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(1)

On

Orlicz-Morrey

spaces

大阪教育大学教育学部 中井英– (Eiichi Nakai)

Department of

Mathematics

Osaka Kyoiku University

1.

INTRODUCTION

In this paper

we

state basic properties of

Orlicz-Morrey

spaces and a

definition

ofitspredual without proofs. This is

an

announcement ofmy recent works.

Orlicz spaces

are

generalization ofLebesgue spaces $L^{\mathrm{p}}$

.

They

are

useful tools to

study

harmonic

analysis and its applications. For example, the Hardy-Littlewood

maximal operator is bounded

on

$IP$ for $1<p\leq\infty$, but not

bounded

on $L^{1}$.

Using Orlicz spaces,

we

caninvestigatethe

boundedness

ofthe operator

near

$p=1$

precisely (see Kita [5, 6] and Cianchi [3]). It is known that fractional integral

operators $I_{\alpha}$ is

bounded

from

$L^{\mathrm{P}}(\mathrm{R}^{n})$ to

$L^{q}(\mathrm{R}^{n})$ for

$1<p<q<\infty \mathrm{t}\mathrm{d}-n/p+$

$\alpha=-n/q$ as the Hardy-Littlewood-Sobolev theorem.

Rudinger [29] investigated the

boundedness

of $I_{\alpha}$

near

$q=\infty$

.

The Hardy-Littlewood-Sobolev

theorem

and

hudinger’s result

are

generalized by several authors, [20, 26, 27, 4, 3, 15, 16, 17],

etc. For the theory of Orlicz spaces,

see

[10, 7, 24].

On the other hand Morrey spaces

was

introduced by [11] to estimate

solutions

of

Partial

differential

equations.

After

that there

are

many

Papers about Morrey

spaces. For the

boundedness

of the Hardy-Littlewood maximal operatdr and

hac-tional integral operators, see [23, 1, 2, 12].

The author introduced Orlicz-Morrey spaces in [18] to investigate the

bounded-ness

ofgeneralized fractional integral operators.

Orlicz-Morrey

spaces unify

Orlicz

and Morrey spaces. Recently, using

Orlicz-Morrey

spaces, Sawano,

Sobukawa

and

Tanaka

[25] proved

a

Tlrudinger type inequality for Morreyspaces.

Our definition of

Orlicz-Morrey

space is

different

from

one

in

Kokilashvih

and

Krbec [7, p.2].

2000MathematicsSubject Classification. $46\mathrm{E}30,42\mathrm{B}35,42\mathrm{B}2526\mathrm{A}33$

.

(2)

We recall the

definitions

and several properties of Orlicz and Morrey spac\’e in

the next section. We state a definition of Orlicz-Morrey spaces in Section 3. In

Section

4,

we

givegeneralized H\"older’s inequality and inclusion relationsfor

Orlicz-Morreyspaces. InSection5wegiveadefinition ofpredualsofOrlicz-Morrey spaces.

2. DEFINITIONS AND

PROPERTIES

OF ORLICZ AND MORREY SPACES

A function $\theta$ :

$(0, +\infty)arrow(0, +\infty)$ is said to be almost increasing (almost

de-creasing) ifthereexists a constant $C>0$such that

$\theta(r)\leq C\theta(s)$ $(\theta(r)\geq C\theta(s))$ for $r\leq s$.

A function $\theta:(0, +\infty)arrow(0, +\infty)$ is said tosatisfy the doubling condition if there

exists aconstant $C>0$ such that

$C^{-1} \leq\frac{\theta(r)}{\theta(s)}\leq C$ for $\frac{1}{2}\leq\frac{r}{s}\leq 2$

.

For functions $\theta,$$\kappa$ : $(0, +\infty)arrow(0, +\infty)$,

we

denote

$\theta(r)\sim\kappa(r)(\theta(r)\approx\kappa(r))$ if

thereexists a constant $C>0$ such that

$C^{-1}\theta(r)\leq\kappa(r)\leq C\theta(r)$ $(\theta(C^{-1}r)\leq\kappa(r)\leq\theta(Cr))$ for $r>0$

.

