coefficients of the given entries.
Theorem 2.11
For the harmonic symbol \(\varphi (z)=\sum_{i=0}^{\infty}a_{i}N_{i}+\sum_{i=1}^{\infty}a_{-i} \overline{N}_{i}\), the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}=\{N_{n}\}_{n\geq 0}\) is given by
and the adjoint of the matrix of \(T_{\varphi}\) is given by
where \(b_{m}(m,n)\in{\mathbb{R}}\) is denoted as in Theorem 2.4.
Proof
For the harmonic symbol \(\varphi (z)=\sum_{i=0}^{\infty}a_{i}N_{i}+\sum_{i=1}^{\infty}a_{-i} \overline{N}_{i}\), the \((m, n)\)th entry of the matrix of \(T_{\varphi}\) with respect to orthonormal basis \(\{N_{n}\}_{n\ge 0}\) of \(N^{2}(\mathbb{P})\) is given by
Then, there are two cases to consider. If \(m\ge n\), then
Thus, the first and third term of the right equation in (2.8) have no term of the form \(a_{i}b_{m}(i,n)N_{m}\). Hence, (2.7) becomes
If \(m< n\), then by a similar method, (2.7) gives
Thus, we have
where m and n are nonnegative integers. Hence, the matrix of \(T_{\varphi}\) with respect to \({\mathcal{B}}=\{N_{n}\}_{n\geq 0}\) is given by
and the adjoint of the matrix of \(T_{\varphi}\) is given by
and, hence, we know that \([T_{\varphi}]_{\mathcal{B}}^{*}=[T_{\overline{\varphi}}]_{\mathcal{B}} \). □
Corollary 2.12
If \([T_{\varphi}]_{\mathcal{B}}\) is self-adjoint, then \(\varphi (z)=\sum_{i=0}^{\infty}a_{i}N_{i}+\sum_{i=1}^{\infty} \overline{a}_{i}\overline{N}_{i}\).
Proof
The proof follows from Theorem 2.11. □
Corollary 2.13
(i) For the harmonic symbol \(\varphi (z)=a_{1}N_{1}+a_{0}+a_{-1}\overline{N_{1}}\), the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}=\{N_{0}, N_{1}\}\) is given by
(ii) For the harmonic symbol \(\varphi (z)=a_{2}N_{2}+a_{1}N_{1}+a_{0}+a_{-1}\overline{N_{1}}+a_{-2} \overline{N_{2}}\), the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}=\{N_{0}, N_{1}, N_{2}\}\) is given by
(iii) Let \(\varphi (z)=a_{3}N_{3}+a_{2}N_{2}+a_{1}N_{1}+a_{0}+a_{-1} \overline{N_{1}}+a_{-2}\overline{N_{2}}+a_{-3}\overline{N_{3}}\) be the harmonic symbol. Then, the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}=\{N_{0}, N_{1},N_{2},N_{3}\}\) is given by
Proof
Since \(N_{0}(z)N_{0}(z)=b_{0}(0,0) N_{0}(z)\) and \(N_{1}(z)N_{0}(z)=b_{1}(1,0) N_{1}(z)\) by Theorem 2.4, we have \(b_{0}(0,0)=1\) and \(b_{1}(1,0)=1\). Moreover, since
by Theorem 2.4, it follows that \(b_{1}(1,1)=-1\). Since \(N_{2}(z)N_{0}(z)=b_{2}(2,0) N_{2}(z)\), we have \(b_{2}(2,0)=1\) and \(b_{2}(2,2)=1\) by Remark 2.5. Since \(b_{m}(m,n)=N_{n}(m)\), we obtain \(b_{2}(2,1)=N_{1}(2)=-2\) and \(b_{2}(1,1)=2\) by Remark 2.9. Hence, the proof follows from Theorem 2.11. □
Corollary 2.14
Let \(\varphi (z)=\sum_{i=0}^{n}a_{i}N_{i}+\sum_{i=1}^{n}a_{-i} \overline{N}_{i}\) be the harmonic symbol for even n. Then, the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}=\{N_{k}\}_{k=0,1,2,\ldots ,n}\) is given by
Proof
The proof follows from Theorem 2.11 and Corollary 2.13. □
Remark 2.15
Set
Then, for \(m\geq n\), \(c_{m,n}=\sum_{i=m-n}^{m}a_{i}b_{m}(i,n)\) and \(c_{n,m}=\sum_{i=m-n}^{m}a_{-i}b_{m}(i,n)\). Hence, \([T_{\varphi}]_{\mathcal{B}}\) is self-adjoint if and only if \(c_{m,n}=\overline{c_{n,m}}\) if and only if \(a_{-i}=\overline{a_{i}}\).
