Composition and multiplication operators between Orlicz function spaces

Tadeusz Chawziuk; Yunan Cui; Yousef Estaremi; Henryk Hudzik; Radosław Kaczmarek

doi:10.1186/s13660-016-0972-9

Research
Open Access

Composition and multiplication operators between Orlicz function spaces

Tadeusz Chawziuk¹,
Yunan Cui²Email author,
Yousef Estaremi³,
Henryk Hudzik¹ and
Radosław Kaczmarek¹

Journal of Inequalities and Applications20162016:52

https://doi.org/10.1186/s13660-016-0972-9

Received: 11 August 2015
Accepted: 14 January 2016
Published: 11 February 2016

Abstract

Composition operators and multiplication operators between two Orlicz function spaces are investigated. First, necessary and sufficient conditions for their continuity are presented in several forms. It is shown that, in general, the Radon-Nikodým derivative $\frac{d(\mu\circ\tau^{-1})}{d\mu}(s)$ need not belong to $L^{\infty}(\Omega)$ to guarantee the continuity of the composition operator $c_{\tau}x(t)=x(\tau(t))$ from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$. Next, the problem of compactness of these operators is considered. We apply a compactness criterion in Orlicz spaces which involves compactness with respect to the topology of local convergence in measure and equi-absolute continuity in norm of all the elements of the set under consideration. In connection with this, we state some sufficient conditions for equi-absolute continuity of the composition operator $c_{\tau}$ and the multiplication operator $M_{w}$ from one Orlicz space into another. Also the problem of necessary conditions is discussed.

Keywords

composition operator
multiplication operator
Orlicz spaces

MSC

47B33
46E30

1 Introduction

Since the early 1930s composition operators have been a subject of study of many mathematicians or physicists. At the beginning they were used to solve problems in mathematical physics and classical mechanics [1, 2], or to study ergodic transformations [3, 4]. Up until now many Ph.D. theses have been defended (for instance: Boyd [5], Gupta [6], Ridge [7], Schwartz [8], Singh [9], Swanton [10], Veluchamy [11]), numerous books published [12, 13], and innumerable papers printed on the composition operator or the weighted composition operator in various function spaces, e.g., $L^{p}$ spaces ([13–23], and others), Orlicz spaces ([24–27], and others), Musielak-Orlicz spaces [28, 29], Musielak-Orlicz spaces of Bochner type ([30] or [31]), Orlicz-Lorentz spaces [32–37], Hilbert spaces [38–40] and many other types of spaces (for instance: [41–43]). The multiplication operator has also been a subject of research of many mathematicians (see for instance: [44–49]). For more details as regards the historical background we refer the reader to [13].

Let $(\Omega,\Sigma,\mu)$ be a non-atomic, σ-finite and complete measure space and let $\tau:\Omega\rightarrow\Omega$ be a measurable function, i.e., a mapping such that $\tau^{-1}(A)\in \Sigma$ if and only if $A\in\Sigma$ for any $A\subset\Omega$, where $\tau^{-1}(A)$ is the counterimage of A. In the whole paper we will assume that τ is non-singular, that is, $\mu(\tau^{-1}(A))=0$ provided $\mu(A)=0$. The last assumption guarantees that the measure $\mu\circ\tau^{-1}$ defined for any $A\in\Sigma$ by the formula

$$\mu\circ\tau^{-1}(A)=\mu\bigl(\tau^{-1}(A)\bigr) $$

is absolutely continuous with respect to the measure μ (what is usually denoted by $\mu\circ\tau^{-1}\ll\mu$). Then the Radon-Nikodým theorem implies the existence of a non-negative locally integrable function $h_{\tau}$ on Ω such that $\mu\circ\tau^{-1}(A)=\int _{A} h_{\tau}(s)\,d\mu(s)$ for any $A\in\Sigma$. The function $h_{\tau}(s)=\frac{d(\mu\circ\tau^{-1})}{d\mu}(s)$ is called the Radon-Nikodým derivative of the measure $\mu\circ \tau^{-1}$ with respect to the measure μ. Let us remark that even if the Radon-Nikodým derivative is unbounded, the corresponding composition operator acting from an Orlicz space onto itself can still be continuous (see [50]).

Let $L^{0}(\Omega)=L^{0}(\Omega,\Sigma,\mu)$ be the space of all (abstract classes of) Σ-measurable functions from Ω into $\mathbb {R}$ with respect to the equivalence relation: $x\sim y$ if and only if $x(t)=y(t)$ for μ-a.e. $t\in\Omega$.

With the help of a non-singular and measurable mapping $\tau:\Omega \rightarrow\Omega$ one defines on $L^{0}$ the composition operator

$$(c_{\tau}x ) (t):=x\bigl(\tau(t)\bigr) $$

for any $t\in\Omega$ and any $x\in L^{0}(\Omega)$.

Let $w \in L^{0} (\Omega, \Sigma,\mu)$ be a strictly positive function. We define the multiplication operator $M_{w}: L^{0} \rightarrow L^{0}$ by the formula

$$(M_{w} x ) (t):=w(t)x(t) $$

for any $t\in\Omega$ and any $x\in L^{0}(\Omega)$.

It is obvious that $c_{\tau}x\in L^{0}(\Omega)$ and $M_{w} x \in L^{0}(\Omega )$ if $x\in L^{0}(\Omega)$.

Remark 1.1

We do not assume, if not specifically stated otherwise, that the mapping τ is a surjection, i.e., $\tau(\Omega)=\Omega$.

A function $\Phi:\mathbb{R}\rightarrow\mathbb{R}_{+}=[0,\infty)$ is said to be an Orlicz function if Φ is convex, even, continuous, vanishing only at 0.

The complementary function in the sense of Young to an Orlicz function Φ is defined to be the function $\Phi^{*}:[0,\infty)\rightarrow [0,\infty]$ such that $\Phi^{*}(u)=\sup_{v>0} \{uv-\Phi(v)\}$.

A function φ from $\Omega\times\mathbb{R}$ into $\mathbb{R}_{+}$ such that $\varphi(t,\cdot)$ is an Orlicz function for μ-a.e. $t\in \Omega$ and $\varphi(\cdot, u)$ is a Σ-measurable function for every $u\in\mathbb{R}$ is called a generalized Orlicz function or a Musielak-Orlicz function. The Musielak-Orlicz space $L^{\varphi}= L^{\varphi}(\Omega,\Sigma,\mu)$ is the space of all (equivalence classes of) Σ-measurable functions $x:\Omega\rightarrow\mathbb{R}$ such that

$$I_{\varphi}(\lambda x)= \int_{\Omega}\varphi\bigl(t,\lambda x(t)\bigr)\,d\mu< \infty $$

for some $\lambda>0$ depending on x. The Musielak-Orlicz space equipped with the Luxemburg norm

$$\|x\|_{\varphi}=\inf\biggl\{ \lambda>0:I_{\varphi}\biggl( \frac{x}{\lambda } \biggr)\leq1 \biggr\} $$

is a Banach space (cf. [51, 52], and in the case of Orlicz spaces also [53–55]). It is obvious that Orlicz functions are Musielak-Orlicz functions, and consequently, Orlicz spaces are Musielak-Orlicz spaces. For instance, an Orlicz weighted space $L^{\Phi}_{h}(\Omega)$ is the Musielak-Orlicz space $L^{\varphi}(\Omega)$ generated by $\varphi(t,u)=\Phi(u)h(t)$ for any $t\in\Omega$ and any $u\in \mathbb{R}$.

Throughout the paper, we will make use of Ishii’s theorem from [56].

Theorem 1.1

For Musielak-Orlicz spaces $L^{\varphi}(\Omega)$ and $L^{\psi}(\Omega)$ over a non-atomic measure space $\Omega=(\Omega,\Sigma,\mu)$, the inclusion $L^{\varphi}(\Omega)\subset L^{\psi}(\Omega)$ holds if and only if there exist $k,K>0$ and $c(\cdot)\in L^{1}(\Omega)$ such that

$$\psi(t,k\xi)\leq K\varphi(t,\xi)+c(t) $$

for all $\xi\geq0$ and a.e. $t \in\Omega$.

For any $A\in\Sigma$, by $I_{\Phi}(x,A)$ we mean the value of the modular $I_{\Phi}$ at x in the Orlicz space $L^{\Phi}(A)$ generated by the Orlicz function Φ over the measure space $(A,\Sigma\cap A,\mu|_{A})$. In the case when $A=\Omega$, we will write $I_{\Phi}(x)$ instead of $I_{\Phi}(x,\Omega)$.

