1 Introduction
Let
$X=(X,d,\mu )$
be a metric measure space, where X is a bounded set, d is a metric on X and
$\mu $
is a nonnegative complete Borel regular outer measure on X which is finite in every bounded set. For
$x \in X$
and
$r>0$
, we denote the open ball in X by
$B(x,r)=\{y \in X: d(x,y)<r \}$
. Let
$d_{X}:=\mathrm {diam} X=\sup \{d(x,y) : x, y \in X \}$
. Suppose that
$d_X<\infty $
,
$ \mu (\{x\}) = 0 $
for
$x \in X$
and
$\mu (B(x,r))>0$
for
$x \in X$
and
$r> 0$
.
As in [Reference Ohno and Shimomura18], we do not assume that
$\mu $
satisfies the doubling condition. We say that a Radon measure
$\mu $
is doubling if there exists a constant
$c_0>0$
such that
$\mu (B(x,2r)) \le c_0 \mu (B(x,r))$
for all
$x \in \mathrm {supp}(\mu )(=X)$
and
$r>0$
. If this does not follow, then we say that
$\mu $
is non-doubling. Let
$Q(\cdot )$
be a measurable function on X such that
Suppose that
$\mu $
is lower Ahlfors
$Q(x)$
-regular, that is, there exists a constant
$A>0$
such that
for all
$x\in X$
and
$0< r< d_X$
[Reference Björn and Björn2, Reference Harjulehto, Hästö and Latvala6]. Note from [Reference Björn and Björn2, Lemma 3.3] that if
$\mu $
satisfies the doubling condition and
$d_{X}<\infty $
, then
$\mu $
is lower Ahlfors
$\log _2 c_0$
-regular. We refer to [Reference Ohno and Shimomura15, Reference Sawano and Shimomura21] for non-doubling measure spaces.
Example 1.1 Let
$X_1=\{x=(x_1,0) \in \mathbf {{R}}^2 : 0< x_1< 1\}$
and
$X_2=\{x=(x_1,x_2) \in \mathbf {{R}}^2 : x_1 \le 0, x_1^2+x_2^2< 1\}$
and define
$(X,d,\mu )=(X_1,d_2,m_1)\cup (X_2,d_2,m_2)$
, where
$d_2$
denotes the
$2$
-dimension Euclidean distance and
$m_i$
denotes the i-dimension Lebesgue measure. Then it is easy to show that
$\mu $
is non-doubling and
for all
$x\in X$
and
$0<r\le 2$
, where
$Q(x)=1$
on
$X_1$
and
$Q(x)=2$
on
$X_2$
.
Let
$\alpha (\cdot )$
be a measurable function on X such that
To obtain results for Sobolev functions as an application, as in [Reference Ohno and Shimomura18], we consider the Riesz potential
$J_{\alpha (\cdot ), \tau }f$
of order
$\alpha (\cdot )$
for
$\tau \ge 1$
and a locally integrable function f on X by
$$\begin{align*}J_{\alpha(\cdot), \tau}f(x) = \sum_{2^i\le 2 d_X} \frac{2^{i\alpha(x)}}{\mu(B(x,\tau 2^i))} \int_{B(x,2^i)} f(y)\, d\mu(y) \end{align*}$$
[Reference Hajłasz and Koskela4, Reference Harjulehto, Hästö and Latvala6].
We have long been interested in extending the classical Trudinger inequality [Reference Trudinger26] to various function spaces. In the previous paper [Reference Ohno and Shimomura18], we studied Trudinger-type inequalities for
$J_{\alpha (\cdot ), \tau }f$
of functions in Musielak–Orlicz spaces
$L^{\Phi }(X)$
over bounded metric measure spaces equipped with lower Ahlfors
$Q(x)$
-regular measures, as an extension of [Reference Hajłasz and Koskela4, Theorem 5.3] for the
$L^p$
case and [Reference Harjulehto, Hästö and Latvala6, Theorem 4.8] for the
$L^{p(\cdot )}$
case.