First

we

recall the definition of Young functions. A function $\Phi$ : $[0, +\infty]arrow$

$[0, +\infty]$ is called a Young function if $\Phi$ is convex, left-continuous,

$\lim\Phi(r)=$ $tarrow+0$

$\Phi(0)=0$ and $\lim_{rarrow+\infty}\Phi(r)=\Phi(+\infty)=+\infty$

.

Any Youngfunction is neither

identi-cally

zero nor

identically infinite on $(0, +\infty)$

.

IFYomthe convexity and $\Phi(0)=0$ it

follows that any Young functionis increasing.

Ifthere exists $s\in(0, +\infty)$ such that $\Phi(s)=+\infty$, then $\Phi(r)=+\infty$ for $r\geq s$

.

Let $r_{0}= \inf\{s>0 : \Phi(s)=+\infty\}$

.

Then $r_{0}>0$, since $\lim_{farrow+0}\Phi(r)=\Phi(0)=0$.

If $\Phi(r_{0})<+\infty$, then $\Phi$ is absolutely continuous on

$[0,r_{0}]$ by the convexity and

increasingness. If $\Phi(r_{0})=+\infty$, then $\Phi$ is absolutely continuous

on

any closed

interval in $[0,r_{0})$ and $\lim_{rarrow\prime 0^{-0}}\Phi(r)=+\infty$ by left-continuity.

Let $\mathcal{Y}$ be the set of all Young

functions $\Phi$ such that

(2.1) $0<\Phi(r)<+\infty$ for $0<r<+\infty$

.

If $\Phi\in \mathcal{Y}$, then $\Phi$ is absolutely continuous on any closed

interval in $[0, +\infty)$ and

bijective from $[0, +\infty)$ to itself.

A Young function $\Phi$ is said to satisfy the $\Delta_{2}$-condition, denoted$\Phi\in\Delta_{2}$, if

(3)

for

some

$C>0$.

A Young function $\Phi$ is said to satisfy the $\nabla_{2}$-condition, denoted $\Phi\in\nabla_{2}$, if

$\Phi(r)\leq\frac{1}{2k}\Phi(kr)$, $r\geq 0$,

for some $k>1$

.

If$p>1$, then $\Phi(r)=r^{\mathrm{p}}$ satisfies both the $\Delta_{2}$-condition and the $\nabla_{2}$-condition. If $p=1$, then $\Phi(r)=r^{\mathrm{p}}$ satisfies the $\Delta_{2}$-condition, but does not

satisfy $\nabla_{2}$-condition.

For aYoung function $\Phi$, the complementary function

is defined by

$\tilde{\Phi}(r)=\sup\{rs-\Phi(s) : s\geq 0\}$, $r\geq 0$

.

Then $\tilde{\Phi}-=\Phi$

, and, $\Phi\in\Delta_{2}$ ifand only if$\overline{\Phi}\in\nabla_{2}$

.

Example 2.1. (i) If$\Phi(r)=r^{p}/p,$ $1<p<\infty$, then $\tilde{\Phi}(r)=r^{\mathrm{p}’}/p’,$ $1/p+1/p’=1$

.

(ii) If$\Phi(r)=r$, then $\tilde{\Phi}(r)=0(0\leq r\leq 1),$$=+\infty(r>1)$

.

(iii) If$\Phi(r)=(r+1)\log(r+1)-r$, then $\tilde{\Phi}(r)=e^{f}-r-1$.

For aYoung function $\Phi$ and for $0\leq s\leq+\infty$, let

$\Phi^{-1}(s)=\inf\{r\geq 0:\Phi(r)>s\}$ (inf$\emptyset=+\infty$).

If $\Phi\in \mathcal{Y}$, then $\Phi^{-1}$ is the usual inverse function

of$\Phi$

.

We note that

$\Phi(\Phi^{-1}(r))\leq r\leq\Phi^{-1}(\Phi(r))$, for $0\leq r<+\infty$

.

For a Young function $\Phi$ and its complementary function $\overline{\Phi}$

, we have

$r\leq\Phi^{-1}(r)\overline{\Phi}^{-1}(r)\leq 2r$, $0<r<+\infty$

.

Using this relation, we havethe following.

Example 2.2. (i) Let $1<p:<\infty,$ $1/p_{i}+1/p_{i}’=1,$ $-\infty<\beta_{i}<+\infty(i=1,2)$

.

If

$\Phi(r)\approx\{$

$r^{p_{1}}(\log r)^{\mathrm{P}1\beta_{1}}$ for large $r$, $r^{\mathrm{p}_{2}}(1/\log(1/r))^{p\mathrm{a}\beta_{2}}$ for small $r$,

then

$\tilde{\Phi}(r)\approx\{$

$r^{d_{1}}(\log r)^{-p_{1}’\rho_{1}}$ forlarge $r$,

(4)

(ii) Let $0<p_{1},p_{2}<\infty$. If

$\Phi(r)\approx\{$

$r(\log r)^{1/p1}$ for large$r$, $r(1/\log(1/r))^{1/p_{2}}$ for small$r$,

then

$\overline{\Phi}(r)\approx\{$

$\exp(r^{p_{1}})$ for large$r$,

$1/\exp(1/r^{\mathrm{P}2})$ for small $r$

.

(iii) Let $0<p_{1},p_{2}<\infty$

.

If

$\Phi(r)\approx\{$

$r(\log\log r)^{1/p_{1}}$ for large$r$, $r(1/\log\log(1/r))^{1/p_{2}}$ for small$r$,

then

$\overline{\Phi}(r)\approx\{$

$\exp\exp(r^{p_{1}})$ for large $r$,

$1/\exp\exp(1/r^{\mathrm{P}2})$ for small $r$

.

Wenotethat, for Young functions $\Phi$ and $\Psi$, ifthereexist $C\geq 1$ and $R\geq 1$ such

that

$\Phi(C^{-1}r)\leq\Psi(r)\leq\Phi(Cr)$ for $r\in(0, R^{-1})\cup(R, +\infty)$, then $\Phi\approx\Psi$.

Definition 2.1 (Orlicz space). For aYoung function $\Phi$, let

$L^{\Phi}(\mathrm{R}^{n})=\{f\in L_{1\mathrm{o}\mathrm{c}}^{1}(\mathrm{R}^{n})$: $\int_{\mathrm{R}^{n}}\Phi(k|f(x)|)dx<+\infty$ for

some

$k>0\}$ ,

$||f||_{L^{\bullet}}= \inf\{\lambda>0:\int_{\mathrm{R}^{\mathfrak{n}}}\Phi(\frac{|f(x)|}{\lambda})dx\leq 1\}$

.

Let

$M^{\Phi}(\mathrm{R}^{n})=\{f\in L^{\Phi}(\mathrm{R}^{n})$ : $\int_{\mathrm{R}^{\mathrm{n}}}\Phi(\forall k|f(x)|)dx<+\infty\}$

.

Then $||f||_{L^{\bullet}}$ is

a

norm and $L^{\Phi}(\mathrm{R}^{n})$ is

a

Banach space. This

norm

is introduced

by Nakano [19] and Luxemburg [9]. $M^{\Phi}(\mathrm{R}^{n})$ is a closed subspace of $L^{\Phi}(\mathrm{R}^{\mathrm{n}})$. If

$\Phi(r)=r^{p},$ $1\leq p<\infty$, then $L^{\Phi}(\mathrm{R}^{n})=L^{\mathrm{p}}(\mathrm{R}^{n})$

.

If $\Phi(r)=0(0\leq r\leq 1),$$=+\infty(\Gamma>$

1), then $L^{\Phi}(\mathrm{R}^{n})=L^{\infty}(\mathrm{R}^{n})$. If $\Phi\approx\Psi$, then $L^{\Phi}(\mathrm{R}^{n})=L^{\Psi}(\mathrm{R}^{n})$ with equivalent

norms.

We notethat

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Theor$e\mathrm{m}2.1$ ([24, p.77, Corollary 5 and Propositopn 6]). Let $\Phi$ be a Young

function.

Then the follouying

are

equivalent.

(1) $\Phi\in\Delta_{2}$.

(2) $L^{\Phi}(\mathrm{R}^{n})=M^{\Phi}(\mathrm{R}^{n})$

.

(3) For all $f\in L^{\Phi}(\mathrm{R}^{n})$ with $f\not\equiv \mathrm{O}$,

$\int_{\mathrm{R}^{n}}\Phi(\frac{|f(x)|}{||f||_{L^{\bullet}}})dx=1$

.

Theorem 2.2 ([7, Theorem 1.2.1]). Let$\Phi\in \mathcal{Y}$. Then the following are equivalent:

(1) $\Phi\in\nabla_{2}$

.

(2) The Hardy-Littlewood maximal operatoris bounded on $L^{\Phi}(\mathrm{R}^{n})$

.

The H\"older’s inequality isgeneralized to Orlicz spaces as follows.

Theorem 2.3 ([30]). For a Young

hnction

$\Phi$ and its complementary

function

$\overline{\Phi}$

,

$\int_{\mathrm{R}^{\hslash}}|f(x)g(x)|dx\leq 2||f||_{L^{\mathrm{B}}}||g||_{L^{\bullet}}-$

.

Theorem 2.4 ([20, Theorem 2.3]).

If

there exists a constant$c>0$ such that

$\Phi_{1}^{-1}(r)\Phi_{3}^{-1}(r)\leq c\Phi_{2}^{-1}(r)$

for

all$r\geq 0$,

then

$||fg||_{L^{l_{2}}}\leq 2c||f||_{L^{\bullet}1}||g||_{L^{\bullet}s}$.

Theorem 2.5 ([24, p.110, Theorem 7]). Let $\Phi\in \mathcal{Y}$

.

Then

$(M^{\Phi}(\mathrm{R}^{\mathfrak{n}}))^{*}=L^{\tilde{\Phi}}(\mathrm{R}^{n})$ ,

$||g||_{(M^{\bullet})^{*}}\sim||g||_{L^{\bullet}}-$.

Next we recall the definition ofMorrey spaces. Let $B(a, r)$ be the ball

{

$x\in \mathrm{R}^{n}$ :

$|x-a|<r\}$ with center $a$ and ofradius $r>0$

.

Deflnition 2.2 (Morrey space). For $1\leq p<\infty$ and $0\leq\lambda\leq n$, let

$L^{p,\lambda}(\mathrm{R}^{n})=\{f\in L_{1\mathrm{o}\mathrm{c}}^{p}(\mathrm{R}^{n}):||f||_{L^{\mathrm{p}.\lambda}}<+\infty\}$, $||f||_{L^{\mathrm{p},\lambda}}= \sup_{B=B(a,t)}(\frac{1}{r^{\lambda}}\int_{B}|f(x)|^{\mathrm{p}}dx)^{1/\mathrm{p}}$

Then $L^{p,\lambda}(\mathrm{R}^{n})$ is a Banach space. If $\lambda=0$, then $L^{\mathrm{p},\lambda}(\mathrm{R}^{n})=L^{p}(\mathrm{R}^{n})$. If $\lambda=n$,

(6)

If $1/p_{1}+1/p_{3}=1/p_{2}$ and $\lambda_{1}/p_{1}+\lambda_{3}/p_{3}=\lambda_{2}/p_{2}$, then we can get by H\"older’s

inequality

(2.2)

11

$fg||_{L^{P2}},x_{2}\leq 11f||_{L^{\mathrm{p}_{1},\lambda_{1}}}||g||_{L^{\mathrm{p}_{3},\lambda_{3}}}$

.

It is known that, if $1\leq p<q<\infty$ and $0\leq\lambda<n$, then there exists a function

$f\in L^{\mathrm{p},\lambda}(\mathrm{R}^{n})$ such that $f\not\in L^{q,\mu}(\mathrm{R}^{n})$ for all $0\leq\mu\leq n$. For preduals of Morrey

spaces, see [8].