2 Continuity of the composition operator $c_{\tau}$ from $L^{\Phi}$ into $L^{\Psi}$ and from $L^{\Phi}$ onto $L^{\Psi}$

We are interested in finding necessary and sufficient conditions for the continuity of the composition operator $c_{\tau}$ from the Orlicz space $L^{\Phi}(\Omega)=L^{\Phi}(\Omega,\Sigma,\mu)$ equipped with the Luxemburg norm into the Orlicz space $L^{\Psi}(\Omega)=L^{\Psi}(\Omega ,\Sigma,\mu)$ endowed with the corresponding Luxemburg norm. The following fact will be very helpful.

Fact 2.1

For an arbitrary function $x\in L^{0}(\Omega)$, we have $c_{\tau}x\in L^{\Psi}(\Omega)$ if and only if $x\in L^{\Psi}_{h}(\tau(\Omega))$, where $L^{\Psi}_{h}(\tau(\Omega))=L^{\Psi}_{h}(\tau(\Omega),\Sigma\cap\tau(\Omega), \mu|_{\Sigma\cap\tau(\Omega)})$ is a weighted Orlicz space with the weight function $h(s)=\frac{d\mu\circ\tau^{-1}}{d\mu}(s)$.

Proof

For any $x\in L^{0}(\Omega)$, we have

$$\begin{aligned} I_{\Psi}(c_{\tau}x,\Omega) =& \int_{\Omega}\Psi\bigl(c_{\tau}x(t)\bigr)\,d\mu(t) \\ =& \int_{\Omega}\Psi\bigl(x\bigl(\tau(t)\bigr)\bigr)\,d\mu(t) \\ =& \int_{\tau(\Omega)} \Psi\bigl(x(s)\bigr)\,d\mu\circ\tau^{-1}(s) \\ =& \int_{\tau(\Omega)} \Psi\bigl(x(s)\bigr)h(s)\,d\mu(s) \\ =& I_{\Psi,h}\bigl(x,\tau(\Omega)\bigr). \end{aligned}$$

□

Theorem 2.1

If the quadruple Φ, Ψ, h, τ satisfies the condition

$$ \underset{K>1}{\exists}\ \underset{\substack{A\in\Sigma\cap \tau( \Omega) \\ \mu(A)=0}}{\exists}\ \underset{g\in L^{1}_{+}(\tau(\Omega))}{ \exists}\ \underset{s\in\tau(\Omega)\backslash A}{\forall}\ \underset {u\geq0}{ \forall} \Psi(u)h(s)\leq\Phi(Ku)+g(s), $$

(1)

or, equivalently, $L^{\Phi}(\tau(\Omega))\subset L^{\Psi}_{h}(\tau(\Omega))$, then the composition operator $c_{\tau}$ acts continuously from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$.

Moreover, if $\mu(\Omega\backslash\tau(\Omega))=0$, then condition (1) is necessary for the continuity of the composition operator $c_{\tau}$ from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$.

Proof

We will show that if condition (1) is satisfied then $c_{\tau}x\in L^{\Psi}(\Omega)$ whenever $x\in L^{\Phi}(\Omega)$, i.e., $x\in L^{\Psi}_{h}(\tau(\Omega))$ whenever $x\in L^{\Phi}(\Omega)$ (see Fact 2.1).

Assume that $x\in L^{\Phi}(\Omega)$. Applying condition (1) and Fact 2.1, we obtain

$$\begin{aligned} I_{\Psi}\biggl(\frac{c_{\tau}x}{K(1+\|g\|_{L^{1}(\tau(\Omega))})\|x\|_{\Phi}},\Omega\biggr) \leq& \frac{1}{1+\|g\|_{L^{1}(\tau(\Omega))}}I_{\Psi}\biggl(\frac{c_{\tau}x}{K\| x\|_{\Phi}},\Omega\biggr) \\ =& \frac{1}{1+\|g\|_{L^{1}(\tau(\Omega))}}I_{\Psi,h} \biggl(\frac{x}{K\| x\| _{\Phi}},\tau(\Omega) \biggr) \\ \leq& \frac{I_{\Phi}(\frac{x}{\|x\|_{\Phi}},\tau(\Omega) )+\| g\|_{L^{1}(\tau(\Omega))}}{1+\|g\|_{L^{1}(\tau(\Omega))}} \\ \leq& \frac{1}{1+\|g\|_{L^{1}(\tau(\Omega))}}\bigl(1+\|g\|_{L^{1}(\tau (\Omega))}\bigr)=1, \end{aligned}$$

which shows that $c_{\tau}$ acts from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$ and

$$\|c_{\tau}x\|_{\Psi}\leq K\bigl(1+\|g\|_{L^{1}(\tau(\Omega))}\bigr)\|x \|_{\Phi}, $$

which finishes the proof of the first part of the theorem.

Now assume that $\mu(\Omega\backslash\tau(\Omega))=0$. If the inclusion in the assumption of the theorem fails to hold, then there exists a function x belonging to $L^{\Phi}(\tau(\Omega))=L^{\Phi}(\Omega)$ but not belonging to $L^{\Psi}_{h}(\tau(\Omega))$. In virtue of Fact 2.1, we obtain $x\in L^{\Phi}(\Omega)$ and, simultaneously, $c_{\tau}x \notin L^{\Psi}(\Omega)$, hence $c_{\tau}$ does not even act from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$. □

The preceding theorem can be formulated in a different language, which in some situations might be more useful.

Theorem 2.2

The composition operator $c_{\tau}: L^{\Phi}(\Omega)\rightarrow L^{\Psi}(\Omega)$ is continuous if the following simple condition is satisfied:

$$ \int_{\tau(\Omega)}\chi\bigl(h(s)\bigr)\,d\mu(s)< \infty, $$

(2)

where $h=\frac{d\mu\circ\tau^{-1}}{d\mu}$ and χ is the function complementary in the sense of Young to the function $\Phi\circ K\Psi ^{-1}$, with K being the constant from condition (1) of Theorem 2.1. If $\mu(\Omega\backslash\tau(\Omega))=0$, then condition (2) is necessary for the continuity of $c_{\tau}$.

Proof

It is not too difficult to see that Φ, Ψ, and h satisfy condition (1) if and only if

$$ \sup_{u\geq0} \bigl[\Psi(u)h(s)-\Phi(Ku)\bigr]\in L^{1}_{+}\bigl(\tau(\Omega)\bigr). $$

But

$$\begin{aligned} \sup_{u\geq0} \bigl[\Psi(u)h(s)-\Phi(Ku)\bigr] =& \sup _{v\geq0} \bigl[v h(s)-\Phi\bigl(K\Psi^{-1}(v)\bigr) \bigr] \\ =&\chi\bigl(h(s)\bigr). \end{aligned}$$

□

Remark 2.1

Notice that if $b(\chi):=\sup\{u\geq0\colon\chi(u)<\infty\}<\infty$ then condition (2) implies that $\Vert h\Vert _{L^{\infty}(\tau(\Omega))}\leq b(\chi)<\infty$, that is, the Radon-Nikodým derivative $h=\frac{d\mu\circ\tau^{-1}}{\,}d\mu$ is essentially bounded. Moreover, it is easy to see that the integral (2) can be finite for some $h\notin L^{\infty}(\tau(\Omega))$ if and only if the function χ has only finite values (for the case when $\Phi=\Psi$ see [50]; the proof in the case when $\Phi\neq\Psi$ is similar).

The next theorem states a necessary and sufficient condition in order that χ is such a function.

Theorem 2.3

The function $\chi=(\Phi\circ K\Psi^{-1})^{*}$, with $K>1$, assumes only finite values (i.e., $b(\chi)=\infty$) if and only if $\liminf_{t\rightarrow\infty}\frac{\Phi(Kt)}{\Psi(t)}=\infty$.

Proof

Sufficiency. Let $\liminf_{t\rightarrow\infty}\frac{\Phi (Kt)}{\Psi(t)}=\infty$. Then $\lim_{t\rightarrow\infty}\frac{\Phi (Kt)}{\Psi(t)}=\infty$ and so $\lim_{t\rightarrow\infty}\frac {\Phi(K\Psi^{-1}(t))}{t}=\infty$. Take an arbitrary $v>0$. In virtue of the last equality, there exists $u_{v}>0$ such that for all $u\geq u_{v}$ the inequality

$$ \frac{\Phi(K\Psi^{-1}(u))}{u}\geq v $$

holds. Hence

$$\begin{aligned} \chi(v):=\sup_{u\geq0} \bigl\{ uv-\Phi\bigl(K\Psi^{-1}(u) \bigr) \bigr\} =&\sup_{u\geq0} \biggl\{ u \biggl(v-\frac{\Phi(K\Psi^{-1}(u))}{u} \biggr) \biggr\} \\ =&\sup_{u\in[0,u_{v}]} \bigl\{ uv-\Phi\bigl(K\Psi^{-1}(u) \bigr) \bigr\} < \infty \end{aligned}$$

as a supremum of a continuous function on a compact interval.