In this article, we give a Trudinger-type inequality for
$J_{\alpha (\cdot ), \tau }f$
(Theorem 4.3) by using Hedberg’s method [Reference Hedberg8], as an extension of [Reference Ohno and Shimomura18, Theorem 3.6]. For this, see Remark 4.4. Our new idea is to investigate the integrability of the modified maximal function
(see Section 3), Corollarly 3.9, using the boundedness of
$M_{\lambda }$
on
$L^{\Phi }(X)$
, Theorem 3.6. We show Theorem 3.6, which is an improvement of [Reference Ohno and Shimomura18, Lemma 3.1], by relaxing the comparing condition
$(\Phi 5;\nu )$
in [Reference Ohno and Shimomura18] by
$(\Phi 5;Q)$
given in Section 2. The goodness of condition
$(\Phi 5;Q)$
will be discussed in Remark 2.1.
The various problems of double phase functionals introduced by Zhikov [Reference Zhikov27] have been a very active topic since the work of Mingione and collaborators [Reference Baroni, Colombo and Mingione1, Reference Colombo and Mingione3]. In Section 5, as one of important special cases of
$\Phi $
, we obtain Trudinger-type inequalities for double phase functionals
$\Phi (x,t) = t^{p(x)} + a(x) t^{q(x)}$
(Corollary 5.1), as an extension of [Reference Ohno and Shimomura18, Corollary 4.2]. See Remarks 5.2 and 5.3.
Finally, in Section 6, as an application of the result for
$J_{\alpha (\cdot ), \tau }f$
, we discuss Trudinger-type inequalities for Sobolev functions (Theorem 6.1 and Corollary 6.3). Our results extend [Reference Ohno and Shimomura18, Theorem 5.1 and Corollary 5.2] as seen in Remarks 6.2 and 6.4.
Throughout the article, we let C denote various constants independent of the variables in question and
$C(a,b,\cdots )$
be a constant that depends on
$a,b,\ldots $
only.
2 Musielak–Orlicz spaces
We consider a function
satisfying conditions (
$\Phi $
1)–(
$\Phi $
3):
-
(Φ1)
$\Phi (\cdot , t)$
is measurable on X for each
$t \ge 0$
and
$\Phi (x,\cdot )$
is continuous on
$[0, \infty )$
for each
$x \in X$
; -
(Φ2) there exists a constant
$A_1 \ge 1$
such that
$$ \begin{align*}A_1^{-1} \le \Phi (x,1) \le A_1 \quad \text{for all} \ x \in X;\end{align*} $$
-
(Φ3)
$t \mapsto \Phi (x,t)/t$
is uniformly almost increasing on
$(0, \infty )$
, namely there exists a constant
$A_2 \ge 1$
such that
$$ \begin{align*}\Phi(x,t_1)/t_1 \le A_2 \Phi(x,t_2)/t_2 \quad \text{for all} \ x \in X \ \text{whenever} \ 0 < t_1 < t_2.\end{align*} $$
(
$\Phi 2$
) and (
$\Phi 3$
) yield
Set
$\bar {\phi }(x,t) = \sup _{0 < s \le t} \{\Phi (x,s)/s\}$
and
$\overline {\Phi }(x,t) = \int _0^t \bar {\phi }(x,r)\, dr$
for
$x \in X$
and
$t \ge 0$
. Then
$\overline {\Phi }(x, \cdot )$
is convex and
for all
$x \in X$
and
$t \ge 0$
. Note that (
$\Phi 3$
) is used to check the second inequality.
Recall that f is a locally integrable function on X if f is an integrable function on all balls B in X. Given
$\Phi (x,t)$
satisfying (
$\Phi $
1)–(
$\Phi $
3), the Musielak–Orlicz space
$L^{\Phi }(X)$
, also called the generalized Orlicz spaces [Reference Harjulehto and Hästö5], is defined as
The space
$L^{\Phi }(X)$
is a Banach space with respect to the norm
Further, consider the following conditions for
$\Phi (x,t)$
: Let
$p \ge 1$
be given.