Example 2.16
(i) Let \(\varphi (z)=N_{1}+2+i\overline{N_{1}}\) be the harmonic symbol. Then, the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}=\{N_{0}, N_{1}\}\) is given by
(ii) Let \(\varphi (z)=iN_{2}-N_{1}+2+i\overline{N_{1}}+2\overline{N_{2}}\) be the harmonic symbol. Then, the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}=\{N_{0}, N_{1}, N_{2}\}\) is given by
A conjugation on \(\mathcal{H}\) is an antilinear operator \({C}: {\mathcal{H}}\rightarrow {\mathcal{H}}\) that satisfies \({C}^{2}=I\) and \(\langle {C}x, {C}y \rangle =\langle y, x\rangle \) for all \(x,y\in {\mathcal{H}}\). An operator \(T\in{\mathcal{L(H)}}\) is complex symmetric if there exists a conjugation C on \({\mathcal{H}}\) such that \(T= {C}T^{\ast}{C}\).
Corollary 2.17
Assume that C and \(C_{\mu ,\lambda}\) are conjugations on \(L^{2}\) given by \(Cf(z)=\overline{f(\overline{z})}\) and \(C_{\mu , \lambda}f(z)=\mu \overline{f(\lambda \overline{z})}\) for \(f\in N^{2}(\mathbb{P})\) with \(|\lambda |=|\mu |=1\), respectively. If for the harmonic symbol \(\varphi (z)=\sum_{i=0}^{\infty}a_{i}N_{i}+\sum_{i=1}^{\infty}a_{-i} \overline{N}_{i}\) and the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}=\{N_{n}\}_{n\geq 0}\), then the following statements are equivalent:
(i) \([T_{\varphi}]_{\mathcal{B}}\) is complex symmetric with the conjugation C;
(ii) \([T_{\varphi}]_{\mathcal{B}}\) is complex symmetric with the conjugation \(C_{\mu , \lambda}\);
(iii) \(a_{i}=a_{-i}\) for \(i=0,1,2,\ldots \) .
Proof
(i) ⇔ (iii) Let \(\varphi (z)=\sum_{i=0}^{\infty}a_{i}N_{i}+\sum_{i=1}^{\infty}a_{-i} \overline{N}_{i}\) be with respect to the basis \({\mathcal {B}}=\{N_{n}\}_{n=0}^{\infty}\). Since the matrix of \([T_{\varphi}]_{\mathcal{B}}\) is of the form as in Theorem 2.11, it follows that the matrix of \(C[T_{\varphi}]_{\mathcal{B}}C\) is the following:
Then, \([T_{\varphi}]_{\mathcal {B}}\) is complex symmetric with the conjugation C if and only if \(a_{i}=a_{-i}\) for \(i=0,1,2,\ldots \) .
(ii) ⇔ (iii) Let \(\varphi (z)=\sum_{i=0}^{\infty}a_{i}N_{i}+\sum_{i=1}^{\infty}a_{-i} \overline{N}_{i}\) be with respect to the basis \({\mathcal {B}}=\{N_{n}\}_{n=0}^{\infty}\). It is known from [5] that \(C_{\mu ,\lambda}\) is unitarily equivalent to \(C_{1,\lambda}\). Since the matrix of \(T_{\varphi}\) is of the form as in Theorem 2.11, it follows that the matrix of \(C_{1,\lambda}T_{\varphi}C_{1,\lambda}\) is the following:
Then, \([T_{\varphi}]_{\mathcal {B}}\) is complex symmetric with the conjugation \(C_{1,\lambda}\) if and only if \(a_{i}=a_{-i}\) for \(i=0,1,2,\ldots \) . □
Corollary 2.18
Let C be a conjugation on \(L^{2}\) given by \(Cf(z)=\overline{f(\overline{z})}\) for \(f\in N^{2}(\mathbb{P})\). If for the harmonic symbol \(\varphi (z)=\sum_{i=0}^{3}a_{i}(N_{i}+\overline{N_{i}})\), the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}=\{N_{0}, N_{1},N_{2},N_{3}\}\) is given by
then \([T_{\varphi}]_{\mathcal{B}}\) is complex symmetric with the conjugation C.
Example 2.19
Let C be a conjugation on \(L^{2}\) given by \(Cf(z)=\overline{f(\overline{z})}\) for \(f\in N^{2}(\mathbb{P})\) and let \({\mathcal{B}}=\{N_{0}, N_{1},N_{2},N_{3}\}\).
(i) Let
be the harmonic symbol. If the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}\) is given by
then \([T_{\varphi}]_{\mathcal{B}}\) is complex symmetric with the conjugation C.
(ii) If for the harmonic symbol \(\varphi (z)=\sum_{i=0}^{3}(N_{i}+\overline{N_{i}})\), the matrix of \(T_{\varphi}\) with respect to orthonormal basis \({\mathcal{B}}\) is given by
then \([T_{\varphi}]_{\mathcal{B}}\) is complex symmetric with the conjugation C.
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The first author was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) (No. 2019R1F1A1058633). The second author was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) (No. 2019R1A2C1002653). The second author was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) (No. 2022R1H1A2091052). The third author was supported by the Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (2021R1C1C1008713).
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Ko, E., Lee, J.E. & Lee, J. Matrix representation of Toeplitz operators on Newton spaces. J Inequal Appl 2024, 43 (2024). https://doi.org/10.1186/s13660-024-03126-0
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DOI: https://doi.org/10.1186/s13660-024-03126-0