Necessity. Assume that $\liminf_{t\rightarrow\infty}\frac{\Phi (Kt)}{\Psi(t)}<\infty$ for $K>1$. Then $\liminf_{t\rightarrow \infty}\frac{\Phi(K\Psi^{-1}(t))}{t}<\infty$ for $K>1$, and so there exist $c>0$ and a sequence of positive numbers $(u_{n} )_{n=1}^{\infty}$ such that $u_{n}\rightarrow\infty$ as $n\rightarrow\infty $ and $\lim_{n\rightarrow\infty}\frac{\Phi(K\Psi ^{-1}(u_{n}))}{u_{n}}=c$. Consequently, $c^{\prime}\in(c,\infty)$ can be found such that for $n\in\mathbb{N}$ large enough we have

$$ \Phi\bigl(K\bigl(\Psi^{-1}(u_{n})\bigr)\bigr)\leq c^{\prime}u_{n}. $$

Therefore, taking $v>c^{\prime}$, we get

$$u_{n}v-\Phi\bigl(K\Psi^{-1}(u_{n})\bigr)\geq u_{n}v-c^{\prime}u_{n}=u_{n} \bigl(v-c^{\prime}\bigr) $$

for $n\in\mathbb{N}$ large enough, whence

$$\begin{aligned} \sup_{u\geq0} \bigl\{ uv-\Phi\bigl(K\Psi^{-1}(u)\bigr) \bigr\} \geq& \sup_{n\in\mathbb{N}} \bigl\{ u_{n}v-\Phi\bigl(K \Psi^{-1}(u_{n})\bigr) \bigr\} \\ \geq& \bigl(v-c^{\prime}\bigr)\sup_{n\in\mathbb{N}} u_{n}=\infty, \end{aligned}$$

which finishes the proof of the theorem. □

Now we show that if the function χ from Theorem 2.2 assumes only finite values, i.e., $b(\chi)=\infty$, then it may happen that the composition operator $c_{\tau}$ from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega )$ is continuous despite the fact that $h=\frac{d\mu\circ\tau^{-1}}{d\mu }\notin L^{\infty}(\tau(\Omega))$.

Example 2.1

Let $\Omega=(0,1]$, $(\Omega,\Sigma,\mu)$ be the Lebesgue measure space and $A_{n}=(\frac{1}{n+1},\frac{1}{n}]$ for every $n\in\mathbb {N}$. Then $\bigcup_{n=1}^{\infty} A_{n}=\Omega$. Let χ be the function from Theorem 2.2, let $b(\chi)=\infty$ and $u_{n}>0$ be such that $\chi(u_{n})=\sqrt{n}$ for every $n\in\mathbb{N}$. Since $u_{n}\nearrow\infty$ as $n\rightarrow\infty$, there exists $m\in \mathbb{N}$ such that $u_{n}\geq1$ for any $n>m$. Define $\tau :(0,1]\rightarrow(0,1]$ by the formula

$$\tau(t)= \textstyle\begin{cases} t, &\mbox{for }t\in A_{n}\mbox{ with }n\leq m,\\ \frac{t}{u_{n}}, &\mbox{for }t\in A_{n},\mbox{ where }n>m. \end{cases} $$

Let us denote $v_{n}=1$ if $n\leq m$ and $v_{n}=u_{n}$ if $n>m$. Then $\tau ^{-1}:\tau(\Omega)\rightarrow\Omega$ is defined by the formula $\tau ^{-1}(s)=v_{n} s$ for any $s\in\tau(A_{n})$. Consequently, for any $A\in \Sigma\cap\tau(\Omega)$, we have

$$\begin{aligned} \mu\circ\tau^{-1}(A) :=&\mu\bigl(\tau^{-1}(A)\bigr)=\mu\Biggl( \bigcup_{n=1}^{\infty}\tau^{-1}\bigl(A\cap\tau(A_{n})\bigr)\Biggr) \\ =&\sum_{n=1}^{\infty}\mu\bigl(\tau^{-1}\bigl(A\cap\tau (A_{n})\bigr)\bigr) \\ =&\sum_{n=1}^{\infty}\mu\biggl(v_{n}\biggl(A\cap \frac{1}{v_{n}}(A_{n})\biggr)\biggr) \\ =&\sum_{n=1}^{\infty}\mu(v_{n} A\cap A_{n}). \end{aligned}$$

(3)

Let us define

$$ h(s)=\sum_{n=1}^{\infty}v_{n}\mathbb{1}_{\frac{1}{u_{n}}A_{n}}(s). $$

(4)

Then, for any $A\in\Sigma\cap\tau(\Omega)$,

$$\begin{aligned} \int_{A} h(s)\,d\mu(s) =&\int_{\bigcup_{n=1}^{\infty}A\cap\tau(A_{n})} h(s)\,d\mu(s)= \sum_{n=1}^{\infty}\int_{A\cap\frac{1}{v_{n}}(A_{n})} v_{n} \,d\mu(s) \\ =& \sum_{n=1}^{\infty}v_{n} \mu\biggl(A\cap\frac {1}{v_{n}}A_{n}\biggr)= \sum_{n=1}^{\infty}\mu(v_{n} A\cap A_{n}). \end{aligned}$$

(5)

By inequalities (3) and (5), we get

$$\mu\circ\tau^{-1}(A)=\int_{A} h(s)\,d\mu(s), \quad\forall A\in\Sigma \cap\tau(\Omega), $$

which means that $h=\frac{d(\mu\circ\tau^{-1})}{d\mu}$. By formula (4) and the definition of $v_{n}$, we have

$$\begin{aligned} \int_{\tau(\Omega)}\chi\bigl(h(s)\bigr) =& \sum_{n=1}^{\infty}\chi(v_{n}) \mu\biggl(\frac{1}{v_{n}}A_{n}\biggr)\\ =& \sum_{n=1}^{m}\mu(A_{n})+ \sum_{n=m+1}^{\infty}\sqrt{n}\mu\biggl(\frac{1}{v_{n}}A_{n}\biggr)\\ \leq&1+\sum_{n=m+1}^{\infty}\sqrt{n} \mu(A_{n})\\ \leq&1+\sum_{n=m+1}^{\infty}\frac{\sqrt{n}}{n(n+1)}\\ < &1+\sum_{n=1}^{\infty}\frac{1}{n^{3\slash 2}}< \infty. \end{aligned}$$

In virtue of Theorem 2.2, we conclude that the composition operator $c_{\tau}$ from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$ is continuous. However, since $u_{n}\rightarrow\infty$ as $n\rightarrow\infty $, we have $\|h\|_{L^{\infty}(\tau(\Omega))}=\infty$.

Theorem 2.4

The composition operator $c_{\tau}$ acts continuously from $L^{\Phi}(\Omega , \Sigma,\mu)$ onto $L^{\Psi}(\Omega, \Sigma,\mu)$ if and only if $\mu(\Omega\backslash\tau(\Omega))=0$ and the following two conditions are jointly satisfied:

(i)

$\exists_{K>1} \mathop{\exists_{A\in\Sigma\cap \Omega}}\limits_{\mu(A)=0} \exists_{g\in L^{1}_{+}(\Omega)} \forall_{s\in\Omega\backslash A} \forall_{u\geq0} \Psi(u)h(s)\leq\Phi(Ku)+g(s)$;
(ii)

$\exists_{K>1} \mathop{\exists_{A\in\Sigma\cap \Omega}}\limits_{\mu(A)=0} \exists_{p\in L^{1}_{+}(\Omega)} \forall_{s\in\Omega\backslash A} \forall_{u\geq0} \Phi(u)\leq\Psi(Ku)h(s)+p(s)$,

where $h(s)=\frac{d\mu\circ\tau^{-1}}{d\mu}(s)$ for μ-a.e. $s \in \Omega$.

Proof

Obviously, the condition $\mu(\Omega\backslash\tau(\Omega))=0$ is necessary for $c_{\tau}(L^{\Phi}(\Omega))=L^{\Psi}(\Omega)$, so in the further part of the proof we assume this condition holds. Therefore, by Fact 2.1, we know that $c_{\tau}$ acts from $L^{\Phi}(\Omega)$ onto $L^{\Psi}(\Omega)$ if and only if $L^{\Phi}(\Omega)=L^{\Psi}_{h}(\Omega)$. Equivalently, this holds if and only if we have two inclusions: $L^{\Phi}(\Omega) \subset L^{\Psi}_{h}(\Omega)$ and $L^{\Psi}_{h}(\Omega)\subset L^{\Phi}(\Omega)$. The first inclusion holds if and only if condition (i) is satisfied and the reverse inclusion holds if and only if condition (ii) is satisfied (see [51] and [56]), and this finishes the proof. □

It is interesting and profitable to observe that the preceding theorem can be written in the following form.