-
(Φ3; p)
$t \mapsto t^{-p}\Phi (x,t)$
is uniformly almost increasing on
$(0,\infty )$
, namely there exists a constant
$A_{2,p} \ge 1$
such that
$$ \begin{align*}t_1^{-p} \Phi(x,t_1) \le A_{2,p}\, t_2^{-p}\, \Phi(x,t_2) \quad \text{for all} \ x \in X \ \text{whenever} \ 0 < t_1 < t_2 ;\end{align*} $$
-
(Φ5; Q) for every
$\gamma>0$
, there exists a constant
$B_{\gamma , Q} \ge 1$
such that whenever
$$ \begin{align*}\Phi(x,t) \le \Phi(y,B_{\gamma, Q}t)\end{align*} $$
$x\in X$
,
$0<r\le d_X$
,
$y\in B(x,r)$
,
$\Phi (x,t) \le \gamma r^{-Q(x)}$
and
$t \ge 1$
.
Here we will remark on
$(\Phi 5;Q)$
.
Remark 2.1 In [Reference Ohno and Shimomura18], we considered the following: Let
$q \ge 1$
and
$\nu>0$
be given.
-
(Φ3; ∞; q)
$t \mapsto t^{-q}\Phi (x,t)$
is uniformly almost increasing on
$[1, \infty )$
, namely there exists a constant
$A_{2,\infty ,q} \ge 1$
such that
$$ \begin{align*}t_1^{-q}\Phi(x,t_1) \le A_{2,\infty,q}\, t_2^{-q}\Phi(x,t_2) \quad \text{for all} \ x \in X \ \text{whenever} \ 1 \le t_1 < t_2 ;\end{align*} $$
-
(Φ5; ν) for every
$\gamma>0$
, there exists a constant
$\tilde {B}_{\gamma , \nu } \ge 1$
such that whenever
$$ \begin{align*}\Phi(x, t) \le \tilde{B}_{\gamma, \nu} \Phi(y,t)\end{align*} $$
$x, y \in X$
,
$d(x,y) \le \gamma t^{-\nu }$
and
$t \ge 1$
.
If
$\Phi (x,t)$
satisfies
$(\Phi 5;\nu )$
with
$\nu>0$
satisfying
$\nu \le q/Q^+$
, then it satisfies
$(\Phi 5;Q)$
.
We will show this. For
$\gamma>0$
, let
$x\in X$
,
$0<r\le d_X$
,
$y \in B(x,r)$
,
$\Phi (x,t) \le \gamma r^{-Q(x)}$
and
$t \ge 1$
. By
$(\Phi 3;\infty ;q)$
, (
$\Phi $
2) and (1.1)
Since
$\nu \le q/Q^+$
,
$1 \le t\le Cr^{-1/\nu } \le C d(x,y)^{-1/\nu }$
, so that
$ d(x,y) \le \gamma ' t^{-\nu } $
and
$t \ge 1$
. Hence, by
$(\Phi 5;\nu )$
, there exists a constant
$B_{\gamma ',\nu } \ge 1$
such that
Taking
$B_{\gamma } \ge A_2 B_{\gamma ',\nu } (\ge 1)$
, it follows from (2.3) and
$(\Phi 3)$
that
Thus
$\Phi (x,t)$
satisfies
$(\Phi 5;Q)$
.
We define
$L_{e}(t) = \log (e + t)$
,
$L_{c}^{(1)}(t) = L_c(t)$
and
$L_{c}^{(j+1)}(t) = L_c( L_c^{(j)}(t))$
. As in [Reference Ohno and Shimomura18], typical examples to apply our theorems are for example
$$ \begin{align*}\Phi_{1}(x,t) = t^{p(x)} \prod_{j=1}^k \big( L_{e}^{(j)}(t) \big)^{q_j(x)} \ \text{and} \ \Phi_2(x,t) = t^{p(x)} + a(x) t^{q(x)} \end{align*} $$
under suitable
$p(\cdot ), q(\cdot ), q_j(\cdot )$
and
$a(\cdot )$
. For
$\Phi _2$
, see [Reference Colombo and Mingione3, Reference Maeda, Mizuta, Ohno and Shimomura11, Reference Ragusa and Tachikawa19].
3 The maximal operator
The following lemma is from [Reference Maeda, Mizuta, Ohno and Shimomura10, Lemma 5.1].
Lemma 3.1 Let
$F(x,t)\ {:}\ X \times (0, \infty ) \to [0, \infty )$
. Consider the following conditions:
-
(F1)
$F(x,\cdot )$
is continuous on
$(0, \infty )$
for each
$x \in X;$
-
(F2) there exist constants
$\hat {t}>0$
and
$K_1 \ge 1$
such that
$K_1^{-1} \le F(x,\hat {t}) \le K_1$
for all
$x \in X;$
-
(F3)
$t \mapsto t^{-\varepsilon }F(x,t)$
is uniformly almost increasing for
$\varepsilon>0;$
namely there exists a constant
$K_2 \ge 1$
such that
$t^{-\varepsilon }F(x,t) \le K_2 s^{-\varepsilon }F(x,s)$
for all
$x \in X$
whenever
$0 < t < s$
.
Set
$F^{-1}(x,s) = \sup \{t>0; F(x,t) < s \}$
for
$x \in X$
and
$s>0$
.
-
(1)
$F^{-1}(x, \cdot )$
is non-decreasing on
$(0, \infty )$
. -
(2) If
$F(x,t)$
satisfies (F3), then
$F^{-1}(x,\lambda s) \le (K_2 \lambda )^{1/\varepsilon } F^{-1}(x,s)$
for all
$x \in X$
,
$s>0$
and
$\lambda \ge 1$
. -
(3) If
$F(x,t)$
satisfies (F1), then
$F(x,F^{-1}(x,t)) = t$
for all
$x \in X$
and
$t>0$
with
$0<F^{-1}(x,t)<\infty $
. -
(4) If
$F(x,t)$
satisfies (F3), then
$K_2^{-1/\varepsilon } t \le F^{-1}(x,F(x,t)) \le K_2^{2/\varepsilon } t$
for all
$x \in X$
and
$t>0$
with
$F(x,t)>0$
. -
(5) If
$F(x,t)$
satisfies (F2) and (F3), then for all
$$ \begin{align*} \min \left\{1, \left( \frac{s}{K_1 K_2} \right)^{1/\varepsilon} \right\}\hat{t} \le F^{-1}(x,s) \le \max \left\{1, (K_1 K_2 s)^{1/\varepsilon} \right\}\hat{t} \end{align*} $$
$x \in X$
and
$s>0$
.
Notice that
$F(x,t)=\Phi (x,t)$
satisfies (F1)–(F3) with
$K_1=A_1, K_2=A_2, \hat {t}=1$
and
$\varepsilon =1$
.
Given a locally integrable function f on X and
$\lambda \ge 1$
, the Hardy–Littlewood maximal function
$M_{\lambda }f$
is defined by
Given
$\lambda \ge 1$
, we say that X satisfies (
$M \lambda $
) if there exists a constant
$C>0$
such that
for all measurable functions
$f\in L^{1}(X)$
and
$k>0$
.
Remark 3.2 Note from [Reference Heinonen9] that X satisfies (
$M \lambda $
) for any
$\lambda>0$
whenever
$\mu $
satisfies the doubling condition. By the Vitali covering theorem, Nazarov, Treil, and Volberg [Reference Nazarov, Treil and Volberg13] showed that X satisfies (
$M 3$
) if X is a separable metric space. Sawano [Reference Sawano20] proved that X satisfies (
$M \lambda $
) for
$\lambda \ge 2$
if X is a separable metric space. In [Reference Terasawa25], Terasawa showed that X satisfies (
$M \lambda $
) for
$\lambda \ge 2$
if
$\mu (B(x,r))$
is continuous in the variable
$r>0$
when
$x\in X$
is fixed. We find another remarkable example of the Poincaré disc in [Reference Strömberg24] where (3.1) with
$\lambda =1$
is established even though the corresponding Riemannian volume
$\mu $
is non-doubling. In [Reference Hashimoto, