This paper was converted on www.awesomepapers.org from LaTeX by an anonymous user.
Want to know more? Visit the Converter page.

Weighted Composition Operators on Discrete Weighted Banach Spaces

Robert F. Allen1 and Matthew A. Pons2 1Department of Mathematics & Statistics, University of Wisconsin-La Crosse 2Department of Mathematics & Actuarial Science, North Central College [email protected], [email protected]
Abstract.

We present the current results in the study of weighted composition operators on weighted Banach spaces of an unbounded, locally finite metric space. Specifically, we determine characterizations of bounded and compact weighted composition operators, including the operator and essential norms. In addition, we characterize the weighted composition operators that are injective, are bounded below, have closed range, and have bounded inverse. We characterize the isometries and surjective isometries among the weighted composition operators, as well as those that satisfy the Fredholm condition. Lastly, we provide numerous interesting examples of the richness of these operators acting on the discrete weighted Banach spaces.

Key words and phrases:
Weighted composition operators, Metric spaces, Weighted Banach spaces.
1991 Mathematics Subject Classification:
primary: 47B33; secondary: 05C05

1. Introduction

Let XX be a Banach space of functions on a domain Ω\Omega. For ψ\psi a function on Ω\Omega and φ\varphi a self-map of Ω\Omega, the linear operator defined on XX by

Wψ,φf=ψ(fφ)W_{\psi,\varphi}f=\psi(f\circ\varphi)

is called the weighted composition operator induced by ψ\psi and φ\varphi. Observe that when ψ1\psi\equiv 1, we have the composition operator Cφf=fφC_{\varphi}f=f\circ\varphi, and similarly when φ(z)=z\varphi(z)=z, we have the multiplication operator Mψf=ψf.M_{\psi}f=\psi f.

Classically, the study of weighted composition operators has been linked to isometries on Banach spaces. In fact, Banach [5] proved that the surjective isometries on C(Q)C(Q), the space of continuous real-valued functions on a compact metric space QQ, are of the form fψ(fφ)f\mapsto\psi(f\circ\varphi), where |ψ|1|\psi|\equiv 1 and φ\varphi is a homeomorphism of QQ onto itself. The characterization of isometries on most Banach spaces of analytic functions is still an open problem. However, there are many spaces for which the isometries are known. In many of these cases, the isometries have the form of a weighted composition operator. The interested reader is directed to [8, 12, 13].

The study of weighted composition operators is not limited to the study of isometries. Moreover, properties of weighted composition operators are not solely determined by the composition and multiplication operators of which they are comprised. There are many examples of bounded (compact) weighted composition operators that are not comprised of bounded (compact) composition or multiplication operators. In the last section of this paper, we provide further examples of such weighted composition operators.

In recent years, spaces of functions defined on discrete structures such as infinite trees have been explored. These spaces provide discrete analogs to classical spaces of analytic functions on the open unit disk 𝔻\mathbb{D} in \mathbb{C}. A discrete version of the Bloch space was developed by Colonna and Easley [9] called the Lipschitz space. Further research on the Lipschitz space, as well as multiplication and composition operators acting on the Lipschitz space, has been conducted by Colonna, Easley, and the first author. The interested reader is directed to [9, 1]. In addition, a discrete analog of the Hardy space was developed by Muthukumar and Ponnusamy, and the multiplication and composition operators were studied [19, 18].

Of interest in this paper is a discrete analog to the weighted Banach spaces Hν(𝔻)H_{\nu}^{\infty}(\mathbb{D}), and their weighted composition operators, as studied in [6, 10, 17]. In [3], the discrete weighted Banach space LμL_{\mu}^{\infty} was defined, and the multiplication operators were studied. In [4], the authors furthered the operator theory on LμL_{\mu}^{\infty} by studying the composition operators. The study of composition operators on such discrete spaces poses more challenges than the study of multiplication operators. In this paper, we study the weighted composition operators on LμL_{\mu}^{\infty}.

1.1. Organization of the paper

In Section 2, we collect useful results on weighted Banach spaces of an unbounded, locally finite metric space, as well as the little weighted Banach space.

In Section 3, we characterize the bounded weighted composition operators as well as determine their operator norms. We also provide necessary and sufficient conditions for the weighted composition operator to be bounded on the little weighted Banach space, while providing a complete characterization in two situations.

In Section 4, we characterize the compact weighted composition operators and determine their essential norm. These results lead to the characterization of compact multiplication and composition operators on the little weighted Banach space, which have not previously been studied.

In Section 5, we characterize the weighted composition operators that are injective, are bounded below, and have closed range. The application of these results to the multiplication operator yields the characterization of bounded below as in [3], but with a completely different proof.

In Section 6, we characterize the weighted composition operators that are invertible with bounded inverse. In addition, we characterize the isometries and surjective isometries among the weighted composition operators. This completes the characterization of the isometries and surjective isometries amongst the composition operators that was started in [4].

In Section 7, we characterize the so-called Fredholm weighted composition operators. This gives rise to characterizations of the Fredholm multiplication and composition operators as well. To date, this is the first study of Fredholm operators on such discrete spaces.

Finally, in Section 8, we illustrate the richness of the weighted composition operators acting on the weighted Banach spaces through several examples. We show in many cases that the weighted composition operator is more than the sum of its parts. Among the examples is a compact weighted composition operator for which neither the corresponding multiplication or composition operators are compact, and an isometric weighted composition operator for which the composition operator is not bounded.

1.2. Preliminary definitions and notation

The domains of the function spaces in this paper are metric spaces that are locally finite, with a distinguished element oo, called the root. Recall, a metric space (T,d)(T,\mathrm{d}) is locally finite if for every M>0M>0, the set {vT:d(o,v)<M}\{v\in T:\mathrm{d}(o,v)<M\} is finite. For a point vv in TT, we define the length of vv by |v|=d(o,v)\left\lvert v\right\rvert=\mathrm{d}(o,v). In this paper, we assume the locally finite metric space (T,d)(T,\mathrm{d}) has root oo and is unbounded, that is for every M>0M>0, there exists vTv\in T with |v|M\left\lvert v\right\rvert\geq M. As the length of a point is used throughout, and not specifically the metric d\mathrm{d}, we will denote the metric space simply by TT. Lastly, we denote by TT^{*} the set T{o}T\setminus\{o\}.

2. Weighted Banach Spaces

In this section, we define the weighted Banach spaces of an unbounded, locally finite metric space TT, and collect useful results for this paper. A positive function μ\mu on TT is called a weight. The weighted Banach space on TT with weight μ\mu, denoted Lμ(T)L_{\mu}^{\infty}(T) or simply LμL_{\mu}^{\infty}, is defined as the space of functions ff on TT for which

supvTμ(v)|f(v)|<.\sup_{v\in T}\;\mu(v)\left\lvert f(v)\right\rvert<\infty.

The little weighted Banach space on TT with weight μ\mu, denoted Lμ0(T)L_{\mu}^{0}(T) or simply Lμ0L_{\mu}^{0}, is the space of functions fLμf\in L_{\mu}^{\infty} for which

lim|v|μ(v)|f(v)|=0.\lim_{\left\lvert v\right\rvert\to\infty}\mu(v)\left\lvert f(v)\right\rvert=0.

It was shown in [3] that, when TT is an infinite rooted tree, the space Lμ(T)L_{\mu}^{\infty}(T) endowed with the norm

fμ=supvTμ(v)|f(v)|\|f\|_{\mu}=\sup_{v\in T}\mu(v)\left\lvert f(v)\right\rvert

is a functional Banach space, that is, a Banach space for which every point-evaluation functional Kv:Lμ(T)K_{v}:L_{\mu}^{\infty}(T)\to\mathbb{C}, ff(v)f\mapsto f(v), is bounded for all vTv\in T. The proof of [3] carries forward for a locally finite metric space TT. It was shown in [2] that Lμ0L_{\mu}^{0} is a closed, separable subspace of LμL_{\mu}^{\infty}. The following lemmas capture the properties most relevant to our work here. We note that similar statements can be made for Lμ0L_{\mu}^{0}.

Lemma 2.1 ([4, Lemma 2.6]).

Suppose ff is a function in LμL_{\mu}^{\infty}. Then for all vTv\in T, it holds that

|f(v)|1μ(v)fμ.\left\lvert f(v)\right\rvert\leq\frac{1}{\mu(v)}\|f\|_{\mu}.

We call a weight function μ\mu typical if lim|v|μ(v)=0.\lim_{\left\lvert v\right\rvert\to\infty}\mu(v)=0. The next result shows that little weighted Banach spaces containing the constant functions are precisely those with a typical weight.

Lemma 2.2.

The constant function 1 is an element of Lμ0L_{\mu}^{0} if and only if μ\mu is a typical weight.

Lemma 2.3.

For wTw\in T, the functions f(v)=χw(v)f(v)=\mbox{\Large$\chi$}_{w}(v) and g(v)=1μ(v)χw(v)g(v)=\frac{1}{\mu(v)}\mbox{\Large$\chi$}_{w}(v) are elements of Lμ0L_{\mu}^{0} with fμ=μ(w)\|f\|_{\mu}=\mu(w) and gμ=1\|g\|_{\mu}=1.

Lemma 2.4.

If {vi}i=1n\{v_{i}\}_{i=1}^{n} is a set of distinct points in TT, then the set of point-evaluation functionals {Kvi}i=1n\{K_{v_{i}}\}_{i=1}^{n} is linearly independent in (Lμ)(L_{\mu}^{\infty})^{*}.

Proof.

The statement follows immediately by considering functions fi(v)=χvi(v)f_{i}(v)=\mbox{\Large$\chi$}_{v_{i}}(v) since each fif_{i} vanishes everywhere except viv_{i}. ∎

3. Boundedness and Operator Norm

In this section, we study the boundedness of weighted composition operators acting on LμL_{\mu}^{\infty} and Lμ0L_{\mu}^{0}. In this endeavor, we define the following quantities for ψ\psi a function on TT and φ\varphi a self-map of TT:

σψ,φ=supvTμ(v)μ(φ(v))|ψ(v)|\sigma_{\psi,\varphi}=\sup_{v\in T}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert

and

ξψ,φ=lim|v|μ(v)μ(φ(v))|ψ(v)|,\xi_{\psi,\varphi}=\lim_{\left\lvert v\right\rvert\to\infty}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert,

if the limit exists. For the boundedness of Wψ,φW_{\psi,\varphi} on LμL_{\mu}^{\infty}, the quantity σψ,φ\sigma_{\psi,\varphi} is the characterizing quantity.

Remark 3.1.

Note if φ\varphi is a self-map of TT with finite range, them ξψ,φ=0\xi_{\psi,\varphi}=0 if and only if lim|v|μ(v)|ψ(v)|=0\lim_{\left\lvert v\right\rvert\to\infty}\mu(v)\left\lvert\psi(v)\right\rvert=0. This follows directly from the definition of ξψ,φ\xi_{\psi,\varphi} and the existence of positive constants m,Mm,M such that mμ(φ(v))Mm\leq\mu(\varphi(v))\leq M for all vTv\in T.

We summarize the main results of this section in the following theorem.

Theorem.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT.

  1. (a)

    The operator Wψ,φ:LμLμW_{\psi,\varphi}:L_{\mu}^{\infty}\to L_{\mu}^{\infty} is bounded if and only if σψ,φ\sigma_{\psi,\varphi} is finite. In this case, Wψ,φ=σψ,φ\|W_{\psi,\varphi}\|=\sigma_{\psi,\varphi}.

  2. (b)

    For the operator Wψ,φ:Lμ0Lμ0W_{\psi,\varphi}:L_{\mu}^{0}\to L_{\mu}^{0},

    1. i.

      if φ\varphi has finite range, then Wψ,φW_{\psi,\varphi} is bounded if and only if ξψ,φ=0\xi_{\psi,\varphi}=0. In this case, Wψ,φ=σψ,φ\|W_{\psi,\varphi}\|=\sigma_{\psi,\varphi}.

    2. ii.

      if φ\varphi has infinite range and μ\mu is a typical weight, then Wψ,φW_{\psi,\varphi} is bounded if and only if ψLμ0\psi\in L_{\mu}^{0} and σψ,φ\sigma_{\psi,\varphi} is finite.

In the remainder of the section, we provide proofs to the elements of the above theorem, along with useful lemmas in a more digestible format.

Theorem 3.2.

Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT. Then Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} if and only if σψ,φ\sigma_{\psi,\varphi} is finite. Moreover, it holds that

Wψ,φ=σψ,φ.\|W_{\psi,\varphi}\|=\sigma_{\psi,\varphi}.
Proof.

Suppose Wψ,φW_{\psi,\varphi} is a bounded operator on LμL_{\mu}^{\infty}. We define the function g(v)=1μ(v)g(v)=\frac{1}{\mu(v)}, which is an element of LμL_{\mu}^{\infty} with gμ=1\|g\|_{\mu}=1. For a fixed point wTw\in T, it holds that

μ(w)μ(φ(w))|ψ(w)|\displaystyle\frac{\mu(w)}{\mu(\varphi(w))}\left\lvert\psi(w)\right\rvert supvTμ(v)μ(φ(v))|ψ(v)|\displaystyle\leq\sup_{v\in T}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert (3.1)
=supvTμ(v)|ψ(v)||g(φ(v))|\displaystyle=\sup_{v\in T}\;\mu(v)\left\lvert\psi(v)\right\rvert\left\lvert g(\varphi(v))\right\rvert
=Wψ,φgμ\displaystyle=\|W_{\psi,\varphi}g\|_{\mu}
Wψ,φ.\displaystyle\leq\|W_{\psi,\varphi}\|.

Taking the supremum over all wTw\in T, it follows that σψ,φWψ,φ.\sigma_{\psi,\varphi}\leq\|W_{\psi,\varphi}\|. Thus σψ,φ\sigma_{\psi,\varphi} is finite.

Conversely, suppose σψ,φ\sigma_{\psi,\varphi} is finite and let fLμf\in L_{\mu}^{\infty} with fμ1\|f\|_{\mu}\leq 1. From Lemma 2.1, it follows that

Wψ,φfμ=supvTμ(v)|ψ(v)||f(φ(v))|supvTμ(v)μ(φ(v))|ψ(v)|fμσψ,φ.\|W_{\psi,\varphi}f\|_{\mu}=\sup_{v\in T}\;\mu(v)\left\lvert\psi(v)\right\rvert\left\lvert f(\varphi(v))\right\rvert\leq\sup_{v\in T}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\|f\|_{\mu}\leq\sigma_{\psi,\varphi}. (3.2)

Thus, Wψ,φW_{\psi,\varphi} is a bounded operator on LμL_{\mu}^{\infty}. Taking the supremum over all such functions ff, we obtain Wψ,φσψ,φ\|W_{\psi,\varphi}\|\leq\sigma_{\psi,\varphi}. ∎

In much of the analysis for weighted composition operators Wψ,φW_{\psi,\varphi} on the discrete weighted Banach spaces, the behavior of the operator depends on the image of TT under φ\varphi. We study the behavior in terms of φ\varphi having either finite or infinite range. When a self-map φ\varphi of TT has infinite range then, since TT is locally finite, there must exist a sequence of points (vn)(v_{n}) in TT with |vn|\left\lvert v_{n}\right\rvert\to\infty such that |φ(vn)|\left\lvert\varphi(v_{n})\right\rvert\to\infty.

In the rest of this section, we characterize the boundedness of Wψ,φW_{\psi,\varphi} on Lμ0L_{\mu}^{0}. By the Closed Graph Theorem and the boundedness of the evaluation functionals, to show the weighted composition operator is bounded, it suffices to show it maps Lμ0L_{\mu}^{0} into itself. We will exploit this reduction frequently. In the next two results, we show that ξψ,φ=0\xi_{\psi,\varphi}=0 is a sufficient condition for boundedness on Lμ0L_{\mu}^{0}. and, for φ\varphi with finite range, it is also necessary.

Lemma 3.3.

Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT. If ξψ,φ=0\xi_{\psi,\varphi}=0, then Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0}. Moreover, it holds that Wψ,φσψ,φ\|W_{\psi,\varphi}\|\leq\sigma_{\psi,\varphi}.

Proof.

Suppose ξψ,φ=0\xi_{\psi,\varphi}=0. It follows that σψ,φ\sigma_{\psi,\varphi} is finite, and thus Wψ,φW_{\psi,\varphi} is bounded as an operator on LμL_{\mu}^{\infty}. To show Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0}, it suffices to show Wψ,φW_{\psi,\varphi} maps Lμ0L_{\mu}^{0} into Lμ0L_{\mu}^{0}. Let fLμ0f\in L_{\mu}^{0} and (vn)(v_{n}) be a sequence in TT with |vn|\left\lvert v_{n}\right\rvert\to\infty as nn\to\infty. From Lemma 2.1 it follows that

μ(vn)|ψ(vn)||f(φ(vn))|μ(vn)μ(φ(vn))|ψ(vn)|fμ0\mu(v_{n})\left\lvert\psi(v_{n})\right\rvert\left\lvert f(\varphi(v_{n}))\right\rvert\leq\frac{\mu(v_{n})}{\mu(\varphi(v_{n}))}\left\lvert\psi(v_{n})\right\rvert\|f\|_{\mu}\to 0

as nn\to\infty. Thus Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0}. Moreover, from (3.2) it follows that Wψ,φσψ,φ\|W_{\psi,\varphi}\|\leq\sigma_{\psi,\varphi}. ∎

Theorem 3.4.

Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT with finite range. Then Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0} if and only if ξψ,φ=0.\xi_{\psi,\varphi}=0. Moreover, it holds that

Wψ,φ=σψ,φ.\|W_{\psi,\varphi}\|=\sigma_{\psi,\varphi}.
Proof.

Suppose Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0}. Since φ\varphi has finite range, it follows that the function g(v)=1μ(v)χφ(T)(v)g(v)=\frac{1}{\mu(v)}\mbox{\Large$\chi$}_{\varphi(T)}(v) is in Lμ0L_{\mu}^{0} with gμ=1\|g\|_{\mu}=1. Thus Wψ,φgW_{\psi,\varphi}g is in Lμ0L_{\mu}^{0} as well. For vTv\in T, we have

μ(v)μ(φ(v))|ψ(v)|\displaystyle\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert =μ(v)μ(φ(v))|ψ(v)|χφ(T)(φ(v))\displaystyle=\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mbox{\Large$\chi$}_{\varphi(T)}(\varphi(v)) (3.3)
=μ(v)|ψ(v)||g(φ(v))|\displaystyle=\mu(v)\left\lvert\psi(v)\right\rvert\left\lvert g(\varphi(v))\right\rvert
=μ(v)|(Wψ,φg)(v)|.\displaystyle=\mu(v)\left\lvert(W_{\psi,\varphi}g)(v)\right\rvert.

It immediately follows that ξψ,φ=0\xi_{\psi,\varphi}=0. Moreover, it holds that σψ,φWψ,φ\sigma_{\psi,\varphi}\leq\|W_{\psi,\varphi}\|. The converse follows from Lemma 3.3. ∎

The following lemma shows that boundedness on Lμ0L_{\mu}^{0} implies boundedness on LμL_{\mu}^{\infty}. With this result, we characterize the boundedness of Wψ,φW_{\psi,\varphi} on Lμ0L_{\mu}^{0} under a typical weight. As will be shown in future sections, the inverse image of φ(w)T\varphi(w)\in T under φ\varphi will play a role in determining characteristics of the weighted composition operator. To this end, for a point wTw\in T and φ\varphi a self-map of TT, we define Sw=φ1(φ(w))S_{w}=\varphi^{-1}(\varphi(w)).

Lemma 3.5.

Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT. If Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0}, then Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}.

Proof.

By Theorem 3.2, it suffices to show that σψ,φ<\sigma_{\psi,\varphi}<\infty. Fix wTw\in T and define the function g(v)=1μ(v)χφ(w)(v)g(v)=\frac{1}{\mu(v)}\mbox{\Large$\chi$}_{\varphi(w)}(v). From Lemma 2.3, gLμ0g\in L_{\mu}^{0} with gμ=1\|g\|_{\mu}=1. Define Y={fLμ0:fμ=1}Y=\{f\in L_{\mu}^{0}:\|f\|_{\mu}=1\}. Then

μ(w)μ(φ(w))|ψ(w)|\displaystyle\frac{\mu(w)}{\mu(\varphi(w))}\left\lvert\psi(w)\right\rvert supvSwμ(v)μ(φ(v))|ψ(v)|\displaystyle\leq\sup_{v\in S_{w}}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert
=supvTμ(v)μ(φ(v))|ψ(v)|χφ(w)(φ(v))\displaystyle=\sup_{v\in T}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mbox{\Large$\chi$}_{\varphi(w)}(\varphi(v))
=Wψ,φgμ\displaystyle=\|W_{\psi,\varphi}g\|_{\mu}
supfYWψ,φfμ\displaystyle\leq\sup_{f\in Y}\;\|W_{\psi,\varphi}f\|_{\mu}
=Wψ,φ:Lμ0Lμ0.\displaystyle=\left\|W_{\psi,\varphi}:L_{\mu}^{0}\to L_{\mu}^{0}\right\|.

Taking the supremum over all wTw\in T, we obtain σψ,φWψ,φ:Lμ0Lμ0\sigma_{\psi,\varphi}\leq\left\|W_{\psi,\varphi}:L_{\mu}^{0}\to L_{\mu}^{0}\right\|. Since Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0}, then σψ,φ<\sigma_{\psi,\varphi}<\infty and hence Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} by Theorem 3.2. ∎

Theorem 3.6.

Let μ\mu be a typical weight. Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT with infinite range. Then Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0} if and only if ψLμ0\psi\in L_{\mu}^{0} and σψ,φ<\sigma_{\psi,\varphi}<\infty.

Proof.

First suppose Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0}. Since μ\mu is a typical weight, the constant function 11 is an element of Lμ0L_{\mu}^{0} from Lemma 2.2. From the boundedness of Wψ,φW_{\psi,\varphi}, we have that Wψ,φ1=ψW_{\psi,\varphi}1=\psi is also an element of Lμ0L_{\mu}^{0}. In addition, Lemma 3.5 implies Wψ,φW_{\psi,\varphi} is bounded as an operator on LμL_{\mu}^{\infty}, and thus σψ,φ<\sigma_{\psi,\varphi}<\infty by Theorem 3.2.

Next, suppose ψLμ0\psi\in L_{\mu}^{0} and σψ,φ<\sigma_{\psi,\varphi}<\infty. To prove the boundedness of Wψ,φW_{\psi,\varphi}, it suffices to show the operator maps Lμ0L_{\mu}^{0} into Lμ0L_{\mu}^{0}. Let ε>0\varepsilon>0 and fLμ0f\in L_{\mu}^{0}. There exists a natural number N1N_{1} such that if |v|>N1\left\lvert v\right\rvert>N_{1}, then μ(v)|f(v)|<εσψ,φ\mu(v)\left\lvert f(v)\right\rvert<\frac{\varepsilon}{\sigma_{\psi,\varphi}}. Define m=1+sup|v|N1|f(v)|m=1+\sup_{\left\lvert v\right\rvert\leq N_{1}}\;\left\lvert f(v)\right\rvert and observe this quantity is finite and non-zero since the set {vT:|v|N1}\{v\in T:\left\lvert v\right\rvert\leq N_{1}\} is finite. In addition, there exists a natural number N2N_{2} such that if |v|>N2\left\lvert v\right\rvert>N_{2}, then μ(v)|ψ(v)|<εm\mu(v)\left\lvert\psi(v)\right\rvert<\frac{\varepsilon}{m}.

Let vTv\in T such that |v|>N2\left\lvert v\right\rvert>N_{2}. If |φ(v)|>N1\left\lvert\varphi(v)\right\rvert>N_{1}, then

μ(v)|ψ(v)||f(φ(v))|\displaystyle\mu(v)\left\lvert\psi(v)\right\rvert\left\lvert f(\varphi(v))\right\rvert =μ(v)μ(φ(v))|ψ(v)|μ(φ(v))|f(φ(v))|\displaystyle=\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert
σψ,φμ(φ(v))|f(φ(v))|\displaystyle\leq\sigma_{\psi,\varphi}\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert
<ε.\displaystyle<\varepsilon.

On the other hand, if |φ(v)|N1\left\lvert\varphi(v)\right\rvert\leq N_{1}, then

μ(v)|ψ(v)||f(φ(v))|μ(v)|ψ(v)|sup|v|N1|f(w)|<μ(v)|ψ(v)|m<ε.\mu(v)\left\lvert\psi(v)\right\rvert\left\lvert f(\varphi(v))\right\rvert\leq\mu(v)\left\lvert\psi(v)\right\rvert\sup_{\left\lvert v\right\rvert\leq N_{1}}\;\left\lvert f(w)\right\rvert<\mu(v)\left\lvert\psi(v)\right\rvert m<\varepsilon.

Thus

lim|v|μ(v)|ψ(v)||f(φ(v))|=0\lim_{\left\lvert v\right\rvert\to\infty}\mu(v)\left\lvert\psi(v)\right\rvert\left\lvert f(\varphi(v))\right\rvert=0

and Wψ,φfLμ0W_{\psi,\varphi}f\in L_{\mu}^{0}. ∎

We complete this section with boundedness characteristics for composition operators CφC_{\varphi} and multiplication operators MψM_{\psi} on Lμ0L_{\mu}^{0}, which were not studied in [4] or [3]. However, bounded composition operators on Lμ0L_{\mu}^{0} are further studied in [2]. For the composition operator induced by a self-map φ\varphi with finite range, the characterization for boundedness from Theorem 3.4 translates to lim|v|μ(v)μ(φ(v))=0\lim_{\left\lvert v\right\rvert\to\infty}\frac{\mu(v)}{\mu(\varphi(v))}=0. From Remark 3.1, this is equivalent to lim|v|μ(v)=0\lim_{\left\lvert v\right\rvert\to\infty}\mu(v)=0, i.e., μ\mu being a typical weight.

Corollary 3.7.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT.

  1. (a)

    For the operator Cφ:Lμ0Lμ0C_{\varphi}:L_{\mu}^{0}\to L_{\mu}^{0},

    1. i.

      If φ\varphi has finite range, then CφC_{\varphi} is bounded on Lμ0L_{\mu}^{0} if and only if μ\mu is a typical weight.

    2. ii.

      If φ\varphi has infinite range and μ\mu is a typical weight, then CφC_{\varphi} is bounded on Lμ0L_{\mu}^{0} if and only if CφC_{\varphi} is bounded on LμL_{\mu}^{\infty}.

  2. (b)

    If μ\mu is a typical weight, then Mψ:Lμ0Lμ0M_{\psi}:L_{\mu}^{0}\to L_{\mu}^{0} is bounded if and only if ψLμ0\psi\in L_{\mu}^{0}.

4. Compactness and Essential Norm

In this section, we study the compactness of weighted composition operators on the discrete weighted Banach spaces. As with boundedness, conditions for compactness depend on the image of TT under φ\varphi. We summarize the main results of this section in the following theorem.

Theorem.

Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}).

  1. (a)

    If φ\varphi has finite range, then Wψ,φW_{\psi,\varphi} is compact on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}).

  2. (b)

    If φ\varphi is infinite range, then

    1. i.

      The operator Wψ,φW_{\psi,\varphi} is compact on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}) if and only if

      limNsup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|=0.\lim_{N\to\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=0.
    2. ii.

      If μ\mu is a typical weight, then Wψ,φW_{\psi,\varphi} is compact on Lμ0L_{\mu}^{0} if and only if ξψ,φ=0\xi_{\psi,\varphi}=0.

Our first result in this section shows that self-maps with finite range induce compact weighted composition operators on both LμL_{\mu}^{\infty} and Lμ0L_{\mu}^{0}, independent of the multiplication symbol. This result utilizes the sequence characterization of compactness contained in the next lemma.

Lemma 4.1 ([3, Lemma 2.5]).

Let X,YX,Y be two Banach spaces of functions on an unbounded, locally finite metric space (T,d)(T,\mathrm{d}). Suppose that

  1. (a)

    the point evaluation functionals of XX are bounded,

  2. (b)

    the closed unit ball of XX is a compact subset of XX in the topology of uniform convergence on compact sets,

  3. (c)

    A:XYA:X\to Y is bounded when XX and YY are given the topology of uniform convergence on compact sets.

Then AA is a compact operator if and only if given a bounded sequence (fn)(f_{n}) in XX such that fn0f_{n}\to 0 pointwise, then the sequence (Afn)(Af_{n}) converges to zero in the norm of YY.

Theorem 4.2.

Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT with finite range for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}). Then Wψ,φW_{\psi,\varphi} is compact on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}).

Proof.

We will prove compactness on LμL_{\mu}^{\infty}, as the proof for the Lμ0L_{\mu}^{0} case is identical. Since Wψ,φW_{\psi,\varphi} is bounded, from Theorem 3.2 we have that σψ,φ\sigma_{\psi,\varphi} is finite. Let (fn)(f_{n}) be a bounded sequence in LμL_{\mu}^{\infty} converging to 0 pointwise and fix ε>0\varepsilon>0. Since φ(T)\varphi(T) is finite, there exists a positive constant mm such that supwφ(T)μ(w)m\sup_{w\in\varphi(T)}\;\mu(w)\leq m. Also, the pointwise convergence of (fn)(f_{n}) to 0 is uniform on φ(T)\varphi(T). Thus, for sufficiently large nn, we have supwφ(T)|fn(w)|<εmσψ,φ\sup_{w\in\varphi(T)}\;\left\lvert f_{n}(w)\right\rvert<\frac{\varepsilon}{m\sigma_{\psi,\varphi}}. With these observations, we see for such nn,

Wψ,φfnμ\displaystyle\|W_{\psi,\varphi}f_{n}\|_{\mu} =supvTμ(v)|ψ(v)fn(φ(v))|\displaystyle=\sup_{v\in T}\;\mu(v)\left\lvert\psi(v)f_{n}(\varphi(v))\right\rvert
=supvTμ(v)μ(φ(v))|ψ(v)|μ(φ(v))|fn(φ(v))|\displaystyle=\sup_{v\in T}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mu(\varphi(v))\left\lvert f_{n}(\varphi(v))\right\rvert
σψ,φsupwφ(T)μ(w)|fn(w)|\displaystyle\leq\sigma_{\psi,\varphi}\sup_{w\in\varphi(T)}\;\mu(w)\left\lvert f_{n}(w)\right\rvert
mσψ,φsupwφ(T)|fn(w)|\displaystyle\leq m\sigma_{\psi,\varphi}\sup_{w\in\varphi(T)}\;\left\lvert f_{n}(w)\right\rvert
<ε.\displaystyle<\varepsilon.

So Wψ,φfnμ0\|W_{\psi,\varphi}f_{n}\|_{\mu}\to 0 as nn\to\infty. Thus by Lemma 4.1, Wψ,φW_{\psi,\varphi} is compact on LμL_{\mu}^{\infty}. ∎

In view of the previous theorem, we assume in the rest of this section that φ\varphi has an infinite range and determine the compactness of the operator Wψ,φW_{\psi,\varphi} by computing its essential norm. To this end, we employ the following sequence of compact operators. First, for fLμf\in L_{\mu}^{\infty} and nn\in\mathbb{N}, define a function fnLμf_{n}\in L_{\mu}^{\infty} by

fn(v)={f(v)if |v|n0if |v|>n.f_{n}(v)=\begin{cases}f(v)&\text{if $\left\lvert v\right\rvert\leq n$}\\ 0&\text{if $\left\lvert v\right\rvert>n$}.\end{cases}

Then define the operator AnA_{n} by Anf=fnA_{n}f=f_{n}. It is easy to see that these operators are linear. The following lemma captures the other most relevant properties.

Lemma 4.3.

For each nn\in\mathbb{N}, the operator AnA_{n} is compact on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}) with An1\|A_{n}\|\leq 1 and IAn1.\|I-A_{n}\|\leq 1.

Theorem 4.4.

Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT with infinite range for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}). Then

Wψ,φe=limNsup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|\|W_{\psi,\varphi}\|_{e}=\lim_{N\to\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert (4.1)

as an operator on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}).

Proof.

We will compute the essential norm for Wψ,φW_{\psi,\varphi} acting on LμL_{\mu}^{\infty}, as the proof for the Lμ0L_{\mu}^{0} case is identical. Observe Wψ,φAnW_{\psi,\varphi}A_{n} is compact for all nn\in\mathbb{N} since Wψ,φW_{\psi,\varphi} is bounded and AnA_{n} is compact from Lemma 4.3. From the definition of the essential norm, we have

Wψ,φeWψ,φWψ,φAn=supfμ1supvTμ(v)|(Wψ,φ(IAn)f)(v)|\|W_{\psi,\varphi}\|_{e}\leq\|W_{\psi,\varphi}-W_{\psi,\varphi}A_{n}\|=\sup_{\|f\|_{\mu}\leq 1}\;\sup_{v\in T}\;\mu(v)\left\lvert(W_{\psi,\varphi}(I-A_{n})f)(v)\right\rvert (4.2)

for every nn\in\mathbb{N}. Now fix NN\in\mathbb{N}. We define

RN(n)\displaystyle R_{N}(n) =supfμ1sup|φ(v)|Nμ(v)|(Wψ,φ(IAn)f)(v)|\displaystyle=\sup_{\|f\|_{\mu}\leq 1}\;\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\mu(v)\left\lvert(W_{\psi,\varphi}(I-A_{n})f)(v)\right\rvert

and

SN(n)\displaystyle S_{N}(n) =supfμ1sup|φ(v)|Nμ(v)|(Wψ,φ(IAn)f)(v)|.\displaystyle=\sup_{\|f\|_{\mu}\leq 1}\;\sup_{\left\lvert\varphi(v)\right\rvert\leq N}\;\mu(v)\left\lvert(W_{\psi,\varphi}(I-A_{n})f)(v)\right\rvert.

Then, from (4.2) we obtain

Wψ,φemax{RN(n),SN(n)}\|W_{\psi,\varphi}\|_{e}\leq\max\{R_{N}(n),S_{N}(n)\}

for each n,Nn,N\in\mathbb{N}. We now consider the case n>Nn>N. From Lemma 4.3, we obtain

RN(n)\displaystyle R_{N}(n) =supfμ1sup|φ(v)|Nμ(v)μ(φ(v))μ(φ(v))|(Wψ,φ(IAn)f)(v)|\displaystyle=\sup_{\|f\|_{\mu}\leq 1}\;\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\mu(\varphi(v))\left\lvert(W_{\psi,\varphi}(I-A_{n})f)(v)\right\rvert
=supfμ1sup|φ(v)|Nμ(v)μ(φ(v))μ(φ(v))|ψ(v)||((IAn)f)(φ(v))|\displaystyle=\sup_{\|f\|_{\mu}\leq 1}\;\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\mu(\varphi(v))\left\lvert\psi(v)\right\rvert\left\lvert((I-A_{n})f)(\varphi(v))\right\rvert
supfμ1sup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|supwTμ(w)|((IAn)f)(w)|\displaystyle\leq\sup_{\|f\|_{\mu}\leq 1}\;\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\sup_{w\in T}\;\mu(w)\left\lvert((I-A_{n})f)(w)\right\rvert
=sup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|supfμ1supwTμ(w)|((IAn)f)(w)|\displaystyle=\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\sup_{\|f\|_{\mu}\leq 1}\;\sup_{w\in T}\;\mu(w)\left\lvert((I-A_{n})f)(w)\right\rvert
=sup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|IAn\displaystyle=\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\|I-A_{n}\|
sup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|.\displaystyle\leq\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert.

Next, observe that

SN(n)\displaystyle S_{N}(n) =supfμ1sup|φ(v)|Nμ(v)μ(φ(v))μ(φ(v))|(Wψ,φ(IAn)f)(v)|\displaystyle=\sup_{\|f\|_{\mu}\leq 1}\;\sup_{\left\lvert\varphi(v)\right\rvert\leq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\mu(\varphi(v))\left\lvert(W_{\psi,\varphi}(I-A_{n})f)(v)\right\rvert
=supfμ1sup|φ(v)|Nμ(v)μ(φ(v))μ(φ(v))|ψ(v)||((IAn)f)(φ(v))|\displaystyle=\sup_{\|f\|_{\mu}\leq 1}\;\sup_{\left\lvert\varphi(v)\right\rvert\leq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\mu(\varphi(v))\left\lvert\psi(v)\right\rvert\left\lvert((I-A_{n})f)(\varphi(v))\right\rvert
supfμ1sup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|sup|w|Nμ(w)|((IAn)f)(w)|.\displaystyle\leq\sup_{\|f\|_{\mu}\leq 1}\;\sup_{\left\lvert\varphi(v)\right\rvert\leq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\sup_{\left\lvert w\right\rvert\leq N}\;\mu(w)\left\lvert((I-A_{n})f)(w)\right\rvert.

If |w|N\left\lvert w\right\rvert\leq N and n>Nn>N, then ((IAn)f)(w)=0((I-A_{n})f)(w)=0 and we have SN(n)=0S_{N}(n)=0. Thus, for n>Nn>N,

Wψ,φemax{RN(n),SN(n)}RN(n)sup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|.\|W_{\psi,\varphi}\|_{e}\leq\max\{R_{N}(n),S_{N}(n)\}\leq R_{N}(n)\leq\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert.

This estimate holds for all NN\in\mathbb{N}, and hence

Wψ,φelimNsup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|.\|W_{\psi,\varphi}\|_{e}\leq\lim_{N\rightarrow\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert.

Now assume the essential norm of Wψ,φW_{\psi,\varphi} is strictly less than the limit in (4.1). Then there is a compact operator KK and constant s>0s>0 such that

Wψ,φK<s<limNsup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|.\|W_{\psi,\varphi}-K\|<s<\lim_{N\rightarrow\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert.

Moreover, we can find a sequence of points (vn)(v_{n}) with |φ(vn)|\left\lvert\varphi(v_{n})\right\rvert\rightarrow\infty such that

lim supnμ(vn)μ(φ(vn))|ψ(vn)|>s.\limsup_{n\rightarrow\infty}\frac{\mu(v_{n})}{\mu(\varphi(v_{n}))}\left\lvert\psi(v_{n})\right\rvert>s. (4.3)

Now, define the sequence of functions (fn)(f_{n}) by

fn(v)=1μ(v)χφ(vn)(v).f_{n}(v)=\frac{1}{\mu(v)}\mbox{\Large$\chi$}_{\varphi(v_{n})}(v).

By [4, Lemmas 2.4 and 2.5], this is a bounded sequence of functions in LμL_{\mu}^{\infty}, with fnμ=1\|f_{n}\|_{\mu}=1 for all nn\in\mathbb{N}, converging to zero pointwise. We also have the lower estimate,

s>Wψ,φK(Wψ,φK)fnμWψ,φfnμKfnμ.s>\|W_{\psi,\varphi}-K\|\geq\|(W_{\psi,\varphi}-K)f_{n}\|_{\mu}\geq\|W_{\psi,\varphi}f_{n}\|_{\mu}-\|Kf_{n}\|_{\mu}.

By Lemma 4.1, Kfnμ0\|Kf_{n}\|_{\mu}\rightarrow 0 as nn\to\infty, and thus

s\displaystyle s lim supn(Wψ,φfnμKfnμ)\displaystyle\geq\limsup_{n\rightarrow\infty}\left(\|W_{\psi,\varphi}f_{n}\|_{\mu}-\|Kf_{n}\|_{\mu}\right)
=lim supnWψ,φfnμ\displaystyle=\limsup_{n\rightarrow\infty}\|W_{\psi,\varphi}f_{n}\|_{\mu}
lim supnμ(vn)|ψ(vn)fn(φ(vn))|\displaystyle\geq\limsup_{n\rightarrow\infty}\mu(v_{n})\left\lvert\psi(v_{n})f_{n}(\varphi(v_{n}))\right\rvert
=lim supnμ(vn)μ(φ(vn))|ψ(vn)|\displaystyle=\limsup_{n\rightarrow\infty}\frac{\mu(v_{n})}{\mu(\varphi(v_{n}))}\left\lvert\psi(v_{n})\right\rvert
>s,\displaystyle>s,

which is a contradiction. Therefore

Wψ,φe=limNsup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|,\|W_{\psi,\varphi}\|_{e}=\lim_{N\to\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert,

as desired ∎

Corollary 4.5.

Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT with infinite range for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}). Then Wψ,φW_{\psi,\varphi} is compact on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}) if and only if

limNsup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|=0.\lim_{N\to\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=0.

For the spaces constructed with typical weights we can reformulate the essential norm of Wψ,φW_{\psi,\varphi} acting on Lμ0L_{\mu}^{0} to be a limit superior, and furthermore the characterization of compactness as ξψ,φ=0\xi_{\psi,\varphi}=0.

Theorem 4.6.

Let μ\mu be a typical weight. Suppose ψ\psi is a function on TT and φ\varphi is a self-map of TT with infinite range for which Wψ,φW_{\psi,\varphi} is bounded on Lμ0L_{\mu}^{0}. Then

Wψ,φe=lim sup|v|μ(v)μ(φ(v))|ψ(v)|.\|W_{\psi,\varphi}\|_{e}=\limsup_{\left\lvert v\right\rvert\to\infty}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert. (4.4)

Moreover, Wψ,φW_{\psi,\varphi} is compact on Lμ0L_{\mu}^{0} if and only if

lim|v|μ(v)μ(φ(v))|ψ(v)|=0.\lim_{\left\lvert v\right\rvert\to\infty}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=0.
Proof.

To establish the essential norm, by Theorem 4.4 it suffices to show the limit in (4.1) is equal to the limit superior in (4.4). We will first show the limit to be less than or equal to the limit superior.

For nn\in\mathbb{N}, define

tn=min{m:|φ(v)|n for some vT with |v|>m}.t_{n}=\min\{m\in\mathbb{N}:\left\lvert\varphi(v)\right\rvert\geq n\text{ for some }v\in T\text{ with }\left\lvert v\right\rvert>m\}.

We claim |tn|\left\lvert t_{n}\right\rvert\to\infty as nn\to\infty. If this is not the case, then there exists NN\in\mathbb{N} and a sequence of points (vn)(v_{n}) with |vn|N\left\lvert v_{n}\right\rvert\leq N and |φ(vn)|\left\lvert\varphi(v_{n})\right\rvert\to\infty. But this is impossible since {vT:|v|N}\{v\in T:\left\lvert v\right\rvert\leq N\} is finite. Then the set {vT:|v|>tn}\{v\in T:\left\lvert v\right\rvert>t_{n}\} is precisely

{vT:|φ(v)|n and |v|>tn}{vT:|φ(v)|<n and |v|>tn}.\{v\in T:\left\lvert\varphi(v)\right\rvert\geq n\text{ and }\left\lvert v\right\rvert>t_{n}\}\cup\{v\in T:\left\lvert\varphi(v)\right\rvert<n\text{ and }\left\lvert v\right\rvert>t_{n}\}.

This implies

limNsup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|\displaystyle\lim_{N\to\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert limnsup|v|>tnμ(v)μ(φ(v))|ψ(v)|\displaystyle\leq\lim_{n\to\infty}\sup_{\left\lvert v\right\rvert>t_{n}}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert (4.5)
=lim sup|v|μ(v)μ(φ(v))|ψ(v)|,\displaystyle=\limsup_{\left\lvert v\right\rvert\to\infty}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert,

where the inequality is due to the fact that tnt_{n} is defined as a minimum.

Now we will show equality must hold. There exists a sequence of vertices (vn)(v_{n}) with |vn|\left\lvert v_{n}\right\rvert\to\infty and

limnμ(vn)μ(φ(vn))|ψ(vn)|\displaystyle\lim_{n\to\infty}\frac{\mu(v_{n})}{\mu(\varphi(v_{n}))}\left\lvert\psi(v_{n})\right\rvert =limNsup|v|Nμ(v)μ(φ(v))|ψ(v)|\displaystyle=\lim_{N\to\infty}\sup_{\left\lvert v\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert (4.6)
=lim sup|v|μ(v)μ(φ(v))|ψ(v)|,\displaystyle=\limsup_{\left\lvert v\right\rvert\to\infty}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert,

i.e. the limit superior is attained along this sequence. If the sequence (φ(vn))(\varphi(v_{n})) is bounded, then ψLμ0\psi\in L_{\mu}^{0} (a consequence of the fact that μ\mu is typical) and (4.6) imply

lim sup|v|μ(v)μ(φ(v))|ψ(v)|=limnμ(vn)μ(φ(vn))|ψ(vn)|=0.\limsup_{\left\lvert v\right\rvert\to\infty}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=\lim_{n\to\infty}\frac{\mu(v_{n})}{\mu(\varphi(v_{n}))}\left\lvert\psi(v_{n})\right\rvert=0.

From (4.5) we have

limNsup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|=0\lim_{N\to\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=0

as well.

Finally, if (φ(vn))(\varphi(v_{n})) is not bounded, then there exists a subsequence (vnk)(v_{n_{k}}) with |vnk|\left\lvert v_{n_{k}}\right\rvert\to\infty and |φ(vnk)|\left\lvert\varphi(v_{n_{k}})\right\rvert\to\infty. Then, by (4.5), we have

limkμ(vnk)μ(φ(vnk))|ψ(vnk)|\displaystyle\lim_{k\to\infty}\frac{\mu(v_{n_{k}})}{\mu(\varphi(v_{n_{k}}))}\left\lvert\psi(v_{n_{k}})\right\rvert limNsup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|\displaystyle\leq\lim_{N\to\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert
lim sup|v|μ(v)μ(φ(v))|ψ(v)|\displaystyle\leq\limsup_{\left\lvert v\right\rvert\to\infty}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert

since |φ(vnk)|.\left\lvert\varphi(v_{n_{k}})\right\rvert\to\infty. From (4.6), it follows that equality must hold in this case as well. The compactness of Wψ,φW_{\psi,\varphi} on Lμ0L_{\mu}^{0} follows immediately. ∎

We complete this section with compactness characteristics for composition operators CφC_{\varphi} and multiplication operators MψM_{\psi} on Lμ0L_{\mu}^{0}, which were not studied in [4] or [3].

Corollary 4.7.

Suppose ψ\psi is a function on TT and φ\varphi a self-map of TT for which CφC_{\varphi} and MψM_{\psi} are bounded on Lμ0L_{\mu}^{0}.

  1. (a)

    For the composition operator CφC_{\varphi},

    1. i.

      if φ\varphi has finite range, then CφC_{\varphi} is compact on Lμ0L_{\mu}^{0}.

    2. ii.

      if φ\varphi has infinite range, then CφC_{\varphi} is compact on Lμ0L_{\mu}^{0} if and only if

      limNsup|φ(v)|Nμ(v)μ(φ(v))=0.\lim_{N\to\infty}\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}=0.
    3. iii.

      if φ\varphi has infinite range and μ\mu is a typical weight, then CφC_{\varphi} is compact on Lμ0L_{\mu}^{0} if and only if

      lim|v|μ(v)μ(φ(v))=0.\lim_{\left\lvert v\right\rvert\to\infty}\frac{\mu(v)}{\mu(\varphi(v))}=0.
  2. (b)

    The operator MψM_{\psi} is compact on Lμ0L_{\mu}^{0} if and only if

    lim|v||ψ(v)|=0.\lim_{\left\lvert v\right\rvert\to\infty}\left\lvert\psi(v)\right\rvert=0.

5. Boundedness From Below and Closed Range

Recall a bounded operator A:XYA:X\to Y between Banach spaces is bounded below if there exists a positive constant δ\delta such that AxYδxX\|Ax\|_{Y}\geq\delta\|x\|_{X} for all xXx\in X. As a consequence of the Open Mapping Theorem, a bounded operator AA is bounded below if and only if it is injective and has closed range [11, Proposition VII.6.4]. Thus, we first characterize the injective weighted composition operators on LμL_{\mu}^{\infty} to aid in the characterization of those operators that are bounded below.

To identify the injective weighted composition operators, we define the set Z=ψ1(0)Z=\psi^{-1}(0). Recall, for wTw\in T and φ\varphi a self-map of TT, the set Sw=φ1(φ(w)).S_{w}=\varphi^{-1}(\varphi(w)).

Theorem 5.1.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT. Then Wψ,φW_{\psi,\varphi}, as an operator on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}), is injective if and only if φ\varphi is surjective and for every wTw\in T, SwZcS_{w}\cap Z^{c}\neq\emptyset.

Proof.

First, suppose φ\varphi is surjective and for every wTw\in T, SwZcS_{w}\cap Z^{c}\neq\emptyset. Let ff be a function in Lμ0L_{\mu}^{0} or LμL_{\mu}^{\infty} that is not the zero function. Then there is a point wTw\in T such that f(w)0f(w)\neq 0. Since φ\varphi is surjective, there is a vTv\in T with φ(v)=w\varphi(v)=w. From the condition on SvS_{v}, there is a point vSvv^{\prime}\in S_{v} such that ψ(v)0\psi(v^{\prime})\neq 0. Thus

(Wψ,φf)(v)=ψ(v)f(φ(v))=ψ(v)f(φ(v))=ψ(v)f(w)0.(W_{\psi,\varphi}f)(v^{\prime})=\psi(v^{\prime})f(\varphi(v^{\prime}))=\psi(v^{\prime})f(\varphi(v))=\psi(v^{\prime})f(w)\neq 0.

Hence Wψ,φfW_{\psi,\varphi}f is not the zero function, and Wψ,φW_{\psi,\varphi} is injective.

For the converse, first suppose φ\varphi is not surjective. Then there exists wTw\in T such that wφ(T)w\not\in\varphi(T). The function χw(v)\mbox{\Large$\chi$}_{w}(v) is a non-zero element of Lμ0L_{\mu}^{0} and Wψ,φf=0W_{\psi,\varphi}f=0. Hence, Wψ,φW_{\psi,\varphi} is not injective.

Next, suppose there exists wTw\in T such that SwZS_{w}\subseteq Z. Then the function χφ(w)\mbox{\Large$\chi$}_{\varphi(w)} is a non-zero element of Lμ0L_{\mu}^{0}, but Wψ,φχφ(w)=0W_{\psi,\varphi}\mbox{\Large$\chi$}_{\varphi(w)}=0. Thus, Wψ,φW_{\psi,\varphi} is not injective. In either case, Wψ,φW_{\psi,\varphi} is not injective, completing the proof. ∎

To characterize the weighted composition operators that are bounded below, we define the set UεU_{\varepsilon} as

Uε={vT:μ(v)μ(φ(v))|ψ(v)|ε}U_{\varepsilon}=\left\{v\in T:\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\geq\varepsilon\right\}

for ψ\psi a function on TT, φ\varphi a self-map of TT, and ε>0\varepsilon>0.

Theorem 5.2.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}). Then Wψ,φW_{\psi,\varphi} is bounded below if and only if φ\varphi is surjective and there is an ε>0\varepsilon>0 such that UεSwU_{\varepsilon}\cap S_{w}\neq\emptyset for every wTw\in T.

Proof.

First, suppose Wψ,φW_{\psi,\varphi} is bounded below. Then Wψ,φW_{\psi,\varphi} is injective and hence φ\varphi is surjective by Lemma 5.1. Also, there is an ε1>0\varepsilon_{1}>0 such that Wψ,φfμε1fμ\|W_{\psi,\varphi}f\|_{\mu}\geq\varepsilon_{1}\|f\|_{\mu} for all ff in LμL_{\mu}^{\infty} or Lμ0L_{\mu}^{0}. For wTw\in T, take f(v)=1μ(v)χφ(w)(v)f(v)=\frac{1}{\mu(v)}\mbox{\Large$\chi$}_{\varphi(w)}(v). Since fμ=1,\|f\|_{\mu}=1, we have Wψ,φfμε1\|W_{\psi,\varphi}f\|_{\mu}\geq\varepsilon_{1} or

supvTμ(v)μ(φ(v))|ψ(v)|χφ(w)(φ(v))=supvSwμ(v)μ(φ(v))|ψ(v)|ε1.\sup_{v\in T}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mbox{\Large$\chi$}_{\varphi(w)}(\varphi(v))=\sup_{v\in S_{w}}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\geq\varepsilon_{1}.

Fix 0<ε<ε10<\varepsilon<\varepsilon_{1}. It follows that for every wTw\in T, there must exist a vSwv\in S_{w} with

μ(v)μ(φ(v))|ψ(v)|ε\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\geq\varepsilon

and thus UεSwU_{\varepsilon}\cap S_{w}\neq\emptyset.

For the converse, suppose there is an ε>0\varepsilon>0 such that UεSwU_{\varepsilon}\cap S_{w}\neq\emptyset for every wTw\in T and φ\varphi is surjective. First, let fLμf\in L_{\mu}^{\infty}, and observe

Wψ,φfμ=supvTμ(v)|ψ(v)f(φ(v))|=supvTμ(v)μ(φ(v))|ψ(v)|μ(φ(v))|f(φ(v))|.\|W_{\psi,\varphi}f\|_{\mu}=\sup_{v\in T}\;\mu(v)\left\lvert\psi(v)f(\varphi(v))\right\rvert=\sup_{v\in T}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert.

For wTw\in T, there exists vUεSwv\in U_{\varepsilon}\cap S_{w} and thus

εμ(φ(w))|f(φ(w))|=εμ(φ(v))|f(φ(v))|μ(v)μ(φ(v))|ψ(v)|μ(φ(v))|f(φ(v))|.\varepsilon\mu(\varphi(w))\left\lvert f(\varphi(w))\right\rvert=\varepsilon\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert\leq\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert.

This implies

supwTεμ(φ(w))|f(φ(w))|supvTμ(v)μ(φ(v))|ψ(v)|μ(φ(v))|f(φ(v))|\sup_{w\in T}\;\varepsilon\mu(\varphi(w))\left\lvert f(\varphi(w))\right\rvert\leq\sup_{v\in T}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert

or

εsupwTμ(φ(w))|f(φ(w))|Wψ,φfμ.\varepsilon\sup_{w\in T}\;\mu(\varphi(w))\left\lvert f(\varphi(w))\right\rvert\leq\|W_{\psi,\varphi}f\|_{\mu}. (5.1)

Since φ\varphi is surjective, the supremum on the left is fμ\|f\|_{\mu} and thus, we have Wψ,φfμεfμ\|W_{\psi,\varphi}f\|_{\mu}\geq\varepsilon\|f\|_{\mu} as desired. ∎

Considering Theorems 5.1 and 5.2, it seems natural to expect that Wψ,φW_{\psi,\varphi} has closed range on LμL_{\mu}^{\infty} or Lμ0L_{\mu}^{0} if and only if there is an ε>0\varepsilon>0 such that UεSwU_{\varepsilon}\cap S_{w}\neq\emptyset for every ww for which ψ(w)0\psi(w)\neq 0. To verify this claim we will exploit quotient spaces and the fact that an injective operator is bounded below if and only if it has closed range. The following outlines the necessary details.

Let XX be a Banach space and A:XXA:X\to X a bounded linear operator. Then consider the quotient space X/ker(A).X/\ker(A). For xXx\in X,

[x]=x+ker(A)={x+m:mker(A)}={yX:Ax=Ay}[x]=x+\ker(A)=\{x+m:m\in\ker(A)\}=\{y\in X:Ax=Ay\}

and

[x]=inf{x+m:mker(A)}.\left\|[x]\right\|=\inf\{\|x+m\|:m\in\ker(A)\}.

One immediate consequence is that [x]x.\left\|[x]\right\|\leq\|x\|. Additionally, define an operator A^:X/ker(A)X\widehat{A}:X/\ker(A)\to X by A^[x]=Ax.\widehat{A}[x]=Ax. This map is well-defined since any y[x]y\in[x] satisfies Ax=AyAx=Ay. It is also easy to see that A^\widehat{A} is linear, injective, and bounded with A^A.\|\widehat{A}\|\leq\|A\|. Finally, range(A)=range(A^).\textup{range}(A)=\textup{range}(\widehat{A}). Thus, AA has closed range if and only if A^\widehat{A} has closed range. But, since A^\widehat{A} is injective, we know AA has closed range if and only if A^\widehat{A} is bounded below.

Theorem 5.3.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}). Then Wψ,φW_{\psi,\varphi} has closed range if and only if there is an ε>0\varepsilon>0 such that UεSwU_{\varepsilon}\cap S_{w}\neq\emptyset for every wZcw\in Z^{c}.

Proof.

Suppose Wψ,φW_{\psi,\varphi} has closed range. We will verify the conclusion for LμL_{\mu}^{\infty}, but the same argument suffices for Lμ0L_{\mu}^{0}. Then W^ψ,φ\widehat{W}_{\psi,\varphi} is bounded below by the discussion above and hence there is an ε1>0\varepsilon_{1}>0 with Wψ,φfμ=W^ψ,φ[f]με1[f]μ\|W_{\psi,\varphi}f\|_{\mu}=\|\widehat{W}_{\psi,\varphi}[f]\|_{\mu}\geq\varepsilon_{1}\|[f]\|_{\mu} for all fLμf\in L_{\mu}^{\infty}. For wZcw\in Z^{c}, take f(v)=1μ(v)χφ(w)(v)f(v)=\frac{1}{\mu(v)}\mbox{\Large$\chi$}_{\varphi(w)}(v). To estimate [f]μ\|[f]\|_{\mu}, let gker(Wψ,φ)g\in\ker(W_{\psi,\varphi}). Then g(φ(v))=0g(\varphi(v))=0 for all vZcv\in Z^{c}, which is equivalent to g(v)=0g(v)=0 for all vφ(Zc)v\in\varphi(Z^{c}). It follows that

f+gμ=supvTμ(v)|f(v)+g(v)|\displaystyle\|f+g\|_{\mu}=\sup_{v\in T}\mu(v)\left\lvert f(v)+g(v)\right\rvert supvφ(Zc)μ(v)|f(v)+g(v)|\displaystyle\geq\sup_{v\in\varphi(Z^{c})}\mu(v)\left\lvert f(v)+g(v)\right\rvert
=supvφ(Zc)μ(v)|f(v)|=1\displaystyle=\sup_{v\in\varphi(Z^{c})}\mu(v)\left\lvert f(v)\right\rvert=1

and

[f]μ=inf{f+gμ:gker(Cφ)}1.\|[f]\|_{\mu}=\inf\{\|f+g\|_{\mu}:g\in\ker(C_{\varphi})\}\geq 1.

But [f]μfμ=1\|[f]\|_{\mu}\leq\|f\|_{\mu}=1 and thus [f]μ=1.\|[f]\|_{\mu}=1. From this, for our chosen ff, we have Wψ,φfμ=W^ψ,φ[f]με1\|W_{\psi,\varphi}f\|_{\mu}=\|\widehat{W}_{\psi,\varphi}[f]\|_{\mu}\geq\varepsilon_{1} or

supvTμ(v)μ(φ(v))|ψ(v)|χφ(w)(φ(v))=supvSwμ(v)μ(φ(v))|ψ(v)|ε1.\sup_{v\in T}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mbox{\Large$\chi$}_{\varphi(w)}(\varphi(v))=\sup_{v\in S_{w}}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\geq\varepsilon_{1}.

For 0<ε<ε10<\varepsilon<\varepsilon_{1}, it follows that for every wZcw\in Z^{c}, there must exist a vSwv\in S_{w} with

μ(v)μ(φ(v))|ψ(v)|ε\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\geq\varepsilon

and thus UεSwU_{\varepsilon}\cap S_{w}\neq\emptyset.

For the converse, suppose there is an ε>0\varepsilon>0 such that UεSwU_{\varepsilon}\cap S_{w}\neq\emptyset for every wZcw\in Z^{c}. Similarly to the proof of the previous theorem, for wZcw\in Z^{c}, there is a vUεSwv\in U_{\varepsilon}\cap S_{w}. From this, for an arbitrary fLμf\in L_{\mu}^{\infty}, it follows that

εμ(φ(w))|f(φ(w))|=εμ(φ(v))|f(φ(v))|μ(v)μ(φ(v))|ψ(v)|μ(φ(v))|f(φ(v))|,\varepsilon\mu(\varphi(w))\left\lvert f(\varphi(w))\right\rvert=\varepsilon\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert\leq\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert,

which implies

supwZcεμ(φ(w))|f(φ(w))|supvTμ(v)μ(φ(v))|ψ(v)|μ(φ(v))|f(φ(v))|\sup_{w\in Z^{c}}\varepsilon\mu(\varphi(w))\left\lvert f(\varphi(w))\right\rvert\leq\sup_{v\in T}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert

or

εsupwZcμ(φ(w))|f(φ(w))|Wψ,φfμ.\varepsilon\sup_{w\in Z^{c}}\mu(\varphi(w))\left\lvert f(\varphi(w))\right\rvert\leq\|W_{\psi,\varphi}f\|_{\mu}. (5.2)

Now, to show the range of Wψ,φW_{\psi,\varphi} is closed, it suffices to show every Cauchy sequence in range(Wψ,φ)\textup{range}(W_{\psi,\varphi}) has its limit in range(Wψ,φ)\textup{range}(W_{\psi,\varphi}). Suppose (Wψ,φfn)(W_{\psi,\varphi}f_{n}) is such a Cauchy sequence. First define gn=fnχφ(Zc)g_{n}=f_{n}\mbox{\Large$\chi$}_{\varphi(Z^{c})}. Observe that

(Wψ,φgn)(v)=ψ(v)fn(φ(v))χφ(Zc)(φ(v))=ψ(v)fn(φ(v))=(Wψ,φfn)(v)(W_{\psi,\varphi}g_{n})(v)=\psi(v)f_{n}(\varphi(v))\mbox{\Large$\chi$}_{\varphi(Z^{c})}(\varphi(v))=\psi(v)f_{n}(\varphi(v))=(W_{\psi,\varphi}f_{n})(v)

for all vTv\in T and hence Wψ,φgn=Wψ,φfnW_{\psi,\varphi}g_{n}=W_{\psi,\varphi}f_{n} for all nn. From (5.2), we have

εsupwZcμ(φ(w))|gn(φ(w))gm(φ(w))|\displaystyle\varepsilon\sup_{w\in Z^{c}}\mu(\varphi(w))\left\lvert g_{n}(\varphi(w))-g_{m}(\varphi(w))\right\rvert Wψ,φgnWψ,φgmμ\displaystyle\leq\|W_{\psi,\varphi}g_{n}-W_{\psi,\varphi}g_{m}\|_{\mu}
=Wψ,φfnWψ,φfmμ.\displaystyle=\|W_{\psi,\varphi}f_{n}-W_{\psi,\varphi}f_{m}\|_{\mu}.

Also,

supwZcμ(φ(w))|gn(φ(w))gm(φ(w))|\displaystyle\sup_{w\in Z^{c}}\mu(\varphi(w))\left\lvert g_{n}(\varphi(w))-g_{m}(\varphi(w))\right\rvert =supvφ(Zc)μ(v)|gn(v)gm(v)|\displaystyle=\sup_{v\in\varphi(Z^{c})}\mu(v)\left\lvert g_{n}(v)-g_{m}(v)\right\rvert
=supvTμ(v)|gn(v)gm(v)|\displaystyle=\sup_{v\in T}\mu(v)\left\lvert g_{n}(v)-g_{m}(v)\right\rvert
=gngmμ\displaystyle=\|g_{n}-g_{m}\|_{\mu}

where the second equality is due to the definition of the sequence (gn)(g_{n}). Hence

εgngmμWψ,φgnWψ,φgmμ=Wψ,φfnWψ,φfmμ,\varepsilon\|g_{n}-g_{m}\|_{\mu}\leq\|W_{\psi,\varphi}g_{n}-W_{\psi,\varphi}g_{m}\|_{\mu}=\|W_{\psi,\varphi}f_{n}-W_{\psi,\varphi}f_{m}\|_{\mu},

which implies (gn)(g_{n}) is a Cauchy sequence in LμL_{\mu}^{\infty} (resp. Lμ0L_{\mu}^{0}). Setting gg to be the norm limit of (gn)(g_{n}), we have Wψ,φg=Wψ,φ(limgn)=limWψ,φgn=limWψ,φfnW_{\psi,\varphi}g=W_{\psi,\varphi}(\lim g_{n})=\lim W_{\psi,\varphi}g_{n}=\lim W_{\psi,\varphi}f_{n} and thus the range of Wψ,φW_{\psi,\varphi} is closed. ∎

It is important to note here that many of the results for the operators under investigation have properties similar to those in the continuous setting. However, in that setting, operators are typically injective by design and hence bounded below if and only if they have closed range. That is not true in this setting and so the utilization of the technique above is not required in the continuous setting (specifically in the case of analytic function spaces). Therefore this setting highlights the difference between operators that are bounded below and those that have closed range more finely than the continuous setting.

Theorem 5.1, with ψ1\psi\equiv 1 on TT, yields a characterization of the injective composition operators on LμL_{\mu}^{\infty} and Lμ0L_{\mu}^{0}.

Corollary 5.4.

Let φ\varphi be a self-map of TT. Then as an operator on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}), CφC_{\varphi} is injective if and only if φ\varphi is surjective.

Theorems 5.2 and 5.3 yield characterizations for composition operators that are bounded below or have closed range. In this case, we define the set VεV_{\varepsilon} to be

Vε={vT:μ(v)μ(φ(v))ε}V_{\varepsilon}=\left\{v\in T:\frac{\mu(v)}{\mu(\varphi(v))}\geq\varepsilon\right\}

for φ\varphi a self-map of TT, and ε>0\varepsilon>0.

Corollary 5.5.

Let φ\varphi be a self-map of TT, and suppose CφC_{\varphi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}). Then CφC_{\varphi} is bounded below if and only if φ\varphi is surjective and there is an ε>0\varepsilon>0 such that VεSwV_{\varepsilon}\cap S_{w}\neq\emptyset for every wTw\in T.

Corollary 5.6.

Let φ\varphi be a self-map of TT and assume CφC_{\varphi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}). Then CφC_{\varphi} has closed range if and only if there is an ε>0\varepsilon>0 such that VεSwV_{\varepsilon}\cap S_{w}\neq\emptyset for every wTw\in T.

To characterize the injective multiplication operators on LμL_{\mu}^{\infty} or Lμ0L_{\mu}^{0}, we can apply Theorem 5.1 to the weighted composition operator Wψ,φW_{\psi,\varphi} where φ\varphi is the identity map on TT. In this case, for a point wTw\in T, the set Sw={w}S_{w}=\{w\}.

Corollary 5.7.

Let ψ\psi be a function on TT. Then as an operator on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}), MψM_{\psi} is injective if and only if ψ(v)0\psi(v)\neq 0 for all vTv\in T.

For multiplication operators acting on LμL_{\mu}^{\infty}, a characterization of those that are bounded below was given in [3, Corollary 3.5] using spectral information. Theorem 5.2 provides a direct proof and extends the result to Lμ0L_{\mu}^{0}.

Corollary 5.8.

Let ψ\psi be a function on TT and assume MψM_{\psi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}). Then MψM_{\psi} is bounded below if and only if infvT|ψ(v)|>0\inf_{v\in T}\left\lvert\psi(v)\right\rvert>0.

For a multiplication operator to have closed range, 0 can be in the image of ψ\psi but cannot be a limit point; this provides the relevant contrast to Corollary 5.8. The result follows immediately from Theorem 5.3.

Corollary 5.9.

Let ψ\psi be a function on TT and suppose MψM_{\psi} is bounded on LμL_{\mu}^{\infty} (respectively Lμ0L_{\mu}^{0}). Then MψM_{\psi} has closed range if and only if infvZc|ψ(v)|>0\inf_{v\in Z^{c}}\left\lvert\psi(v)\right\rvert>0.

6. Invertible and Isometric Weighted Composition Operators

In the next two sections we explore ideas related to those in Section 5 and we restrict our attention to Wψ,φW_{\psi,\varphi} on LμL_{\mu}^{\infty}; some results carry over to Wψ,φW_{\psi,\varphi} on Lμ0L_{\mu}^{0} with the same proof while other results require more analysis. We begin with invertibility of weighted composition operators. Bourdon [7] noted that when defined, W1/ψφ1,φ1W_{1/\psi\circ\varphi^{-1},\varphi^{-1}} is the inverse of Wψ,φW_{\psi,\varphi}.

Theorem 6.1.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}. Then Wψ,φW_{\psi,\varphi} has a bounded inverse if and only if φ\varphi is bijective and

infvTμ(v)μ(φ(v))|ψ(v)|>0.\inf_{v\in T}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert>0.

In this case, we have Wψ,φ1=W1/ψφ1,φ1W_{\psi,\varphi}^{-1}=W_{1/\psi\circ\varphi^{-1},\varphi^{-1}} and

Wψ,φ1=supvTμ(v)μ(φ1(v))|1ψ(φ1(v))|=supvTμ(φ(v))μ(v)|1ψ(v)|.\|W_{\psi,\varphi}^{-1}\|=\sup_{v\in T}\frac{\mu(v)}{\mu(\varphi^{-1}(v))}\left\lvert\frac{1}{\psi(\varphi^{-1}(v))}\right\rvert=\sup_{v\in T}\frac{\mu(\varphi(v))}{\mu(v)}\left\lvert\frac{1}{\psi(v)}\right\rvert.
Proof.

Suppose Wψ,φW_{\psi,\varphi} has a bounded inverse. We know φ\varphi is surjective by Theorem 5.1. Next assume there is a vTv\in T with ψ(v)=0\psi(v)=0. Then

Wψ,φKv=ψ(v)Kφ(v)=0,W_{\psi,\varphi}^{*}K_{v}=\psi(v)K_{\varphi(v)}=0,

where Wψ,φW_{\psi,\varphi}^{*} is the adjoint on the dual space of LμL_{\mu}^{\infty}. However, this cannot happen since Wψ,φW_{\psi,\varphi}^{*} is also invertible. Thus ψ(v)0\psi(v)\neq 0 for all vTv\in T. To show φ\varphi is injective, assume v,wTv,w\in T with φ(v)=φ(w)\varphi(v)=\varphi(w). Then

Wψ,φKv=ψ(v)Kφ(v)=ψ(v)ψ(w)ψ(w)Kφ(w)=ψ(v)ψ(w)Wψ,φKw.W_{\psi,\varphi}^{*}K_{v}=\psi(v)K_{\varphi(v)}=\frac{\psi(v)}{\psi(w)}\psi(w)K_{\varphi(w)}=\frac{\psi(v)}{\psi(w)}W_{\psi,\varphi}^{*}K_{w}.

Again using the fact that Wψ,φW_{\psi,\varphi}^{*} is invertible, we have Kv=(ψ(v)/ψ(w))KwK_{v}=(\psi(v)/\psi(w))K_{w}, but this can only happen if v=wv=w by Lemma 2.4. We conclude that φ\varphi is injective and hence bijective. This conclusion together with the observation that an invertible operator is bounded below and Theorem 5.2 provides the desired infimum condition.

Conversely, consider the weighted composition operator W1/ψφ1,φ1W_{1/\psi\circ\varphi^{-1},\varphi^{-1}}. The symbols of this operator are defined by our hypotheses on ψ\psi and φ\varphi, and

supvTμ(v)μ(φ1(v))|1ψ(φ1(v))|=supvTμ(φ(v))μ(v)|1ψ(v)|<\sup_{v\in T}\frac{\mu(v)}{\mu(\varphi^{-1}(v))}\left\lvert\frac{1}{\psi(\varphi^{-1}(v))}\right\rvert=\sup_{v\in T}\frac{\mu(\varphi(v))}{\mu(v)}\left\lvert\frac{1}{\psi(v)}\right\rvert<\infty

by the infimum condition. It follows that W1/ψφ1,φ1W_{1/\psi\circ\varphi^{-1},\varphi^{-1}} is bounded by Theorem 3.2, and thus Wψ,φW_{\psi,\varphi} has a bounded inverse. ∎

We now focus on characterizing the isometric weighted composition operators acting on LμL_{\mu}^{\infty}. The characteristic functions give insight into the necessary interplay between φ\varphi and ψ\psi to induce an isometry.

Theorem 6.2.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded. Then Wψ,φW_{\psi,\varphi} is an isometry on LμL_{\mu}^{\infty} if and only if φ\varphi is surjective and supvSwμ(v)μ(φ(v))|ψ(v)|=1\sup_{v\in S_{w}}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=1 for all wTw\in T. Moreover, Wψ,φW_{\psi,\varphi} is a surjective isometry on LμL_{\mu}^{\infty} if and only if φ\varphi is a bijection and μ(v)μ(φ(v))|ψ(v)|=1\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=1 for all vTv\in T.

Proof.

We first prove the characterization of the isometric weighted composition operators on LμL_{\mu}^{\infty}. Suppose Wψ,φW_{\psi,\varphi} is an isometry on LμL_{\mu}^{\infty}. Then Wψ,φW_{\psi,\varphi} is injective, and thus φ\varphi is surjective by Theorem 5.1. Fix wTw\in T and consider the function f(v)=1μ(v)χφ(w)(v)f(v)=\frac{1}{\mu(v)}\mbox{\Large$\chi$}_{\varphi(w)}(v). Since Wψ,φW_{\psi,\varphi} is an isometry on LμL_{\mu}^{\infty}, it follows that

1=fμ=Wψ,φfμ=supvTμ(v)μ(φ(v))|ψ(v)|χφ(w)(φ(v))=supvSwμ(v)μ(φ(v))|ψ(v)|.1=\|f\|_{\mu}=\|W_{\psi,\varphi}f\|_{\mu}=\sup_{v\in T}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mbox{\Large$\chi$}_{\varphi(w)}(\varphi(v))=\sup_{v\in S_{w}}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert.

Conversely, suppose φ\varphi is surjective and supvSwμ(v)μ(φ(v))|ψ(v)|=1\sup_{v\in S_{w}}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=1 for all wTw\in T. Observe that for each vTv\in T, μ(v)μ(φ(v))|ψ(v)|1\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\leq 1 since vSvv\in S_{v}. Let fLμf\in L_{\mu}^{\infty}. It follows from Lemma 2.1 that

Wψ,φfμ=supvTμ(v)|ψ(v)||f(φ(v))|supvTμ(v)μ(φ(v))|ψ(v)|fμfμ.\|W_{\psi,\varphi}f\|_{\mu}=\sup_{v\in T}\mu(v)\left\lvert\psi(v)\right\rvert\left\lvert f(\varphi(v))\right\rvert\leq\sup_{v\in T}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\|f\|_{\mu}\leq\|f\|_{\mu}.

To verify the reverse inequality, fix wTw\in T and choose 0<ε<10<\varepsilon<1. Then there exists vUεSwv\in U_{\varepsilon}\cap S_{w}. Observe

εμ(φ(w))|f(φ(w))|\displaystyle\varepsilon\mu(\varphi(w))\left\lvert f(\varphi(w))\right\rvert =εμ(φ(v))|f(φ(v))|\displaystyle=\varepsilon\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert
μ(v)μ(φ(v))|ψ(v)|μ(φ(v))|f(φ(v))|\displaystyle\leq\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\mu(\varphi(v))\left\lvert f(\varphi(v))\right\rvert
=μ(v)|ψ(v)||f(φ(v))|\displaystyle=\mu(v)\left\lvert\psi(v)\right\rvert\left\lvert f(\varphi(v))\right\rvert
Wψ,φfμ.\displaystyle\leq\|W_{\psi,\varphi}f\|_{\mu}.

Taking the supremum over all wTw\in T, and letting ε\varepsilon go to 1, we have fμWψ,φfμ\|f\|_{\mu}\leq\|W_{\psi,\varphi}f\|_{\mu}. Thus, Wψ,φW_{\psi,\varphi} is an isometry on LμL_{\mu}^{\infty}.

We complete the proof by characterizing the surjective isometric weighted composition operators on LμL_{\mu}^{\infty}. Suppose Wψ,φW_{\psi,\varphi} is a surjective isometry. Then Wψ,φW_{\psi,\varphi} has bounded inverse and it follows from Theorem 6.1 that φ\varphi is bijective. Thus Sw={w}S_{w}=\{w\} for every wTw\in T and

μ(w)μ(φ(w))|ψ(w)|=supvSwμ(v)μ(φ(v))|ψ(v)|=1\frac{\mu(w)}{\mu(\varphi(w))}\left\lvert\psi(w)\right\rvert=\sup_{v\in S_{w}}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=1

for every wTw\in T.

Finally, suppose φ\varphi is a bijection and μ(v)μ(φ(v))|ψ(v)|=1\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=1 for all vTv\in T. Then Wψ,φW_{\psi,\varphi} is an isometry. It follows from Theorem 6.1 that Wψ,φW_{\psi,\varphi} is invertible, and thus surjective. ∎

We complete this section by considering the results applied to the composition and multiplication operators acting on LμL_{\mu}^{\infty}.

Corollary 6.3.

Suppose ψ\psi is a function on TT and φ\varphi a self-map of TT for which both CφC_{\varphi} and MψM_{\psi} are bounded on LμL_{\mu}^{\infty}.

  1. (a)

    Then CφC_{\varphi} has a bounded inverse if and only if φ\varphi is bijective and

    infvTμ(v)μ(φ(v))>0.\inf_{v\in T}\frac{\mu(v)}{\mu(\varphi(v))}>0.