Theorem 2.5

The composition operator $c_{\tau}$ acts continuously from $L^{\Phi}(\Omega )$ onto $L^{\Psi}(\Omega)$ if and only if $\mu(\Omega\backslash\tau(\Omega))=0$ and for some $K>1$ the following two conditions are jointly satisfied:

(1)

$\int_{\Omega} \chi(h(s) )\,d\mu(s)< \infty$;
(2)

$\int_{\Omega} h(s)q (\frac{1}{h(s)} )\,d\mu(s)<\infty$,

where χ is the function complementary in the sense of Young to the function $\Phi\circ K \Psi^{-1}$, q is the function complementary in the sense of Young to the function $\Psi\circ K \Phi ^{-1}$, and $h(s)=\frac{d\mu\circ\tau^{-1}}{d\mu}(s)$ for μ-a.e. $s \in\Omega$.

Proof

In the proof of Theorem 2.2 we already showed that condition (i) from Theorem 2.4 is equivalent to condition (1). So, the proof will be finished if we show that condition (2) is equivalent to condition (ii) from Theorem 2.4.

It is easy to see that condition (ii) is equivalent to the fact that $q\in L^{1}_{+}(\Omega)$, where

$$\begin{aligned} q(s)=\sup_{u \geq0} \bigl[\Phi(u)-\Psi(Ku)h(s)\bigr] \end{aligned}$$

for all $s\in\Omega$. Since $h(s)\neq0$ for μ-a.e. $s\in\Omega$, we have

$$\begin{aligned} q(s) &= h(s)\sup_{u\geq0} \biggl[\frac{\Phi(u)}{h(s)}-\Psi(Ku) \biggr] \\ &= h(s)\sup_{v\geq0} \biggl[\frac{v}{h(s)}-\Psi\bigl(K\Phi ^{-1}(v)\bigr) \biggr] \\ &= h(s) \bigl(\Psi\circ K\Phi^{-1}\bigr)^{*} \biggl(\frac{1}{h(s)} \biggr) \end{aligned}$$

for μ-a.e. $s\in\Omega$, where $(\Psi\circ K\Phi^{-1})^{*}$ is the complementary function to the function $\Psi\circ K\Phi^{-1}$, which finishes the proof. □

3 Continuity of the multiplication operator $M_{w}$ from $L^{\Phi}$ into $L^{\Psi}$ and from $L^{\Phi}$ onto $L^{\Psi}$

We will state criteria in order that $M_{w}$ map $L^{\Phi}(\Omega, \Sigma ,\mu)$ into $L^{\Psi}(\Omega, \Sigma,\mu)$, where Φ and Ψ are distinct Orlicz functions. Note that $M_{w} x \in L^{\Psi}(\Omega, \Sigma ,\mu)$ means that there is $\lambda>0$ such that $I_{\Psi}(\lambda w(t)x(t) )=\int_{\Omega} \Psi(\lambda w(t)x(t) )\,d\mu (t)<\infty$. This is equivalent to the fact that $x\in L^{\Psi_{w}} (\Omega, \Sigma,\mu)$, where $L^{\Psi_{w}} (\Omega, \Sigma,\mu)$ is a Musielak-Orlicz space generated by the Musielak-Orlicz function $\Psi_{w} (t,u):=\Psi(w(t)u )$. Let us begin with the following.

Theorem 3.1

The multiplication operator $M_{w}$ maps $L^{\Phi}(\Omega, \Sigma,\mu)$ into $L^{\Psi}(\Omega, \Sigma,\mu)$ if and only if $\int_{\Omega}\chi_{K} (t,1)\,d\mu(t)<\infty$ for some $K>1$, where $\chi_{K} (t,u)$ is, for fixed $t\in\Omega$, the function complementary in the sense of Young to the function $\Phi\circ\frac{K}{w(t)} \Psi^{-1}$ with respect to u.

Proof

The fact that $M_{w}:L^{\Phi}(\Omega, \Sigma,\mu)\rightarrow L^{\Psi}(\Omega , \Sigma,\mu)$ means that $L^{\Phi}(\Omega, \Sigma,\mu) \subset L^{\Psi _{w}} (\Omega, \Sigma,\mu)$, which, by Theorem 1.1, holds if and only if there are $A\in\Sigma$ with $\mu(A)=0$, a constant $K>1$, and a function $h\in L_{+} ^{1} (\Omega,\Sigma,\mu)$ such that the inequality

$$ \Psi\bigl(w(t)u \bigr)\leq\Phi(Ku)+h(t) $$

(6)

holds for all $t\in\Omega\setminus A$ and all $u\in\mathbb{R}$. It is easy to see that this is equivalent to the fact that for some $K>1$ the function $\tilde{h}_{K}$ defined by the formula

$$ \tilde{h}_{K} (t)=\sup_{u\in\mathbb{R}} \bigl[ \Psi\bigl(w(t)u \bigr)-\Phi(Ku)\bigr]=\sup_{u\geq0} \bigl[\Psi \bigl(w(t)u \bigr)-\Phi(Ku)\bigr] $$

(7)

is integrable over Ω. In fact, $\tilde{h}_{K}$ is the smallest function such that condition (6) holds with $\tilde{h}_{K}$ in place of h. Setting in (7) $u=\frac{\Psi^{-1}(v)}{w(t)}$, we get

$$ \tilde{h}_{K} (t)=\sup_{v>0} \biggl[v-\Phi\biggl( \frac{K}{w(t)}\Psi^{-1}(v) \biggr) \biggr]=\chi_{K} (t,1), $$

where $\chi_{K} (t,u)$ is the function complementary in the sense of Young to $\Phi\circ\frac{K}{w(t)}\Psi^{-1}$. Therefore, the fact that $M_{w}$ maps continuously $L^{\Phi}(\Omega,\Sigma,\mu)$ into $L^{\Psi}(\Omega,\Sigma,\mu)$ is equivalent to the fact that $\int_{\Omega}\chi_{K} (t,1)\,d\mu(t)<\infty$. □

Theorem 3.2

The multiplication operator $M_{w}$ maps $L^{\Phi}(\Omega, \Sigma,\mu)$ onto the whole of $L^{\Psi}(\Omega, \Sigma,\mu)$ if and only if the following two conditions are jointly satisfied:

(i)

$\int_{\Omega}\chi_{K} (t,1)\,d\mu(t)< \infty$ for some $K>1$, where $\chi_{K} (t,u)$ is the function defined in Theorem 3.1;
(ii)

$\int_{\Omega}U_{K} (t,1)\,d\mu(t)< \infty$ for some $K>1$, where $U_{K} (t,u)$ is, for fixed $t\in\Omega$, the function complementary in the sense of Young, with respect to u, to the function $(\Psi\circ Kw(\cdot)\Phi^{-1} ) (t,u)=\Psi(Kw(t)\Phi^{-1}(u) )$.

Proof

It is obvious that $M_{w}$ maps $L^{\Phi}(\Omega, \Sigma,\mu)$ onto $L^{\Psi}(\Omega, \Sigma,\mu)$ if and only if $\mu(\Omega\backslash \operatorname {supp}w)=0$ and $\{ w(t)x(t): x\in L^{\Phi}\}=L^{\Psi}(\Omega, \Sigma,\mu)$. The space on the left-hand side of the last equality is the Musielak-Orlicz space $L^{\Phi_{w}}(\Omega)$, where $\Phi_{w} (t,u)=\Phi(\frac{u}{w(t)} )$. Observe that $L^{\Phi_{w}}(\Omega,\Sigma,\mu)=L^{\Psi}(\Omega,\Sigma ,\mu)$ is equivalent to $L^{\Phi}(\Omega,\Sigma,\mu)=L^{\Psi_{w}} (\Omega ,\Sigma,\mu)$, where $\Psi_{w} (t,u)=\Psi(w(t)u )$. Therefore, the assumption that $M_{w}$ maps $L^{\Phi}(\Omega, \Sigma,\mu)$ onto $L^{\Psi}(\Omega, \Sigma,\mu)$ means that $L^{\Phi}(\Omega,\Sigma,\mu )=L^{\Psi_{w}} (\Omega,\Sigma,\mu)$, that is, the inclusions $L^{\Phi}(\Omega) \subset L^{\Psi_{w}}(\Omega)$ and $L^{\Psi_{w}}(\Omega) \subset L^{\Phi}(\Omega)$ hold. The preceding theorem established that the first inclusion is equivalent to condition (i). We need only to prove that the reverse inclusion is equivalent to (ii). However, by Ishii’s theorem, the inclusion $L^{\Psi_{w}}(\Omega) \subset L^{\Phi}(\Omega)$ holds if and only if there is a constant $K>1$, a set $A\in\Sigma$ with $\mu(A)=0$, and $g\in L^{1} _{+} (\Omega, \Sigma,\mu)$, such that

$$\begin{aligned} \Phi(u)\leq\Psi\bigl(Kw(t)u \bigr)+g(t) \end{aligned}$$

for all $t\in\Omega\setminus A$ and $u\geq0$. The last condition is equivalent to the condition

$$\begin{aligned} \sup_{u\geq0} \bigl[\Phi(u)-\Psi\bigl(Kw(t)u \bigr) \bigr] \in L^{1} _{+} (\Omega,\Sigma,\mu). \end{aligned}$$