Let $\mathcal{G}$ be the set of all functions $\phi$ : $(0, +\infty)arrow(0, +\infty)$ such that $\phi$ is almost

decreasing and $\phi(r)r$ is almost increasing. If $\phi\in \mathcal{G}$, then $\phi$ satisfies doubling

condition.

Proposition 2.6.

If

$\phi\in \mathcal{G}$, then there exists $\overline{\phi}\in \mathcal{G}$ such that$\overline{\phi}\sim\phi$ and that 5 is

continuous and strictly decreasing.

Deflnition 2.3 (generalized Morrey space). For $1\leq p<\infty$ and $\phi\in \mathcal{G}$, let

$L^{(\mathrm{p},\phi)}(\mathrm{R}^{n})=\{f\in L_{1\mathrm{o}\mathrm{c}}^{p}(\mathrm{R}^{n}):||f||_{L^{(\mathrm{p},\phi)}}<+\infty\}$,

$||f||_{L^{(\mathrm{p},\phi)}}= \sup_{B}(\frac{1}{|B|\phi(|B|)}\int_{B}|f(x)|^{p}dx)^{1/\mathrm{p}}$

Then $L^{(p,\phi)}(\mathrm{R}^{\mathfrak{n}})=L^{p,\lambda}(\mathrm{R}^{n})$ for $\phi(r)=r^{\lambda-n}$

.

3. ORLICZ-MORREY SPACES

Now

we

deflne Orlicz-Morrey spaces. For $\Phi\in \mathcal{Y},$ $\phi\in \mathcal{G}$ and aball $B$, let

IIflle,th,$B= \inf\{\lambda>0:\frac{1}{|B|\phi(|B|)}\int_{B}\Phi(\frac{|f(x)|}{\lambda})dx\leq 1\}$

Deflnition 3.1 (Orlicz-Morrey space). For $\Phi\in \mathcal{Y}$ and $\phi\in \mathcal{G}$, let

$L^{(\Phi,\phi)}(\mathrm{R}^{n})=$

{

$f\in L_{1\mathrm{o}\mathrm{c}}^{1}(\mathrm{R}^{n})$ :

lIfll

$L^{(\bullet,\phi)}<+\infty$

},

$||f||_{L^{(\bullet,\phi)}}= \sup_{B}||f||_{\Phi,\phi,B}$

.

Then $||\cdot||_{L^{\langle 3.\phi)}}$ is a norm and $L^{(\Phi,\phi)}(\mathrm{R}^{n})$ is a Banach space, since llflle,th,$B=$

Ilfll

$L^{b}(B,\overline{d}x)$ is a norm on the Orlicz space

$L^{\Phi}(B,\overline{d}x)$where $\overline{d}x=dx/(|B|\phi(|B|)))$

.

Bythe definition wehavethe following.

Proposition 3.1.

If

$\phi(r)=1/r$, then $L^{(\Phi,\phi)}(\mathrm{R}^{n})$ coincides utth the Orlicz space

$L^{\Phi}(\mathrm{R}^{n})$. $If\Phi(r)=r^{\mathrm{p}}$ and $\phi(r)=r^{-1+\lambda/n}(0\leq\lambda\leq n)$, then $L^{(\Phi,\phi)}(\mathrm{R}^{n})$ coincides

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Proposition 3.2. Let$\Phi,$$\Psi$ be Young

functions

and let$\phi,\psi\in \mathcal{G}$

.

(1)

If

$\Phi(r)\leq\Psi(Cr)$, then

$L^{(\Phi,\phi)}(\mathrm{R}^{n})\supset L^{(\Psi,\phi)}(\mathrm{R}^{n})$, $||f||_{L^{(8,\phi)}}\leq C||f||_{L^{(\Psi,\phi)}}$

.