    In this case, we have

    Cφ1=Cφ1=supvTμ(v)μ(φ1(v))=supvTμ(φ(v))μ(v).\|C_{\varphi}^{-1}\|=\|C_{\varphi^{-1}}\|=\sup_{v\in T}\frac{\mu(v)}{\mu(\varphi^{-1}(v))}=\sup_{v\in T}\frac{\mu(\varphi(v))}{\mu(v)}.
  2. (b)

    Then MψM_{\psi} has a bounded inverse if and only if infvT|ψ(v)|>0\inf_{v\in T}\left\lvert\psi(v)\right\rvert>0. In this case, we have

    Mψ1=M1/ψ=1/ψ.\|M_{\psi}^{-1}\|=\|M_{1/\psi}\|=\|1/\psi\|_{\infty}.

The following characterization of the isometric composition operators on LμL_{\mu}^{\infty} completes the work of the authors in [4], where only partial results were obtained for LμL_{\mu}^{\infty}. The characterization of the isometric multiplication operators on LμL_{\mu}^{\infty} agrees with [3, Theorem 3.6], while providing the additional conclusion that all such isometries are in fact surjective.

Corollary 6.4.

Suppose ψ\psi is a function on TT and φ\varphi a self-map of TT for which both CφC_{\varphi} and MψM_{\psi} are bounded on LμL_{\mu}^{\infty}.

  1. (a)

    The operator CφC_{\varphi} is an isometry on LμL_{\mu}^{\infty} if and only if φ\varphi is a surjective and supvSwμ(v)μ(φ(v))=1\sup_{v\in S_{w}}\frac{\mu(v)}{\mu(\varphi(v))}=1 for all wTw\in T.

  2. (b)

    The operator CφC_{\varphi} is a surjective isometry on LμL_{\mu}^{\infty} if and only if φ\varphi is a bijection and μ(v)μ(φ(v))=1\frac{\mu(v)}{\mu(\varphi(v))}=1 for all vTv\in T.

  3. (c)

    For the multiplication operator MψM_{\psi}, the following are equivalent:

    1. i.

      MψM_{\psi} is an isometry on LμL_{\mu}^{\infty},

    2. ii.

      MψM_{\psi} is a surjective isometry on LμL_{\mu}^{\infty},

    3. iii.

      |ψ(v)|=1\left\lvert\psi(v)\right\rvert=1 for all vTv\in T.

7. Fredholm Weighted Composition Operators

Recall a linear operator AA between Banach spaces is Fredholm if AA has closed range and both ker(A)\ker(A) and ker(A)\ker(A^{*}) are finite dimensional. In fact, the condition of closed range is redundant, since this follows from the dimension of the cokernel being finite. However, this condition typically remains to mirror the definition of Fredholm operators on a Hilbert space. Alternatively, AA is Fredholm if there exists a bounded operator SS such that SAISA-I and ASIAS-I are both compact. This is sometimes referred to as Atkinson’s Theorem. Every invertible operator is Fredholm. The converse is not true, but an operator that is Fredholm must be invertible “modulo the compacts”. Thus a compact operator can not be Fredholm. For a general reference on Fredholm operators see [11, Section XI.2] or [16, Section 5.8].

To classify the Fredholm weighted composition operators, we begin with a sequence of useful lemmas.

Lemma 7.1.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}. If Wψ,φW_{\psi,\varphi} is Fredholm on LμL_{\mu}^{\infty}, then ψ\psi can have at most finitely many zeros.

Proof.

First, we show Kwker(Wψ,φ)K_{w}\in\ker(W_{\psi,\varphi}^{*}) whenever ψ(w)=0\psi(w)=0. Suppose wTw\in T with ψ(w)=0\psi(w)=0 and let fLμf\in L_{\mu}^{\infty}. Then

(Wψ,φKwf)(v)=Kw(ψ(v)f(φ(v)))=ψ(w)f(φ(w))=0.(W_{\psi,\varphi}^{*}K_{w}f)(v)=K_{w}(\psi(v)f(\varphi(v)))=\psi(w)f(\varphi(w))=0.

Since ff was arbitrary, this implies Wψ,φKwW_{\psi,\varphi}^{*}K_{w} is the zero functional and thus Kwker(Wψ,φ)K_{w}\in\ker(W_{\psi,\varphi}^{*}).

If ψ\psi has infinitely many zeros {vi}i=1\{v_{i}\}_{i=1}^{\infty}, then {Kvi}i=1ker(Wψ,φ).\{K_{v_{i}}\}_{i=1}^{\infty}\subseteq\textup{ker}(W_{\psi,\varphi}^{*}). From Lemma 2.4, the set {Kvi}\{K_{v_{i}}\} is linearly independent and thus dim(ker(Wψ,φ))=.\dim(\ker(W_{\psi,\varphi}^{*}))=\infty. However, since Wψ,φW_{\psi,\varphi} is Fredholm, dim(ker(Wψ,φ))<\dim(\ker(W_{\psi,\varphi}^{*}))<\infty. This is a contradiction and the result follows. ∎

Lemma 7.2.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT. If φ\varphi has finite range and Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}, then Wψ,φW_{\psi,\varphi} cannot be Fredholm.

Proof.

This follows from the fact that such a weighted composition operator is compact, and hence cannot be Fredholm. ∎

Lemma 7.3.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}. If Wψ,φW_{\psi,\varphi} is Fredholm on LμL_{\mu}^{\infty}, then there is an NN\in\mathbb{N} such that φ1(w)\varphi^{-1}(w) contains at most NN points for every wφ(T)w\in\varphi(T).

Proof.

First, suppose there exist points {v1,,v2m}\{v_{1},\dots,v_{2m}\} in TT such that φ(v1)==φ(v2m)\varphi(v_{1})=\cdots=\varphi(v_{2m}) and ψ(vi)0\psi(v_{i})\neq 0 for 1i2m1\leq i\leq 2m. For 1jm1\leq j\leq m, define kj=1ψ(v2j)Kv2j1ψ(v2j1)Kv2j1.k_{j}=\frac{1}{\psi(v_{2j})}K_{v_{2j}}-\frac{1}{\psi(v_{2j-1})}K_{v_{2j-1}}. It follows that {k1,,km}ker(Wψ,φ)\{k_{1},\dots,k_{m}\}\subseteq\ker(W_{\psi,\varphi}^{*}).

Now, if Wψ,φW_{\psi,\varphi} is Fredholm and the condition of the lemma does not hold, then for every nn there is a wnφ(T)w_{n}\in\varphi(T) such that φ1(wn)\varphi^{-1}(w_{n}) contains at least nn elements. Furthermore, ψ\psi has at most finitely many zeros by Lemma 7.1, say MM, and thus for nn sufficiently large φ1(wn)\varphi^{-1}(w_{n}) contains at least nM>0n-M>0 points where ψ\psi does not vanish. Letting nn tend to infinity, the first part of the proof implies dim(ker(Wψ,φ))=\dim(\ker(W_{\psi,\varphi}^{*}))=\infty. However this contradicts the fact that Wψ,φW_{\psi,\varphi} is Fredholm. ∎

Lemma 7.4.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}. If Wψ,φW_{\psi,\varphi} is Fredholm on LμL_{\mu}^{\infty}, then φ1(w)\varphi^{-1}(w) contains exactly one element for all but a finite number of points wφ(T)w\in\varphi(T).

Proof.

Suppose Wψ,φW_{\psi,\varphi} is Fredholm and define

K={wφ(T):φ1(w) contains more than one element}.K=\{w\in\varphi(T):\varphi^{-1}(w)\textup{ contains more than one element}\}.

Assume to the contrary that KK is an infinite set. From Lemma 7.1 it follows that Z=ψ1(0)Z=\psi^{-1}(0) is finite. Thus, there is an infinite subset K1KK_{1}\subseteq K such that for every wK1w\in K_{1}, there exists two distinct points v1,v2φ1(w)v_{1},v_{2}\in\varphi^{-1}(w) for which ψ(v1)0\psi(v_{1})\neq 0 and ψ(v2)0\psi(v_{2})\neq 0. Define kw=1ψ(v1)Kv11ψ(v2)Kv2k_{w}=\frac{1}{\psi(v_{1})}K_{v_{1}}-\frac{1}{\psi(v_{2})}K_{v_{2}} and let S={kw:wK1}S=\{k_{w}:w\in K_{1}\}. Note SS is infinite and linearly independent. A computation similar to the one above shows Sker(Wψ,φ).S\subseteq\ker(W_{\psi,\varphi}^{*}). Again, this contradicts the fact that Wψ,φW_{\psi,\varphi} is Fredholm and the conclusion follows. ∎

Lemma 7.5.

Let ψ\psi be a function on TT and φ\varphi a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}. If Wψ,φW_{\psi,\varphi} is Fredholm on LμL_{\mu}^{\infty}, then Tφ(T)T\setminus\varphi(T) must be finite.

Proof.

Assume Tφ(T)T\setminus\varphi(T) is infinite. First notice {χw:wTφ(T)}\{\mbox{\Large$\chi$}_{w}:w\in T\setminus\varphi(T)\} is linearly independent in LμL_{\mu}^{\infty}. Also, for wTφ(T)w\in T\setminus\varphi(T), we have

(Wψ,φχw)(v)=ψ(v)χw(φ(v))=0.(W_{\psi,\varphi}\mbox{\Large$\chi$}_{w})(v)=\psi(v)\mbox{\Large$\chi$}_{w}(\varphi(v))=0.

Thus {χw:wTφ(T)}ker(Wψ,φ)\{\mbox{\Large$\chi$}_{w}:w\in T\setminus\varphi(T)\}\subseteq\ker(W_{\psi,\varphi}). However, this contradicts the fact that dim(ker(Wψ,φ))<\dim(\ker(W_{\psi,\varphi}))<\infty. ∎

The last lemma we need is derived from Theorems 3.2 and 6.1.

Lemma 7.6.

Let XX and YY be unbounded subsets of TT. Suppose ψ\psi is a function on TT and φ\varphi a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on Lμ(T)L_{\mu}^{\infty}(T). If φ:XY\varphi:X\to Y, then Wψ,φ:Lμ(Y)Lμ(X)W_{\psi,\varphi}:L_{\mu}^{\infty}(Y)\to L_{\mu}^{\infty}(X) is bounded and satisfies

Wψ,φ=supvXμ(v)μ(φ(v))|ψ(v)|.\|W_{\psi,\varphi}\|=\sup_{v\in X}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert.

Moreover, if φ\varphi is bijective and infvXμ(v)μ(φ(v))|ψ(v)|>0,\inf_{v\in X}\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert>0, then Wψ,φW_{\psi,\varphi} has bounded inverse with

Wψ,φ1=supvYμ(v)μ(φ1(v))|1ψ(φ1(v))|=supvXμ(φ(v))μ(v)|1ψ(v)|.\|W_{\psi,\varphi}^{-1}\|=\sup_{v\in Y}\;\frac{\mu(v)}{\mu(\varphi^{-1}(v))}\left\lvert\frac{1}{\psi(\varphi^{-1}(v))}\right\rvert=\sup_{v\in X}\frac{\mu(\varphi(v))}{\mu(v)}\left\lvert\frac{1}{\psi(v)}\right\rvert.

Combining the previous lemmas leads to our Fredholm characterization. For the proof here, recall the notation

Sw\displaystyle S_{w} ={vT:φ(v)=φ(w)}\displaystyle=\{v\in T:\varphi(v)=\varphi(w)\}
Uε\displaystyle U_{\varepsilon} ={vT:μ(v)μ(φ(v))|ψ(v)|ε}.\displaystyle=\left\{v\in T:\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\geq\varepsilon\right\}.
Theorem 7.7.

Let ψ\psi be a function on TT and φ\varphi be a self-map of TT for which Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}. Then Wψ,φW_{\psi,\varphi} is Fredholm if and only if

  1. (a)

    Tφ(T)T\setminus\varphi(T) is finite,

  2. (b)

    there exists MM\in\mathbb{N} such that φ1(w)\varphi^{-1}(w) contains at most MM points for every wφ(T)w\in\varphi(T),

  3. (c)

    φ1(w)\varphi^{-1}(w) contains exactly one element for all but a finite number of points wφ(T)w\in\varphi(T),

  4. (d)

    Z={vT:ψ(v)=0}Z=\{v\in T:\psi(v)=0\} is finite,

  5. (e)

    there is an ε>0\varepsilon>0 such that UεSwU_{\varepsilon}\cap S_{w}\neq\emptyset for every wZcw\in Z^{c}.

Proof.

First, suppose Wψ,φW_{\psi,\varphi} is Fredholm. Then properties (a) through (e) follow directly from Lemmas 7.5, 7.3, 7.4, 7.1, and Theorem 5.3 (since Fredholm implies closed range).

Now, suppose conditions (a) through (e) hold. To prove Wψ,φW_{\psi,\varphi} is Fredholm, we define the following sets

𝒮\displaystyle\mathcal{S} ={wφ(T):|φ1(w)|=1}\displaystyle=\{w\in\varphi(T):\left\lvert\varphi^{-1}(w)\right\rvert=1\}
\displaystyle\mathcal{F} ={wφ(T):1<|φ1(w)|M}.\displaystyle=\{w\in\varphi(T):1<\left\lvert\varphi^{-1}(w)\right\rvert\leq M\}.

Note φ(T)=𝒮\varphi(T)=\mathcal{S}\cup\mathcal{F} from condition (b). Also, by condition (c), \mathcal{F} is a finite set, which we enumerate as ={w1,,wm}\mathcal{F}=\{w_{1},\dots,w_{m}\}. For each 1im1\leq i\leq m, we denote viv_{i} to be a fixed element in the set φ1(wi)\varphi^{-1}(w_{i}).

Next, define the function η:TT\eta:T\to T by

η(w)={φ1(w)if wSviif wwif wφ(T)\eta(w)=\begin{cases}\varphi^{-1}(w)&\text{if $w\in S$}\\ v_{i}&\text{if $w\in\mathcal{F}$}\\ w&\text{if $w\not\in\varphi(T)$}\end{cases}

and the function τ:T\tau:T\to\mathbb{C} by

τ(w)={1/ψ(v)if vZc1if vZ.\tau(w)=\begin{cases}1/\psi(v)&\text{if $v\in Z^{c}$}\\ 1&\text{if $v\in Z$}.\\ \end{cases}

Note that by properties (a) through (c), the set {vT:η(v)Z}\{v\in T:\eta(v)\in Z\} is finite by construction since ZZ is finite.

We will now show Wτη,ηW_{\tau\circ\eta,\eta} to be bounded as an operator on LμL_{\mu}^{\infty}. First, define S1=𝒮φ(Zc)S_{1}=\mathcal{S}\cap\varphi(Z^{c}) and T1=φ1(S1)T_{1}=\varphi^{-1}(S_{1}). Then, as a mapping, φ:T1S1\varphi:T_{1}\to S_{1} is bijective. Also, by condition (c), S1S_{1} is infinite and hence unbounded; it follows then that T1T_{1} is also unbounded. Restricting η\eta to S1S_{1}, we have η=φ1\eta=\varphi^{-1} and τη=1/ψφ1\tau\circ\eta=1/\psi\circ\varphi^{-1}. By Lemma 7.6 and condition (e), Wψ,φW_{\psi,\varphi} has a bounded inverse W1/ψφ1,φ1W_{1/\psi\circ\varphi^{-1},\varphi^{-1}} as an operator from Lμ(S1)L_{\mu}^{\infty}(S_{1}) to Lμ(T1)L_{\mu}^{\infty}(T_{1}). But this inverse is Wτη,ηW_{\tau\circ\eta,\eta}. As TS1=𝒮c(Tφ(T))φ(Z)T\setminus S_{1}=\mathcal{S}^{c}\cup(T\setminus\varphi(T))\cup\varphi(Z) is the union of finite sets by conditions (a), (c), and (d), and thus is a finite set, Wτη,ηW_{\tau\circ\eta,\eta} extends to a bounded operator on Lμ(T)L_{\mu}^{\infty}(T).

To show Wψ,φW_{\psi,\varphi} is Fredholm, we will show Wψ,φWτη,ηIW_{\psi,\varphi}W_{\tau\circ\eta,\eta}-I and Wτη,ηWψ,φIW_{\tau\circ\eta,\eta}W_{\psi,\varphi}-I are both compact. Observe that

φ(η(v))={vif vφ(T)φ(v)if vφ(T).\varphi(\eta(v))=\begin{cases}v&\text{if $v\in\varphi(T)$}\\ \varphi(v)&\text{if $v\not\in\varphi(T)$}.\end{cases}

and for fLμf\in L_{\mu}^{\infty} and vTv\in T,

(Wτη,ηWψ,φf)(v)={f(v)if vφ(T) and η(v)Zcf(φ(v))if vφ(T) and η(v)Zc0if η(v)Z.(W_{\tau\circ\eta,\eta}W_{\psi,\varphi}f)(v)=\begin{cases}f(v)&\text{if $v\in\varphi(T)$ and $\eta(v)\in Z^{c}$}\\ f(\varphi(v))&\text{if $v\notin\varphi(T)$ and $\eta(v)\in Z^{c}$}\\ 0&\text{if $\eta(v)\in Z$}.\end{cases}

So

((Wτη,ηWψ,φI)f)(v)=wφ(T)η(w)Zc(f(φ(w))f(w))χw(v)wTη(w)Zf(w)χw(v).((W_{\tau\circ\eta,\eta}W_{\psi,\varphi}-I)f)(v)=\sum_{\begin{subarray}{c}w\notin\varphi(T)\\ \eta(w)\in Z^{c}\end{subarray}}(f(\varphi(w))-f(w))\mbox{\Large$\chi$}_{w}(v)-\sum_{\begin{subarray}{c}w\in T\\ \eta(w)\in Z\end{subarray}}f(w)\mbox{\Large$\chi$}_{w}(v).

As these are finite sums, the operator Wτη,ηWψ,φIW_{\tau\circ\eta,\eta}W_{\psi,\varphi}-I is finite-rank, and thus compact. Likewise,

η(φ(v))={vif φ(v)𝒮viif φ(v)\eta(\varphi(v))=\begin{cases}v&\text{if $\varphi(v)\in\mathcal{S}$}\\ v_{i}&\text{if $\varphi(v)\in\mathcal{F}$}\end{cases}

and for fLμf\in L_{\mu}^{\infty} and vTv\in T

(Wψ,φWτη,ηf)(v)={f(v)if φ(v)Sφ(Zc)ψ(v)τ(vi)f(vi)if φ(v)Fφ(Zc)0if φ(v)φ(Z).(W_{\psi,\varphi}W_{\tau\circ\eta,\eta}f)(v)=\begin{cases}f(v)&\text{if $\varphi(v)\in S\cap\varphi(Z^{c})$}\\ \psi(v)\tau(v_{i})f(v_{i})&\text{if $\varphi(v)\in F\cap\varphi(Z^{c})$}\\ 0&\text{if $\varphi(v)\in\varphi(Z)$}.\end{cases}

So Wψ,φWτη,ηIW_{\psi,\varphi}W_{\tau\circ\eta,\eta}-I is compact since

((Wψ,φWτη,ηI)f)(v)=\displaystyle((W_{\psi,\varphi}W_{\tau\circ\eta,\eta}-I)f)(v)=
wTφ(w)φ(Zc)(ψ(w)τ(vi)f(vi)f(w))χw(v)wTφ(w)φ(Z)f(w)χw(v).\displaystyle\qquad\sum_{\begin{subarray}{c}w\in T\\ \varphi(w)\in\mathcal{F}\cap\varphi(Z^{c})\end{subarray}}(\psi(w)\tau(v_{i})f(v_{i})-f(w))\mbox{\Large$\chi$}_{w}(v)-\sum_{\begin{subarray}{c}w\in T\\ \varphi(w)\in\varphi(Z)\end{subarray}}f(w)\mbox{\Large$\chi$}_{w}(v).

Therefore Wψ,φW_{\psi,\varphi} is Fredholm. ∎

In the case when φ\varphi is a bijection on TT, we see that the Fredholm condition is almost the same as that for bounded below.

Corollary 7.8.

Let ψ\psi be a function on TT and φ\varphi be a bijective self-map of TT and assume Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}. Then Wψ,φW_{\psi,\varphi} is Fredholm if and only if Wψ,φW_{\psi,\varphi} is bounded below and ψ\psi has finitely many zeros.

For composition operators we have the following. Recall the notation

Vε={vT:μ(v)μ(φ(v))ε}.V_{\varepsilon}=\left\{v\in T:\frac{\mu(v)}{\mu(\varphi(v))}\geq\varepsilon\right\}.
Corollary 7.9.

Let φ\varphi be a self-map of TT for which CφC_{\varphi} is bounded on LμL_{\mu}^{\infty}. Then CφC_{\varphi} is Fredholm if and only if

  1. (a)

    Tφ(T)T\setminus\varphi(T) is finite,

  2. (b)

    there exists MM\in\mathbb{N} such that φ1(w)\varphi^{-1}(w) contains at most NN points for every wφ(T)w\in\varphi(T),

  3. (c)

    φ1(w)\varphi^{-1}(w) contains exactly one element for all but a finite number of points wφ(T)w\in\varphi(T),

  4. (d)

    there is an ε>0\varepsilon>0 such that VεSwV_{\varepsilon}\cap S_{w}\neq\emptyset for every wTw\in T.

In addition to the characterization above, for composition operators we have an interesting sufficient condition for an operator to be Fredholm.

Proposition 7.1.

Let φ\varphi be self-map of TT for which CφC_{\varphi} is bounded on LμL_{\mu}^{\infty}. If there is a self-map η\eta of TT such that φ(v)=η(v)\varphi(v)=\eta(v) except for a finite number of points in TT and CηC_{\eta} is invertible (with bounded inverse), then CφC_{\varphi} is Fredholm.

Proof.

First observe that CηC_{\eta} is bounded on LμL_{\mu}^{\infty} since CφC_{\varphi} is bounded. The fact that CηC_{\eta} is invertible implies η\eta is surjective by Theorem 5.1. Furthermore, CηC_{\eta}^{*} is also invertible. If v,wTv,w\in T with η(v)=η(w)\eta(v)=\eta(w), it must be the case that Kη(v)=Kη(w)K_{\eta(v)}=K_{\eta(w)} or CηKv=CηKwC_{\eta}^{*}K_{v}=C_{\eta}^{*}K_{w} and thus Kv=KwK_{v}=K_{w} or v=wv=w. Thus η\eta is injective and hence invertible. It is easy to check that Cη1=Cη1C_{\eta}^{-1}=C_{\eta^{-1}}.

Let R={v1,v2,,vn}R=\{v_{1},v_{2},\ldots,v_{n}\} be the set of points where φ\varphi and η\eta do not agree. We now claim that Im(CφCη1I)\textup{Im}(C_{\varphi}C_{\eta}^{-1}-I) and Im(Cη1CφI)\textup{Im}(C_{\eta}^{-1}C_{\varphi}-I) are both finite dimensional. This in turn implies that both operators are finite rank and hence compact. We verify these claims from which the conclusion is apparent.

For CφCη1I=CφCη1IC_{\varphi}C_{\eta}^{-1}-I=C_{\varphi}C_{\eta^{-1}}-I and vTv\in T, we have ((CφCη1I)f)(v)=f(η1(φ(v)))f(v)((C_{\varphi}C_{\eta^{-1}}-I)f)(v)=f(\eta^{-1}(\varphi(v)))-f(v), which will be zero for vRv\not\in R. Thus we can write

((CφCη1I)f)(v)=viR(f(η1(φ(vi)))f(vi))χvi(v).((C_{\varphi}C_{\eta^{-1}}-I)f)(v)=\sum_{v_{i}\in R}(f(\eta^{-1}(\varphi(v_{i})))-f(v_{i}))\mbox{\Large$\chi$}_{v_{i}}(v).

Thus Im(CφCη1I){ciχvi:ci,viR}\textup{Im}(C_{\varphi}C_{\eta}^{-1}-I)\subseteq\left\{\sum c_{i}\mbox{\Large$\chi$}_{v_{i}}:c_{i}\in\mathbb{C},v_{i}\in R\right\}, which is finite dimensional.

Similarly, ((Cη1CφI)f)(v)=f(φ(η1(v)))f(v)((C_{\eta^{-1}}C_{\varphi}-I)f)(v)=f(\varphi(\eta^{-1}(v)))-f(v), which will be zero if η1(v)R\eta^{-1}(v)\not\in R. If η1(v)R\eta^{-1}(v)\in R, then η1(v)=vi\eta^{-1}(v)=v_{i} for some ii and thus, in this case, we have

((Cη1CφI)f)(v)=viR(f(φ(vi))f(η(vi)))χη(vi)(v).((C_{\eta^{-1}}C_{\varphi}-I)f)(v)=\sum_{v_{i}\in R}(f(\varphi(v_{i}))-f(\eta(v_{i})))\mbox{\Large$\chi$}_{\eta(v_{i})}(v).

We conclude Im(Cη1CφI){ciχη(vi):ci,viR}\textup{Im}(C_{\eta}^{-1}C_{\varphi}-I)\subseteq\left\{\sum c_{i}\mbox{\Large$\chi$}_{\eta(v_{i})}:c_{i}\in\mathbb{C},v_{i}\in R\right\}. ∎

For multiplication operators, we immediately see the following.

Corollary 7.10.

Let ψ\psi be a function on TT for which MψM_{\psi} is bounded on LμL_{\mu}^{\infty}. The following are equivalent:

  1. (i)

    MψM_{\psi} is Fredholm,

  2. (ii)

    Z={vT:ψ(v)=0}Z=\{v\in T:\psi(v)=0\} is finite and infvZc|ψ(v)|>0\inf_{v\in Z^{c}}\left\lvert\psi(v)\right\rvert>0,

  3. (iii)

    there exists ε>0\varepsilon>0 and NN\in\mathbb{N} such that |ψ(v)|ε\left\lvert\psi(v)\right\rvert\geq\varepsilon for all vTv\in T with |v|>N\left\lvert v\right\rvert>N.

Note condition (ii) is derived from Theorem 7.7. In addition, condition (iii), while easily shown to be equivalent to (ii), is a simpler condition to use for actually determining if MψM_{\psi} is Fredholm on LμL_{\mu}^{\infty}.

8. Examples

In this section, we construct several examples that illustrate the richness of the operator theory as well as several key features of the results throughout this paper. Specifically, when not indicated, TT will be an infinite tree with root oo, where d\mathrm{d} is the edge-counting metric on TT, as defined in any of [1, 3, 4, 9]. For the first example, we construct a weighted composition operator that is bounded on LμL_{\mu}^{\infty} but not bounded on Lμ0L_{\mu}^{0}, thus showing the converse of Lemma 3.5 does not hold.

Example 8.1.

Let μ\mu be a weight function and φ\varphi a self-map of TT with finite range. Define ψ(v)=1/μ(v)\psi(v)=1/\mu(v) for all vTv\in T, m=minwφ(T)ψ(w)m=\min_{w\in\varphi(T)}\psi(w), and M=maxwφ(T)ψ(w)M=\max_{w\in\varphi(T)}\psi(w). Note 0<mM<0<m\leq M<\infty and

μ(v)μ(φ(v))|ψ(v)|=ψ(φ(v))\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=\psi(\varphi(v))

for all vTv\in T. Thus σψ,φ=M\sigma_{\psi,\varphi}=M. So Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} by Theorem 3.2. However, since ψ(φ(v))\psi(\varphi(v)) is bounded away from zero on TT, it follows that ξψ,φ\xi_{\psi,\varphi} can not equal 0. Thus Wψ,φW_{\psi,\varphi} is not bounded on Lμ0L_{\mu}^{0} by Theorem 3.4.

In the next three examples, we construct bounded and compact weighted composition operators on LμL_{\mu}^{\infty} for which the induced multiplication or composition operators are not bounded or compact.

Example 8.2.

In this example, we construct a bounded weighted composition operators on LμL_{\mu}^{\infty} for which the induced composition operator is bounded but the induced multiplication operator is unbounded. We specifically provide separate examples for which μ\mu is typical and atypical.

  1. (i)

    Define

    μ(v)={1/|v|if vo1if v=o,\mu(v)=\begin{cases}1/\left\lvert v\right\rvert&\text{if $v\neq o$}\\ 1&\text{if $v=o$},\end{cases}

    ψ(v)=1/μ(v)\psi(v)=1/\mu(v) and φ(v)=o\varphi(v)=o for all vTv\in T. Since ψ\psi is not a bounded function on TT, MψM_{\psi} is not bounded on LμL_{\mu}^{\infty} [3, Theorem 3.1]. Additionally, CφC_{\varphi} is bounded (it is in fact compact) [4, Theorem 3.1] since

    μ(v)μ(φ(v))=1|v|\frac{\mu(v)}{\mu(\varphi(v))}=\frac{1}{\left\lvert v\right\rvert}

    for all vTv\in T^{*}. However, Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} since

    μ(v)μ(φ(v))|ψ(v)|=1\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=1

    for all vTv\in T.

  2. (ii)

    Define

    μ(v)={|v|if vo1if v=o,\mu(v)=\begin{cases}\left\lvert v\right\rvert&\text{if $v\neq o$}\\ 1&\text{if $v=o$},\end{cases}

    and ψ(v)=μ(v)\psi(v)=\mu(v) for all vTv\in T. Let (wn)(w_{n}) be a sequence in TT for which |wn|=n2\left\lvert w_{n}\right\rvert=n^{2} for all n{0}n\in\mathbb{N}\cup\{0\} and define φ(v)=w|v|\varphi(v)=w_{\left\lvert v\right\rvert} for all vTv\in T. For the same reasoning as in (i), MψM_{\psi} is not bounded and CφC_{\varphi} is bounded on LμL_{\mu}^{\infty}, and Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty}.

Example 8.3.

In this example, we construct a compact weighted composition operator on LμL_{\mu}^{\infty} for which the induced multiplication operator is compact but the induced composition operator is not bounded. We provide specific examples for which μ\mu is typical and atypical.

  1. (i)

    Define

    μ(v)={1/|v|if vo1if v=o,\mu(v)=\begin{cases}1/\left\lvert v\right\rvert&\text{if $v\neq o$}\\ 1&\text{if $v=o$},\end{cases}

    and ψ(v)=μ3(v)\psi(v)=\mu^{3}(v) for all vTv\in T. Let (wn)(w_{n}) be a sequence in TT for which |wn|=n2\left\lvert w_{n}\right\rvert=n^{2} for all n{0}n\in\mathbb{N}\cup\{0\} and define φ(v)=w|v|\varphi(v)=w_{\left\lvert v\right\rvert} for all vTv\in T. Observe MψM_{\psi} is compact on LμL_{\mu}^{\infty} [3, Theorem 3.2] since μ3(v)0\mu^{3}(v)\to 0 as |v|\left\lvert v\right\rvert\to\infty. Also note CφC_{\varphi} is not bounded on LμL_{\mu}^{\infty} since

    μ(v)μ(φ(v))=|v|\frac{\mu(v)}{\mu(\varphi(v))}=\left\lvert v\right\rvert\to\infty

    as |v|\left\lvert v\right\rvert\to\infty. However, Wψ,φW_{\psi,\varphi} is compact on LμL_{\mu}^{\infty} by Corollary 4.5 since

    sup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|=1N.\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=\frac{1}{N}.
  2. (ii)

    Define

    μ(v)={|v|2if vo1if v=o,\mu(v)=\begin{cases}\left\lvert v\right\rvert^{2}&\text{if $v\neq o$}\\ 1&\text{if $v=o$},\end{cases}

    and ψ(v)=1/μ(v)\psi(v)=1/\mu(v) for all vTv\in T. Let (wn)(w_{n}) be a sequence in TT for which |wn|=n\left\lvert w_{n}\right\rvert=n for all n{0}n\in\mathbb{N}\cup\{0\} and define φ(v)=w|v|\varphi(v)=w_{\left\lvert v\right\rvert} for all vTv\in T. For the same reasoning as in (i), MψM_{\psi} is compact and CφC_{\varphi} is not bounded on LμL_{\mu}^{\infty}, and Wψ,φW_{\psi,\varphi} is compact on LμL_{\mu}^{\infty}.

Example 8.4.

In this example, we construct a compact weighted composition operator on LμL_{\mu}^{\infty} for which neither induced multiplication or composition operators is compact on LμL_{\mu}^{\infty}. We provide examples for which μ\mu is both typical and atypical.

  1. (i)

    Define

    μ(v)={1/|v|if vo1if v=o,\mu(v)=\begin{cases}1/\left\lvert v\right\rvert&\text{if $v\neq o$}\\ 1&\text{if $v=o$},\end{cases}

    and

    ψ(v)={1if |v| is odd1/(|v|+1)if |v| is even.\psi(v)=\begin{cases}1&\text{if $\left\lvert v\right\rvert$ is odd}\\ 1/(\left\lvert v\right\rvert+1)&\text{if $\left\lvert v\right\rvert$ is even}.\end{cases}

    Let (wn)(w_{n}) be a sequence in TT for which |wn|=n\left\lvert w_{n}\right\rvert=\lfloor\sqrt{n}\rfloor for all nn\in\mathbb{N} and define

    φ(v)={w|v|if |v| is oddvif |v| is even.\varphi(v)=\begin{cases}w_{\left\lvert v\right\rvert}&\text{if $\left\lvert v\right\rvert$ is odd}\\ v&\text{if $\left\lvert v\right\rvert$ is even}.\end{cases}

    Observe MψM_{\psi} and CφC_{\varphi} are both bounded on LμL_{\mu}^{\infty}, but neither is compact. However, Wψ,φW_{\psi,\varphi} is compact on LμL_{\mu}^{\infty} since

    sup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|1N.\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert\leq\frac{1}{N}.
  2. (ii)

    Define

    μ(v)={|v|if vo1if v=o,\mu(v)=\begin{cases}\left\lvert v\right\rvert&\text{if $v\neq o$}\\ 1&\text{if $v=o$},\end{cases}

    and

    ψ(v)={1if |v| is odd1/(|v|+1)if |v| is even.\psi(v)=\begin{cases}1&\text{if $\left\lvert v\right\rvert$ is odd}\\ 1/(\left\lvert v\right\rvert+1)&\text{if $\left\lvert v\right\rvert$ is even}.\end{cases}

    Let (wn)(w_{n}) be a sequence in TT for which |wn|=n(n+1)\left\lvert w_{n}\right\rvert=n(n+1) for all nn\in\mathbb{N} and define

    φ(v)={w|v|if |v| is oddvif |v| is even.\varphi(v)=\begin{cases}w_{\left\lvert v\right\rvert}&\text{if $\left\lvert v\right\rvert$ is odd}\\ v&\text{if $\left\lvert v\right\rvert$ is even}.\end{cases}

    Observe MψM_{\psi} and CφC_{\varphi} are both bounded on LμL_{\mu}^{\infty}, but neither is compact. However, Wψ,φW_{\psi,\varphi} is compact on LμL_{\mu}^{\infty} since

    sup|φ(v)|Nμ(v)μ(φ(v))|ψ(v)|=1N+1.\sup_{\left\lvert\varphi(v)\right\rvert\geq N}\;\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=\frac{1}{N+1}.

In the next example, we see that composition operators on LμL_{\mu}^{\infty} induced by bijections do not necessarily have inverses that are bounded in LμL_{\mu}^{\infty}.

Example 8.5.

In this example, we take TT to be \mathbb{Z} with root 0. Define the weight μ\mu and φ\varphi on TT by

μ(v)={1if v0|v|if v<0\mu(v)=\begin{cases}1&\text{if $v\geq 0$}\\ |v|&\text{if $v<0$}\end{cases}

and

φ(v)={0if v=0(v+1)/2if v>0 and oddvif v>0 and even2v+1if v<0.\varphi(v)=\begin{cases}0&\text{if $v=0$}\\ (v+1)/2&\text{if $v>0$ and odd}\\ -v&\text{if $v>0$ and even}\\ 2v+1&\text{if $v<0$}.\end{cases}

By direct calculation,

μ(v)μ(φ(v))={1if v=0, or v>0 and odd1/|v|if v>0 and even|v|/(2|v|+1)if v<0.\frac{\mu(v)}{\mu(\varphi(v))}=\begin{cases}1&\text{if $v=0$, or $v>0$ and odd}\\ 1/|v|&\text{if $v>0$ and even}\\ |v|/(2|v|+1)&\text{if $v<0$}.\end{cases}

As μ(v)μ(φ(v))1\frac{\mu(v)}{\mu(\varphi(v))}\leq 1 for all vTv\in T, CφC_{\varphi} is bounded. Note φ\varphi is a bijection, and thus Cφ1C_{\varphi^{-1}} is well defined as an operator on LμL_{\mu}^{\infty}. However, we see that Cφ1C_{\varphi^{-1}} is not bounded on LμL_{\mu}^{\infty} because, if it were the case, then supvTμ(v)μ(φ1(v))\sup_{v\in T}\frac{\mu(v)}{\mu(\varphi^{-1}(v))} would be finite, which is equivalent to supvTμ(φ(v))μ(v)\sup_{v\in T}\frac{\mu(\varphi(v))}{\mu(v)} being finite. However, this is not true since for the sequence vn=2nv_{n}=2n in TT, we have

limnμ(φ(vn))μ(vn)=limn|vn|=limn2n=.\lim_{n\to\infty}\frac{\mu(\varphi(v_{n}))}{\mu(v_{n})}=\lim_{n\to\infty}|v_{n}|=\lim_{n\to\infty}2n=\infty.

Fredholm composition and weighted composition operators acting on classical spaces of analytic functions over the unit disk typically arise from automorphic symbols; in other words, in most of the cases where Fredholm composition operators have been characterized, they are in fact invertible (see [15] and [14]). Here we give a simple example to show this is not the case for our spaces. The example also illustrates Proposition 7.1.

Example 8.6.

Let μ\mu be a weight on TT. For a fixed wTw\in T^{*} define

φ(v)={vif vowif v=o.\varphi(v)=\begin{cases}v&\text{if $v\neq o$}\\ w&\text{if $v=o$}.\end{cases}

Also take η(v)=v\eta(v)=v for all vTv\in T. It follows that both CφC_{\varphi} and CηC_{\eta} are bounded on LμL_{\mu}^{\infty} and CφCηI=CηCφI=CφI.C_{\varphi}C_{\eta}-I=C_{\eta}C_{\varphi}-I=C_{\varphi}-I. Moreover, ((CφI)f)(v)=0((C_{\varphi}-I)f)(v)=0 if vov\neq o and ((CφI)f)(o)=f(v1)f(o)((C_{\varphi}-I)f)(o)=f(v_{1})-f(o), which means Im(CφI)={cχo(v):c}\textup{Im}(C_{\varphi}-I)=\{c\mbox{\Large$\chi$}_{o}(v):c\in\mathbb{C}\}. Thus CφIC_{\varphi}-I has finite rank and is compact. Hence CφC_{\varphi} is Fredholm.

In the final example, we construct a surjective isometric weighted composition operator (and thus Fredholm) on LμL_{\mu}^{\infty} whose composition component is not bounded.

Example 8.7.

For this example, we take TT to be [i]\mathbb{Z}[i], the points in \mathbb{C} with integer real and imaginary parts, with root o=0o=0. In TT we define the quadrants as follows:

I\displaystyle\mathrm{I} ={reiθ[i]:r>0, 0θ<π/2},\displaystyle=\left\{re^{i\theta}\in\mathbb{Z}[i]:r>0,\;0\leq\theta<\pi/2\right\},
II\displaystyle\mathrm{II} ={reiθ[i]:r>0,π/2θ<π},\displaystyle=\left\{re^{i\theta}\in\mathbb{Z}[i]:r>0,\;\pi/2\leq\theta<\pi\right\},
III\displaystyle\mathrm{III} ={reiθ[i]:r>0,πθ<3π/2},\displaystyle=\left\{re^{i\theta}\in\mathbb{Z}[i]:r>0,\;\pi\leq\theta<3\pi/2\right\},
IV\displaystyle\mathrm{IV} ={reiθ[i]:r>0, 3π/2θ<2π}.\displaystyle=\left\{re^{i\theta}\in\mathbb{Z}[i]:r>0,\;3\pi/2\leq\theta<2\pi\right\}.

Thus, T={0}IIIIIIIVT=\{0\}\cup\mathrm{I}\cup\mathrm{II}\cup\mathrm{III}\cup\mathrm{IV}. On TT, define the weight μ\mu by

μ(v)={1if vI{0}|v|if vII or IV|v|2if vIII.\mu(v)=\begin{cases}1&\text{if $v\in\mathrm{I}\cup\{0\}$}\\ \left\lvert v\right\rvert&\text{if $v\in\mathrm{II}$ or $\mathrm{IV}$}\\ \left\lvert v\right\rvert^{2}&\text{if $v\in\mathrm{III}$}.\end{cases}

Define φ:TT\varphi:T\to T to be rotation by π/2\pi/2, i.e. φ(v)=eiπ/2v\varphi(v)=e^{i\pi/2}v for all vTv\in T. Thus φ\varphi is a bijection with the root as the only fixed point. We see that CφC_{\varphi} is not bounded on LμL_{\mu}^{\infty} since for any sequence (vn)(v_{n}) in III\mathrm{III} with |vn|\left\lvert v_{n}\right\rvert\to\infty as nn\to\infty, we have

limnμ(vn)μ(φ(vn))=lim|v||v|2|v|=.\lim_{n\to\infty}\frac{\mu(v_{n})}{\mu(\varphi(v_{n}))}=\lim_{\left\lvert v\right\rvert\to\infty}\frac{\left\lvert v\right\rvert^{2}}{\left\lvert v\right\rvert}=\infty.

Finally, define ψ:T\psi:T\to\mathbb{C} by

ψ(v)={|v|if vI or II1/|v|if vIII or IV1if v=0.\psi(v)=\begin{cases}\left\lvert v\right\rvert&\text{if $v\in\mathrm{I}$ or $\mathrm{II}$}\\ 1/\left\lvert v\right\rvert&\text{if $v\in\mathrm{III}$ or $\mathrm{IV}$}\\ 1&\text{if $v=0$}.\end{cases}

First, observe Wψ,φW_{\psi,\varphi} is bounded on LμL_{\mu}^{\infty} since

μ(v)μ(φ(v))|ψ(v)|=1\frac{\mu(v)}{\mu(\varphi(v))}\left\lvert\psi(v)\right\rvert=1

for all vTv\in T. By Theorem 6.2, Wψ,φW_{\psi,\varphi} is a surjective isometry. So Wψ,φW_{\psi,\varphi} is invertible, and thus Fredholm.

Acknowledgements

The authors would like to thank Ruben Martínez-Avendaño of the Instituto Tecnológico Autónomo de México for the idea to generalize the results to unbounded, locally finite metric spaces.

References

  • [1] Robert F. Allen, Flavia Colonna, and Glenn R. Easley, Composition operators on the Lipschitz space of a tree, Mediterr. J. Math. 11 (2014), no. 1, 97–108. MR 3160615
  • [2] Robert F. Allen, Flavia Colonna, Rubén A. Martínez-Avendaño, and Matthew A. Pons, Hypercyclicity of composition operators on discrete weighted Banach spaces, Mediterr. J. Math. 16 (2019), no. 5, Art. 115, 20. MR 3994861
  • [3] Robert F. Allen and Isaac M. Craig, Multiplication operators on weighted Banach spaces of a tree, Bull. Korean Math. Soc. 54 (2017), no. 3, 747–761. MR 3659146
  • [4] Robert F. Allen and Matthew A. Pons, Composition operators on weighted Banach spaces of a tree, Bull. Malays. Math. Sci. Soc. 41 (2018), no. 4, 1805–1818. MR 3854493
  • [5] Stefan Banach, Théorie des opérations linéaires, Chelsea Publishing Co., New York, 1955. MR 0071726
  • [6] José Bonet, Mikael Lindström, and Elke Wolf, Isometric weighted composition operators on weighted Banach spaces of type HH^{\infty}, Proc. Amer. Math. Soc. 136 (2008), no. 12, 4267–4273. MR 2431039
  • [7] Paul S. Bourdon, Invertible weighted composition operators, Proc. Amer. Math. Soc. 142 (2014), no. 1, 289–299. MR 3119203
  • [8] Joseph A. Cima and Warren R. Wogen, On isometries of the Bloch space, Illinois J. Math. 24 (1980), no. 2, 313–316. MR 575069
  • [9] Flavia Colonna and Glenn R. Easley, Multiplication operators on the Lipschitz space of a tree, Integral Equations Operator Theory 68 (2010), no. 3, 391–411. MR 2735443
  • [10] Manuel D. Contreras and Alfredo G. Hernández-Díaz, Weighted composition operators in weighted Banach spaces of analytic functions, J. Austral. Math. Soc. Ser. A 69 (2000), no. 1, 41–60. MR 1767392
  • [11] John B. Conway, A course in functional analysis, second ed., Graduate Texts in Mathematics, vol. 96, Springer-Verlag, New York, 1990. MR 1070713
  • [12] Mohamad El-Gebeily and John Wolfe, Isometries of the disc algebra, Proc. Amer. Math. Soc. 93 (1985), no. 4, 697–702. MR 776205
  • [13] Clinton J. Kolaski, Isometries of weighted Bergman spaces, Canadian J. Math. 34 (1982), no. 4, 910–915. MR 672684
  • [14] Ching-On Lo and Anthony Wai-Keung Loh, Fredholm weighted composition operators, Oper. Matrices 13 (2019), no. 1, 169–186. MR 3924378
  • [15] Barbara D. MacCluer, Fredholm composition operators, Proc. Amer. Math. Soc. 125 (1997), no. 1, 163–166. MR 1371134
  • [16] by same author, Elementary functional analysis, Graduate Texts in Mathematics, vol. 253, Springer, New York, 2009. MR 2462971
  • [17] Alfonso Montes-Rodríguez, Weighted composition operators on weighted Banach spaces of analytic functions, J. London Math. Soc. (2) 61 (2000), no. 3, 872–884. MR 1766111
  • [18] Perumal Muthukumar and Saminathan Ponnusamy, Composition operators on the discrete analogue of generalized Hardy space on homogenous trees, Bull. Malays. Math. Sci. Soc. 40 (2017), no. 4, 1801–1815. MR 3712587
  • [19] by same author, Discrete analogue of generalized Hardy spaces and multiplication operators on homogenous trees, Anal. Math. Phys. 7 (2017), no. 3, 267–283. MR 3683009