But note that

$$\begin{aligned} \sup_{u\geq0} \bigl[\Phi(u)-\Psi\bigl(Kw(t)u \bigr) \bigr]&=\sup _{v\geq0} \bigl[v-\Psi\bigl(Kw(t)\Phi^{-1}(v) \bigr) \bigr] \\ &=U_{K} (t,1), \end{aligned}$$

where $U_{K} (t,u)$ is, for fixed $t\in\Omega$, the function complementary in the sense of Young, with respect to u, to the function $M(t,u)=\Psi(Kw(t)\Phi^{-1}(u) )$. This finishes the proof. □

4 Compactness of the composition operator $c_{\tau}$ from one Orlicz space into another

We begin with some notions that will be useful in the following. Let $(\Omega,\Sigma, \mu)$ be a non-atomic, complete and σ-finite measure space. We say that functions in a set A contained in the Musielak-Orlicz space $L^{\Phi}(\Omega)$ have equi-absolutely continuous norms if for any real number $\varepsilon>0$ there exist a set $B_{\varepsilon}\in\Sigma$ with $\mu(B_{\varepsilon})<\infty$ and a real number $\delta=\delta(\varepsilon)>0$ such that for any function $x\in A$ we have $\|x \chi_{\Omega\setminus B_{\varepsilon}}\|_{\Phi}<\varepsilon $ and $\|x\chi_{B}\|_{\Phi}<\varepsilon$ whenever $B\in\Sigma\cap B_{\varepsilon}$ and $\mu(B)< \delta$.

Let $L^{\Phi}(\Omega)=L^{\Phi}(\Omega, \Sigma, \mu)$ and $L^{\Psi}(\Omega )=L^{\Psi}(\Omega, \Sigma, \mu)$ be distinct Orlicz spaces. We say that the operator $T: L^{\Phi}(\Omega) \rightarrow L^{\Psi}(\Omega)$ is equi-absolutely continuous if for any bounded set $A \subset L^{\Phi}(\Omega)$ all functions of the set $T (A)\subset L^{\Psi}(\Omega)$ have equi-absolutely continuous norms.

We will make use of the following theorem which gives necessary and sufficient conditions for the relative compactness of a set of functions in a Musielak-Orlicz space.

Theorem 4.1

(Theorem 1.2 in [57])

Let $(\Omega,\Sigma,\mu)$ be a non-atomic σ-finite measure space and let φ be a Musielak-Orlicz function. If the functions in a set $A\subset L^{\varphi}(\Omega)$ all have equi-absolutely continuous norms and A is relatively compact with respect to local convergence in measure, then A is relatively compact in $E^{\varphi}(\Omega)$, the subspace of absolutely continuous functions in $L^{\varphi}(\Omega)$.

Conversely, if a set $A\subset E^{\varphi}(\Omega)$ is relatively compact, then all the functions in A have equi-absolutely continuous norms and A is relatively compact with respect to local convergence in measure.

In the proof of the forthcoming theorem we will need the following.

Lemma 4.1

(Lemma 8.3 in [51])

Let the measure μ be atomless and let a sequence $\{\alpha_{i}\}$ of positive numbers and a sequence $\{a_{i}\}$ of measurable, finite, non-negative functions in Ω be given, satisfying the inequalities

$$\int_{\Omega}a_{i} (t)\,d\mu\geq2^{i} \alpha_{i} \quad\textit{for } i=1,2,\ldots. $$

Then there exist an increasing sequence $\{i_{k}\}$ of positive integers and a sequence $\{A_{k}\}$ of pairwise disjoint sets from Σ such that

$$\int_{A_{k}} a_{i_{k}} (t)\,d\mu=\alpha_{i_{k}} \quad \textit{for } k=1,2\ldots. $$

The following theorem will be of great importance in proving necessary and sufficient conditions for the compactness of the composition operator $c_{\tau}: L^{\Phi}(\Omega) \rightarrow L^{\Psi}(\Omega)$.

Theorem 4.2

Let $(\Omega,\Sigma,\mu)$ be a finite or infinite but σ-finite non-atomic and complete measure space and τ be such that $\mu(\tau ^{-1}(A))<\infty$ whenever $\mu(A)<\infty$ for any $A\in\Sigma\cap \tau(\Omega)$. Then the composition operator $c_{\tau}: L^{\Phi}(\Omega )\rightarrow L^{\Psi}(\Omega)$ is equi-absolutely continuous whenever the following condition is satisfied:

$$ \underset{\sigma>0}{\forall}\ \underset{\substack{A\in \Sigma\cap \tau(\Omega) \\ \mu(A)=0}}{\exists}\ \underset{g_{\sigma}\in L^{1}_{+}(\tau( \Omega))}{\exists}\ \underset{s\in\tau(\Omega)\backslash A}{\forall }\ \underset{u\geq0}{\forall} \Psi(u)h(s)\leq\Phi(\sigma u)+g_{\sigma}(s). $$

(8)

Condition (8) is necessary for the equi-absolute continuity of $c_{\tau}$ if $\mu(\Omega)<\infty$.

Proof

Sufficiency. First we prove that for any $\varepsilon>0$ there exists a set $D\in\Sigma$ with $\mu(\Omega\setminus D)<\infty$ such that all the functions in the set $\{c_{\tau}x: x\in S(L^{\Phi})\}$, where $S(L^{\Phi})$ is the unit sphere of $L^{\Phi}$, satisfy the condition $\|(c_{\tau}x)\chi_{D}\|_{\Psi}<\varepsilon$.

Let $\sigma>0$ be a number such that $(1+\sigma)\sigma<\varepsilon$ and let $g_{\sigma}$ be a function from condition (8) corresponding to σ. Since $g_{\sigma}\in L^{1}_{+}(\tau(\Omega))$, there exists a set $C\in\Sigma\cap\tau(\Omega)$ such that $\|g_{\sigma}\chi_{C}\|_{\Psi}<\sigma$ and $\mu(\tau(\Omega)\setminus C)<\infty$. Defining $D=\tau^{-1}(C)$, we have for any function $x\in S(L^{\Phi})$

$$\begin{aligned} I_{\Psi}\biggl(\frac{c_{\tau}x}{\sigma}\chi_{D} \biggr)&= \int_{\Omega}\Psi\biggl(\frac{c_{\tau}x(t)}{\sigma}\chi_{D} (t) \biggr)\,d\mu(t) \\ &= \int_{D} \Psi\biggl(\frac{x(\tau(t))}{\sigma} \biggr)\,d\mu(t) \\ &= \int_{\tau(D)}\Psi\biggl(\frac{x(s)}{\sigma} \biggr)\,d\mu\circ\tau ^{-1}(s) \\ &= \int_{C}\Psi\biggl(\frac{x(s)}{\sigma} \biggr)h(s)\,d\mu(s) \\ &\leq \int_{C} \Phi\bigl(x(s)\bigr)\,d\mu(s)+ \int_{C} g_{\sigma}(s)\,d\mu(s) \\ &\leq1+\sigma. \end{aligned}$$

(9)

By (9) we get

$$I_{\Psi}\biggl(\frac{(c_{\tau}x)\chi_{D}}{(1+\sigma)\sigma} \biggr)\leq\frac {1}{1+\sigma}I_{\Psi}\biggl(\frac{c_{\tau}x}{\sigma}\chi_{D} \biggr)\leq\frac {1}{1+\sigma}(1+ \sigma)=1 $$

for any $x\in S(L^{\Phi})$. Consequently, $\|(c_{\tau}x)\chi_{D}\|_{\Psi}\leq (1+\sigma)\sigma<\varepsilon$ for any $x\in S(L^{\Phi})$, which finishes the first part of the proof.

Now we show the following implication:

$$\underset{\sigma>0}{\forall}\ \underset{\delta=\delta(\varepsilon)}{\exists}\ \underset{B\subset\tau(\Omega) \setminus D}{\forall}\ \underset{x\in S (L^{\Phi})}{\forall} \mu(B)< \delta\quad\implies\quad \bigl\| (c_{\tau}x)\chi_{B}\bigr\| _{\Psi}< \varepsilon, $$

where D is the set from the first part of this proof.