(2)

If

$\phi(r)\leq C\psi(r)$, then

$L^{(\Phi,\phi)}(\mathrm{R}^{n})\subset L^{(\Phi,\psi)}(\mathrm{R}^{n})$, $\max(1, C)||f||_{L13,\phi)}\geq||f||_{L^{(\bullet,\psi)}}$.

Therefore, if$\Phi\approx\Psi$ and $\phi\sim\psi$, then $L^{(\Phi,\phi)}(\mathrm{R}^{n})=L^{(\Psi,\psi)}(\mathrm{R}^{n})$

.

Proposition 3.3. Let$\Phi\in \mathcal{Y}$ and $\phi\in \mathcal{G}$.

(1)

If

$\mathrm{q}_{\mathrm{I}}=\sup_{u>0}\phi(u)<+\infty$, then

$L^{(\Phi,\phi)}(\mathrm{R}^{n})\subset L^{\infty}(\mathrm{R}^{n})$ and $||f||_{L\infty}\leq\Phi^{-1}(\mathrm{q}_{1})||f||_{L^{(\bullet,\phi)}}$ .

(2)

If

$c_{1}= \inf_{u>0}\phi(u)>0$, then

$L^{(\Phi,\phi)}(\mathrm{R}^{n})\supset L^{\infty}(\mathrm{R}^{n})$ and $||f||_{L\infty}\geq\Phi^{-1}(c_{1})||f||_{L^{(\bullet,\phi)}}$.

Therefore, if$\phi\sim 1$, then $L^{(\Phi,\phi)}(\mathrm{R}^{n})=L^{\infty}(\mathrm{R}^{n})$ with equivalent

norms.

4. BASIC PROPERTIES

Theor$e\mathrm{m}4.1$

.

Let $\Phi_{i}$ be Young

functions

and $\emptyset:\in \mathcal{G},$ $i=1,2,3$

.

Assume that

there exists a constant $c>0$ such that

$\Phi_{1}^{-1}(r\phi_{1}(s))\Phi_{3}^{-1}(r\phi_{3}(s))\leq c\Phi_{2}^{-1}(r\phi_{2}(s))$

for

$r,$$s>0$

.

If

$f\in L^{(\Phi_{1},\phi_{1})}(\mathrm{R}^{n})$ and$g\in L^{(\Phi_{3},\phi_{\theta})}(\mathrm{R}^{n})$, then $fg\in L^{(\Phi_{2},\phi_{2})}(\mathrm{R}^{n})$ and $||fg||_{L^{\{\partial_{2\prime}\phi_{2})}}\leq 2c||f||_{L^{(C_{1\prime}\phi_{1})}}||g||_{L^{(\partial_{3\prime}\phi_{3})}}$.

Corollary 4.2. Let $\Phi_{2}$ be Youngfunctions, $i=1,2,3$, and $\phi\in \mathcal{G}$

.

Assume that

there enists a constant $c>0$ such that

$\Phi_{1}^{-1}(r)\Phi_{3}^{-1}(r)\leq c\Phi_{2}^{-1}(r)$

for

$r>0$.

If

$f\in L^{(\Phi_{1},\phi)}(\mathrm{R}^{n})$ and$g\in L^{(\Phi_{3},\phi)}(\mathrm{R}^{n})$, then$f_{\mathit{9}}\in L^{(\Phi_{2},\phi)}(\mathrm{R}^{n})$ and $||fg||_{L^{(\epsilon_{2},\phi)}}\leq 2c||f||_{L^{(\bullet_{1}.\phi)}}||g||_{L^{(\bullet}\mathrm{s}^{\phi)}},$ .

(8)

Corollary 4.3 ([13, 14]). Let $1\leq p:<\infty$ and $\phi_{*}\in \mathcal{G},$ $i=1,2,3$

.

Assume that

$1/p_{1}+1/p_{3}=1/p_{2}$ and that there ezzsts a constant $c>0$ such that

$\phi_{1}^{1/p_{1}}(r)\phi_{3}^{1/p\mathrm{a}}(r)\leq c\phi_{2}^{1/p_{2}}(r)$

for

$r>0$

.

If

$f\in L^{(p_{1},\phi_{1})}(\mathrm{R}^{n})$ and$g\in L^{(p_{3},\phi_{3})}(\mathrm{R}^{n})$, then $fg\in L^{(p_{2},\phi_{2})}(\mathrm{R}^{n})$ and $||fg||_{L^{(\mathrm{p}_{2\prime}\phi_{2})}}\leq 2c||f||_{L^{(_{\mathrm{P}1},\phi_{1})}}||g||_{L^{(\mathrm{p}_{3},\phi_{3})}}$

.

Theorem 4.4. Let$\Phi_{1}\in \mathcal{Y}$ and$\emptyset:\in \mathcal{G},$ $i=1,2$

.

Assume that

$\Phi_{2}(r)\Phi_{2}(s)\leq \mathrm{c}_{0}\Phi_{2}(rs)$

for

$r>0,$ $s>0$,

and that there $e$vists $\Phi_{3}\in \mathcal{Y}$ such that

$\Phi_{1}^{-1}(r)\Phi_{3}^{-1}(r)\leq c_{1}\Phi_{2}^{-1}(r)$ and $\phi_{1}(r)/\Phi_{2}(\Phi_{3}^{-1}(\phi_{1}(r)))\leq\alpha\phi_{2}(r)$

for

$r>0$

.

Then

$L^{(\Phi_{1},\phi_{1})}(\mathrm{R}^{n})\subset L^{(\Phi_{2},\phi_{2})}(\mathrm{R}^{n})$ and

$||f||_{L^{(l_{2},\phi_{2})}} \leq 2\max(1,\mathrm{q})c_{1}\max(1, c_{2})||f||_{L(\mathrm{a}_{1}.\phi_{1})}$

.

Corollary 4.5. Let $1\leq q\leq p<\infty$ and$\phi\in \mathcal{G}$

.

Then

$L^{(\mathrm{p},\phi)}(\mathrm{R}^{n})\subset L^{(q,\phi^{q/\mathrm{p}})}(\mathrm{R}^{n})$ and

$||f||_{L^{(q}},’ q/\mathrm{p}_{)}\leq||f||_{L^{(\mathrm{p},i)}}$

.

Corollary 4.6. Let$\Phi\in \mathcal{Y}$ and $\phi\in \mathcal{G}$. Then $\Phi^{-1}(\phi)\in \mathcal{G}$ and

$L^{(\Phi,\phi)}(\mathrm{R}^{n})\subset L^{(1,\Phi^{-1}(\phi))}(\mathrm{R}^{n})$ and

$||f||_{L^{(1,3^{-1_{(\phi))}}}}\leq||f||_{L^{(\bullet,\phi)}}$.

Corollary 4.7 ([17]). Let$\Phi\in \mathcal{Y}$ and $\emptyset(r)=\Phi^{-1}(1/r)$. Then $\phi\in \mathcal{G}$ and $L^{\Phi}(\mathrm{R}^{n})\subset L^{(1,\phi)}(\mathrm{R}^{n})$ and $||f||_{L^{(1,\phi)}}\leq C||f||_{L}\Leftrightarrow$

.

Theor$e\mathrm{m}4.8$

.

Let $\Phi,$$\Psi$ $\in \mathcal{Y},$ $\phi\in \mathcal{G}$ and $\phi(r)$ $arrow+\infty$ as $rarrow 0$

.

If

$\lim_{rarrow+\infty}\Phi^{-1}(r)/\Psi^{-1}(r)=+\infty$, then there exists a

function

$f\in L^{(\Phi,\phi)}(\mathrm{R}^{n})$ with

compact support such that $f\not\in L^{(\Psi,\psi)}(\mathrm{R}^{n})$

for

$dl\psi\in \mathcal{G}$

.

Corollary 4.9. Let $1\leq p<q<\infty,$ $\phi\in \mathcal{G}$ and$\phi(r)arrow+\infty$ as $rarrow \mathrm{O}$

.

Then there

exists a

function

$f\in L^{p,\phi}(\mathrm{R}^{n})$ urith compact supportsuch that $f\not\in L^{q,\psi}(\mathrm{R}^{n})$

for

all $\psi\in \mathcal{G}$.

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5. PREDUAL

Definition 5.1. Let $\Phi\in \mathcal{Y}$ and $\phi\in \mathcal{G}$

.

A function$b$ on $\mathrm{R}^{n}$ is called a $(\Phi, \phi)$-block

if there exists aball $B$ such that

$\{_{(iii)}^{(i)}(ii)$ $\int^{\sup}B\Phi,(k|b(x)’|)dx<+,\infty||b||_{\Phi\phi,B}\leq \mathrm{p}b\subset\overline{B}\frac{1}{|B|\phi(|B|)}$ for all

$k>0$,

where $\overline{B}$

is the closure of$B$

.

Let $\mathfrak{D}’$ be the space of distributions

on

$\mathrm{R}^{n}$

.

Definition 5.2. Let $\Phi\in \mathcal{Y}$ and $\phi\in \mathcal{G}$. We deflne the space $B_{(\Phi,\phi)}(\mathrm{R}^{n})\subset \mathfrak{D}’$ as

follows:

$f\in B_{(\Phi,\phi)}(\mathrm{R}^{n})$ if andonly ifthereexist sequences $(\Phi, \phi)$-blo&s $\{b_{j}\}$

and positive numbers $\{\lambda_{j}\}$ suchthat

(5.1) $f= \sum_{\mathrm{j}}\lambda_{j}b_{j}$in $\mathfrak{D}’$ and $\sum_{j}\lambda_{j}<+\infty$

.

$||f||_{B_{(\bullet.\phi)}}= \inf\{\sum_{j}\lambda_{j}$ : $f= \sum_{j}\lambda_{j}b_{j}$ in $\mathfrak{D}^{j}\}$ ,

Then $B_{(\Phi,\phi)}(\mathrm{R}^{n})$ is a Banach space.

Theorem 5.1. Let$\Phi\in \mathcal{Y}$ and$\phi\in \mathcal{G}$

.

Assume that $\tilde{\Phi}\in \mathcal{Y}$. Then

$(B_{(\Phi,\phi)}(\mathrm{R}^{\mathfrak{n}}))^{*}=L^{(\tilde{\Phi},\phi)}(\mathrm{R}^{n})$

.

Moreprecisely,

for

$\mathit{9}\in L^{(\tilde{\Phi},\phi)}(\mathrm{R}^{n})$, there exists a linear

functiond

$L$ given by

(5.2) $L(f)= \int_{\mathrm{R}^{n}}f(x)g(x)dx$

for

$f\in M_{\infty \mathrm{m}\mathrm{p}}^{\Phi}(\mathrm{R}^{n})$,

and

satisfies

$||L||\leq c||g||_{L\mathrm{t}^{-}}\bullet,\phi)$

.

Conversely, every linear jfunctional $L$ on $B_{(\Phi,\phi)}(\mathrm{R}^{\mathfrak{n}})$ can be realized as (5.2), uyith

$g\in L^{(\tilde{\Phi},\phi)}(\mathrm{R}^{n})$, and with

(10)

Lemma 5.2. Let $f\in M_{\infty \mathrm{m}_{\mathrm{P}}}^{\Phi}(\mathrm{R}^{n})$ and $f= \sum_{j}\lambda_{j}b_{j}$ be any decomposition in

$B_{(\Phi,\phi)}(\mathrm{R}^{n})$. Then

(5.3) $\int_{\mathrm{R}^{\mathfrak{n}}}f(x)g(x)dx=\sum_{j}\lambda_{j}\int_{\mathrm{R}^{n}}b_{j}(x)g(x)dx$,

for

all$g\in L^{(\tilde{\Phi},\phi)}(\mathrm{R}^{n})$

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DEPARTMENT OF MATHEMATICS, OSAKA KYOIKU UNIVERSITY, KASHIWAHA, OSAKA

582-8582, JAPAN

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