Take any $x\in S(L^{\Phi})$. Since $g_{\sigma}\in L^{1}_{+}(\tau(\Omega))$, it is obvious that there is $\delta=\delta(\sigma)>0$ such that, if $C\in \Sigma\cap(\tau(\Omega)\setminus D)$ and $\mu(C)<\delta$, then $\int_{C} g_{\sigma}(s)\,d\mu(s)<\sigma$. Let $B=\tau^{-1}(C)$. Then applying condition (8), we get

$$\begin{aligned} I_{\Psi}\biggl(\frac{c_{\tau}x}{\sigma}\chi_{B} \biggr)&= \int_{\Omega}\Psi\biggl(\frac{c_{\tau}x(t)}{\sigma}\chi_{B} (t) \biggr)\,d\mu(t) \\ &= \int_{B} \Psi\biggl(\frac{x(\tau(t))}{\sigma} \biggr)\,d\mu(t) \\ &= \int_{\tau(B)}\Psi\biggl(\frac{x(s)}{\sigma} \biggr)\,d\mu\circ\tau ^{-1}(s) \\ &= \int_{C}\Psi\biggl(\frac{x(s)}{\sigma} \biggr)h(s)\,d\mu(s) \\ &\leq \int_{C} \Phi\bigl(x(s)\bigr)\,d\mu(s)+ \int_{C} g_{\sigma}(s)\,d\mu(s) \\ &\leq1+\sigma. \end{aligned}$$

(10)

Now, by convexity of the modular $I_{\Psi}$ and the fact that $I_{\Psi}$ vanishes at zero we have $I_{\Psi}(\lambda x)\leq\lambda I_{\Psi}(x)$ for any $x\in L^{\Psi}(\Omega)$ and $\lambda\in[0,1]$. From this fact and from (10), we get

$$I_{\Psi}\biggl(\frac{(c_{\tau}x)\chi_{B}}{(1+\sigma)\sigma} \biggr)\leq\frac {1}{1+\sigma}I_{\Psi}\biggl(\frac{c_{\tau}x}{\sigma}\chi_{B} \biggr)\leq\frac {1}{1+\sigma}(1+ \sigma)=1. $$

Hence $\|(c_{\tau}x)\chi_{B}\|_{\Psi}\leq(1+\sigma)\sigma<\varepsilon$. Since σ depends only on ε, $\delta=\delta(\sigma )$ depends only on ε, and so the proof of sufficiency is finished.

Necessity. Assume that $\mu(\Omega)<\infty$ and for any $\sigma>0$ define the function

$$h_{\sigma}(s)=\sup_{u\geq0}\bigl\{ \Psi(u)h(s)-\Phi(\sigma u)\bigr\} . $$

$h_{\sigma}(s)$ is a non-negative (since for $u=0$, we have $\Psi(0)h(s)-\Phi (\sigma0)=0$) measurable function.

Suppose condition (8) is not satisfied. Then there is $\sigma _{0}>0$ such that

$$\int_{\tau(\Omega)} h_{\sigma_{0}}(s)\,d\mu(s)=+\infty. $$

Let $\{r_{i}\}_{i=0}^{\infty}$ be a sequence of all non-negative rational numbers with $r_{0} =0$. By the continuity of the Orlicz functions Φ and Ψ, we have

$$h_{\sigma_{0}} (s)=\sup_{i=0,1,2 \dots}\bigl\{ \Psi(r_{i})h(s)- \Phi(\sigma_{0} r_{i})\bigr\} . $$

Let us write

$$h_{\sigma_{0},n} (s)=\max_{0\leq i \leq n}\bigl\{ \Psi(r_{i})h(s)- \Phi(\sigma_{0} r_{i})\bigr\} . $$

It is obvious that $h_{\sigma_{0},n}\geq0$ and $h_{\sigma_{0},n}$ are measurable functions such that $h_{\sigma_{0},n} \nearrow h_{\sigma _{0}}$ as $n\rightarrow+\infty$ μ-a.e. in $\tau(\Omega)$. By Beppo Levi’s theorem, we have

$$\int_{\tau(\Omega)} h_{\sigma_{0},n} (s)\,d\mu(s) \nearrow \int_{\tau(\Omega)} h_{\sigma_{0}} (s)\,d\mu(s). $$

Hence there exists a subsequence $\{h_{\sigma_{0},n_{k}} \}\subset\{ h_{\sigma_{0},n}\}$ satisfying

$$\int_{\tau(\Omega)} h_{\sigma_{0},n_{k}} (s)\,d\mu(s) \geq2^{k}. $$

Without loss of generality we may assume that $\int_{\tau(\Omega)} h_{\sigma _{0},n} (s)\,d\mu(s) \geq2^{n}$ for each $n\in\mathbb{N}\cup\{0\}$. It is clear that for each $s\in\tau(\Omega)$ and each $n\in\mathbb{N}\cup\{ 0\}$ there exists $\widetilde{r}_{n} (s)\in\{r_{0},r_{1},r_{2}, \ldots, r_{n}\}$ such that

$$h_{\sigma_{0},n} (s)=\Psi\bigl(\widetilde{r}_{n} (s)\bigr)h(s)-\Phi \bigl(\sigma_{0} \widetilde{r}_{n} (s)\bigr). $$

Hence

$$\begin{aligned} \int_{\tau(\Omega)}\Psi\bigl(\widetilde{r}_{n} (s)\bigr)h(s)\,d\mu(s)&= \int_{\tau(\Omega)} h_{\sigma _{o},n} (s)\,d\mu(s)+ \int_{\tau(\Omega)}\Phi\bigl(\sigma_{0} \widetilde{r}_{n} (s)\bigr)\,d\mu(s) \geq2^{n}. \end{aligned}$$

Applying Lemma 4.1, we conclude that there is a sequence of sets $\{\Omega_{k}\} \subset \tau(\Omega)$ with $\Omega_{i} \cap\Omega_{j} =\emptyset$ for $i\neq j$ such that

$$\int_{\Omega_{n}} \Psi\bigl(\widetilde{r}_{n} (s)\bigr)h(s)\,d\mu(s)=1. $$

Let $\bar{r}_{n} (s)=\widetilde{r}_{n} (s) \chi_{\Omega_{n}} (s)$. Since $\bar {r}_{n}$ are bounded measurable functions and $h\in L^{1} (\operatorname {supp}\bar {r}_{n})$, we get $\bar{r}_{n} \in E^{\Psi}_{h} (\Omega)$ with $\|\bar{r}_{n}\| _{\Psi,h} =1$ and $\bar{r}_{n} \in L^{\Phi}(\Omega)$ for any $n\in\mathbb {N}\cup\{0\}$.

Since, by assumption, $\mu(\Omega)<\infty$, we have $\sum_{n=0}^{\infty } \mu(\Omega_{n})=\mu(\bigcup_{n=0}^{\infty}\Omega _{n})\leq\mu(\Omega)<\infty$, whence $\lim_{n\rightarrow\infty} \mu(\Omega_{n})=0$. This means that $\{\bar{r}_{n}\}_{n=1}^{+\infty}$ does not have equi-absolutely continuous norms in $E^{\Psi}_{h} (\Omega)$. Yet, using the fact that $g_{\sigma_{0},n}\geq0 $ ($n\in\mathbb{N}\cup\{0\}$), we get the following:

$$\Psi\bigl(\bar{r}_{n} (s)\bigr)h(s)\geq\Phi\bigl(\sigma_{0} \bar{r}_{n} (s)\bigr), \quad n\in\mathbb{N}\cup\{0\}. $$

So $I_{\Phi}(\sigma_{0} \bar{r}_{n})\leq1$, that is, $\|\bar{r}_{n}\|_{\Phi}\leq\frac{1}{\sigma_{0}}$, which means that the operator $c_{\tau}: L^{\Phi}(\Omega)\rightarrow L^{\Psi}(\Omega)$ is not equi-absolutely continuous. Hence we proved that condition (8) is necessary for the equi-absolutely continuity of $c_{\tau}$. □

From Theorem 4.2, applying Theorem 4.1 and the definition of a compact operator, we directly get the following.

Theorem 4.3

If $(\Omega,\Sigma, \mu)$ is a non-atomic complete finite or infinite but σ-finite measure space and τ satisfies the assumption from Theorem 4.2, then the composition operator $c_{\tau}$ from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$ is compact whenever the set $c_{\tau}(S(L^{\Phi}))$ is relatively compact with respect to local convergence in measure and condition (8) from Theorem 4.2 is satisfied.

Under the assumption that $\mu(\Omega)<\infty$, if the composition operator $c_{\tau}$ from $L^{\Phi}(\Omega)$ into $E^{\Psi}(\Omega)$ is compact then the set $c_{\tau}(S(L^{\Phi}))$ is relatively compact with respect to convergence in measure and condition (8) is satisfied.

In the case when Ω has infinite measure, we were unable to show that (8) is a necessary condition for the equi-absolute continuity of the composition operator $c_{\tau}$. Instead, we can deduce a slightly different (and weaker) condition, as the following theorem states.

Theorem 4.4

Assume that $\mu(\Omega)=\infty$ and $\mu(\Omega\backslash\tau(\Omega))=0$. If the composition operator $c_{\tau}: L^{\Phi}(\Omega)\rightarrow L^{\Psi}(\Omega)$ is equi-absolutely continuous, then the condition

$$ \underset{\lambda>0}{\forall}\ \underset{\substack{A\in \Sigma \\ \mu(A)=0}}{\exists}\ \underset{K_{\lambda}>0}{\exists}\ \underset{g_{\lambda}\in L^{1}_{+}(\Omega)}{\exists}\ \underset{s \in\Omega\backslash A}{\forall}\ \underset{u\geq0}{\forall} \Psi (\lambda u)h(s) \leq K_{\lambda}\Phi(u)+g_{\lambda}(s) $$

(11)

is satisfied.

Proof

We can assume without loss of generality that $\tau(\Omega)=\Omega$. First, notice that if Φ, Ψ, and h satisfy condition (11) then $L^{\Phi}(\Omega) \subset E^{\Psi}_{h} (\Omega)$, where

$$E^{\Psi}_{h} (\Omega)=\biggl\{ x\in L^{0} (\Omega): \underset{\lambda>0}{\forall} I_{\Psi,h} (\lambda x)= \int_{\Omega}\Psi\bigl(\lambda x(t)\bigr)h(t)\,d\mu(t)< \infty\biggr\} $$

is the subspace of absolutely continuous elements of $L^{\Psi}_{h} (\Omega)$. The inclusion results from the assumption that $c_{\tau}$ is an equi-absolutely continuous operator, i.e., for any bounded set $A \subset L^{\Phi}(\Omega)$, the functions of the set $c_{\tau}(A)\subset L^{\Psi}(\Omega)$ all have equi-absolutely continuous norms, and the observation that, for any $x\in L^{\Phi}(\Omega)$, the singleton set $\{x\}$ is bounded, and thus x has an equi-absolutely continuous norm, which means that x is an absolutely continuous element of $L^{\Psi}_{h} (\Omega)$, i.e., $x\in E^{\Psi}_{h} (\Omega)$.

Further, observe that

$$\begin{aligned}& L^{\Phi}(\Omega)=\bigcup_{\lambda>0} L^{{\Phi_{\lambda}},*} (\Omega),\qquad E^{\Psi}_{h} (\Omega)=\bigcap_{\lambda>0} L^{{\Psi_{\lambda}},*}_{h} (\Omega), \end{aligned}$$

where for any $\lambda>0$ we define $\Phi_{\lambda}(u)=\Phi(u)$ and $L^{\Phi,*} (\Omega)=\{x\in L^{0} (\Omega): I_{\Phi}(x)<\infty\}$ is a Musielak-Orlicz class ($\Psi_{\lambda}$ and $L^{\Psi,*}_{h} (\Omega)$ are defined analogously). Hence the inclusion $L^{\Phi}(\Omega) \subset E^{\Psi}_{h} (\Omega)$ can be expressed as

$$\bigcup_{\lambda>0} L^{{\Phi_{\lambda}},*} (\Omega) \subset \bigcap_{\lambda>0} L^{{\Psi_{\lambda}},*}_{h} ( \Omega). $$

This means that, for any $\lambda_{1}>0$, the Musielak-Orlicz class $L^{\Phi_{\lambda_{1}},*} (\Omega)$ is contained in all of $L^{\Psi _{\lambda},*}_{h} (\Omega) $ ($\lambda>0$). In particular, taking $\lambda _{1} =1$, we see that $L^{\Phi,*} (\Omega)$ is contained in all the Musielak-Orlicz classes $L^{\Psi_{\lambda},*}_{h} (\Omega) $ ($\lambda>0$). By Theorem 8.4 in [51], this is equivalent to

$$ \underset{\lambda>0}{\forall}\ \underset{\substack{A\in\Sigma \\ \mu(A)=0}}{\exists}\ \underset{K_{\lambda}>0}{\exists}\ \underset{g_{\lambda}\in L^{1}_{+}(\Omega)}{\exists}\ \underset{s \in\Omega\backslash A}{\forall}\ \underset{u\geq0}{\forall} \Psi (\lambda u)h(s) \leq K_{\lambda}\Phi(u)+g_{\lambda}(s), $$

which finishes the proof. □

From the preceding theorem, applying Theorem 4.1, we can deduce the following necessary condition for the compactness of the composition operator $c_{\tau}$:

Theorem 4.5

Assume that $\mu(\Omega)=\infty$ and $\mu(\Omega\backslash\tau(\Omega))=0$. If the composition operator $c_{\tau}: L^{\Phi}(\Omega)\rightarrow E^{\Psi}(\Omega)$ is compact then the following conditions are jointly satisfied:

(1)

the set $c_{\tau}(S(L^{\Phi}))$ is relatively compact with respect to local convergence in measure;
(2)

the functions Φ and Ψ satisfy condition (11).

Remark 4.1

If there exists $\varepsilon>0$ such that the set

$$B_{\varepsilon}:= \Bigl\{ t\in\tau(\Omega)\colon\underset{u\geq0}{\forall} \Psi(u)h(t)>\Phi(\varepsilon u) \Bigr\} $$

has positive measure, then no composition operator $c_{\tau}:L^{\Phi}(\Omega)\rightarrow L^{\Psi}(\Omega)$ over a non-atomic measure space $(\Omega,\Sigma,\mu)$ is compact.

Proof of Remark 4.1

Assume that there exists $\varepsilon >0$ such that the measure of the set $B_{\varepsilon }$ is positive. Then in the set $B_{\varepsilon }$ we can find a sequence of measurable and pairwise disjoint sets $\{B_{n} \}$ in $\tau(\Omega)$ having positive and finite measure. Define

$$x_{n}=\frac{\chi_{B_{n}}}{\Vert \chi_{B_{n}}\Vert _{\Phi}}=\Phi^{-1} \biggl(\frac{1}{\mu(B_{n})} \biggr)\chi_{B_{n}}. $$

Obviously, $I_{\Phi}(x_{n})=1$, so $\|x_{n}\|_{\Phi}=1$ for all $n\in\mathbb{N}$. We have

$$\begin{aligned} I_{\Phi}\biggl(\frac{\varepsilon x_{n}}{\Vert x_{n}\circ\tau \Vert _{\Psi}}, \Omega \biggr) =& \int_{\tau(\Omega)}\Phi\biggl(\frac{\varepsilon x_{n}(t)}{\Vert x_{n}\circ\tau \Vert _{\Psi}} \biggr)\,d\mu(t)\\ < & \int_{\tau(\Omega)}\Psi\biggl(\frac{x_{n}(t)}{\Vert x_{n}\circ\tau \Vert _{\Psi}} \biggr)h(t)\,d\mu(t) \\ =& \int_{\Omega}\Psi\biggl(\frac{(x_{n}\circ\tau)(t)}{\Vert x_{n}\circ\tau \Vert _{\Psi}} \biggr)\,d\mu(t) =I_{\Psi}\biggl(\frac{c_{\tau}x_{n}}{\Vert c_{\tau}x_{n} \Vert _{\Psi}},\Omega\biggr)\leq1. \end{aligned}$$

Therefore,

$$\biggl\Vert \frac{\varepsilon x_{n}}{\Vert x_{n}\circ\tau \Vert _{\Psi}}\biggr\Vert _{\Phi}\leq1, $$

i.e., $\Vert c_{\tau}x_{n}\Vert _{\Psi}\geq \varepsilon \Vert x_{n}\Vert _{\Phi}=\varepsilon $ because $\|x_{n}\|_{\Phi}=1$. Since the supports of $x_{n}$ are pairwise disjoint, for all $n,m\in \mathbb {N}$, $m\neq n$ we get

$$\Vert c_{\tau}x_{n}-c_{\tau}x_{m} \Vert _{\Psi}=\bigl\Vert c_{\tau}(x_{n}-x_{m}) \bigr\Vert _{\Psi}\geq\max\bigl\{ \Vert c_{\tau}x_{n}\Vert _{\Psi}, \Vert c_{\tau}x_{m} \Vert _{\Psi}\bigr\} \geq \varepsilon . $$

Hence the sequence $\{c_{\tau}x_{n} \}_{n=1}^{\infty}$ has no Cauchy subsequence, that is, $c_{\tau}(S (L^{\Phi}(\Omega) ) )$ is not relatively compact. Consequently, no composition operator $c_{\tau}$ from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$ over a non-atomic measure space $(\Omega,\Sigma ,\mu)$ is compact. □

5 Compactness of the multiplication operator $M_{w}$ from one Orlicz space into another

We state a sufficient condition for the compactness of the multiplication operator $M_{w}:L^{\Phi}(\Omega)\rightarrow L^{\Psi}(\Omega)$.

Theorem 5.1

Let $(\Omega,\Sigma,\mu)$ be a non-atomic complete, finite or infinite but σ-finite measure space and let Φ, Ψ be two Orlicz functions and $w\in L^{0} _{+} (\Omega,\Sigma,\mu)$. If the triple Φ, Ψ, w satisfies the condition

$$ \underset{\sigma>0}{\forall}\ \underset{\substack{A_{\sigma}\in\Sigma \\ \mu(A_{\sigma})=0}}{\exists}\ \underset{g_{\sigma}\in L^{1}_{+}(\Omega)}{\exists}\ \underset{t\in\Omega\backslash A}{\forall}\ \underset{u\geq0}{\forall} \Psi\bigl(w(t)u\bigr)\leq\Phi(\sigma u)+g_{\sigma}(t) $$

(12)

then the multiplication operator $M_{w}$ from $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$ is equi-absolutely continuous.

Proof

First we show that given $\varepsilon>0$ there exists a set $B\in\Sigma $ with $\mu(B)<\infty$ such that $\|x \chi_{\Omega\setminus B}\|_{\Psi}<\varepsilon$ for any function $x\in S(L^{\Phi}(\Omega))$.

Take $\varepsilon>0$ and let $\sigma>0$ be such that $\sigma(1+\sigma )<\varepsilon$. Let $g_{\sigma}$ be a function from condition (12) corresponding to σ. Since $g_{\sigma}\in L^{1} _{+} (\Omega)$, there exists $B\in\Sigma$ with $\mu(B)<\infty$ such that $\|g_{\sigma}\chi_{\Omega\setminus B}\|_{L^{1} (\Omega)}<\sigma$. Then

$$ I_{\Psi}\biggl(\frac{M_{w} x}{\sigma}\chi_{\Omega\setminus B} \biggr) \leq I_{\Phi}(x\chi_{\Omega\backslash B}) + \int_{\Omega\setminus B} g_{\sigma}(t)\,d\mu(t)\leq1+\sigma, $$

whence

$$ I_{\Psi}\biggl(\frac{M_{w} x}{\sigma(1+\sigma)}\chi_{\Omega\setminus B} \biggr)\leq \frac{1}{1+\sigma}I_{\Psi}\biggl(\frac{M_{w} x\chi_{\Omega\backslash B}}{\sigma} \biggr)\leq \frac{1}{1+\sigma}(1+\sigma)=1, $$

that is, $\|M_{w} x\chi_{\Omega\setminus B}\|_{\Psi}\leq\sigma(1+\sigma )<\varepsilon$.

Next, we show that for $\varepsilon>0$ there exists $\delta=\delta (\varepsilon)>0$ such that for any $D\subset B$ and any function $x\in S(L^{\Phi})$, if $\mu(D)<\delta$ then $\|M_{w} x\chi_{D}\| _{\Psi}<\varepsilon$.

Let $\varepsilon>0$ and let $\sigma>0$ be such that $\sigma(1+\sigma )<\varepsilon$. By the absolute continuity of $g_{\sigma}$ in $L_{1} (\Omega \cap B)$, there exists $\delta=\delta(\sigma)$ such that $\|g_{\sigma}\chi_{C}\|_{L^{1} (\Omega)} <\sigma$ whenever $C\subset B$ and $\mu (C)<\delta$. Then, by condition (12),

$$ I_{\Psi}\biggl(\frac{M_{w} x}{\sigma}\chi_{C} \biggr) \leq I_{\Phi}(x\chi_{C}) + \|g_{\sigma}\chi_{C} \|_{L^{1} (\Omega)}\leq1+\sigma, $$

whence

$$ I_{\Psi}\biggl(\frac{M_{w} x}{\sigma(1+\sigma)}\chi_{C} \biggr)\leq \frac {1}{1+\sigma}I_{\Psi}\biggl(\frac{M_{w} x\chi_{C}}{\sigma} \biggr)\leq1, $$

and so $\|M_{w} x\|_{\Psi}\leq\sigma(1+\sigma)<\varepsilon$, which finishes the proof. □

Remark 5.1

Let us note that in the case when $\Phi=\Psi$, Theorem 5.1 can only hold when $\Phi\in\Delta_{2}(\infty)$.

Indeed, if Theorem 5.1 holds, then the operator $M_{w}$ acts, in fact, from $L^{\Phi}(\Omega)$ into $E^{\Phi}(\Omega)$. However, if we assume that $\Phi\notin\Delta_{2}(\infty)$ and $w\notin L^{\infty}(\Omega ,\Sigma,\mu)$, then defining the set

$$A=\bigl\{ t\in\Omega: w(t)\geq2\bigr\} , $$

we have $\mu(A)>0$. Therefore, we can build $x\in L^{\Phi}(\Omega)$ such that $\operatorname{ \operatorname {supp}} x\subset A$, $I_{\Phi}(x)\leq1$, and $I_{\Phi}(\lambda x)=\infty$ for any $\lambda>1$ (see [58] and [59]). Hence $I_{\Phi}(M_{w} x)\geq I_{\Phi}(2x)=\infty$, which means that $M_{w} x\notin E^{\Phi}(\Omega)$, so $M_{w}$ does not act from $L^{\Phi}(\Omega)$ into $E^{\Phi}(\Omega)$.

Applying Theorem 4.1, we directly get from Theorem 5.1 and the definition of a compact operator the following.

Theorem 5.2

If $(\Omega,\Sigma, \mu)$ is a non-atomic complete finite or infinite but σ-finite measure space, then the multiplication operator $c_{\tau}$ form $L^{\Phi}(\Omega)$ into $L^{\Psi}(\Omega)$ is compact whenever the set $M_{w}(S(L^{\Phi}))$ is relatively compact with respect to local convergence in measure and condition (12) from Theorem 5.1 is satisfied.

Theorems 5.1 and 5.2 resemble closely the sufficiency part of Theorems 4.2 and 4.3 for the composition operator. Similarly, we will formulate necessary conditions for the equi-absolute continuity of the multiplication operator: one in the case when $\mu(\Omega)<\infty$ and the other in the case when $\mu(\Omega)=\infty$. The respective proofs proceed along the lines of the proofs for the composition operator, and therefore will be omitted.

Theorem 5.3

If $(\Omega,\Sigma,\mu)$ is a finite non-atomic and complete measure space and the multiplication operator $M_{w}: L^{\Phi}(\Omega)\rightarrow L^{\Psi}(\Omega)$ is equi-absolutely continuous then the following condition is satisfied:

$$ \underset{\sigma>0}{\forall}\ \underset{\substack{A\in\Sigma \\ \mu(A)=0}}{\exists}\ \underset{g_{\sigma}\in L^{1}_{+}(\Omega)}{ \exists}\ \underset{t\in\Omega\backslash A}{\forall}\ \underset{u\geq 0}{\forall} \Psi\bigl(w(t)u\bigr)\leq\Phi(\sigma u)+g_{\sigma}(t). $$

Theorem 5.4

If $(\Omega,\Sigma,\mu)$ is an infinite but σ-finite non-atomic and complete measure space and the multiplication operator $M_{w}: L^{\Phi}(\Omega)\rightarrow L^{\Psi}(\Omega)$ is equi-absolutely continuous, then the following condition is satisfied:

$$ \underset{\lambda>0}{\forall}\ \underset{\substack{A\in\Sigma \\ \mu(A)=0}}{\exists}\ \underset{K_{\lambda}>0}{\exists}\ \underset{g_{\lambda}\in L^{1}_{+}(\Omega)}{\exists}\ \underset{t \in\Omega\backslash A}{\forall}\ \underset{u\geq0}{\forall} \Psi\bigl(w(t) \lambda u\bigr)\leq K_{\lambda}\Phi(u)+g_{\lambda}(t). $$

The respective necessary conditions for the compactness of the multiplication operator are analogous to the ones for the composition operator from Theorems 4.3 and 4.5.

Declarations

Acknowledgements

The second author is supported by NFS of Heilong Jiang province (A2015018).

Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Authors’ Affiliations

(1)

Department of Mathematics, Faculty of Mathematics and Computer Science, Adam Mickiewicz University in Poznań, Poznań, Poland

(2)

Department of Mathematics, Harbin University of Science and Technology, Harbin, 150080, P.R. China

(3)

Department of Mathematics, Payame Noor University (PNU), P.O. Box: 19395-3697, Tehran, Iran

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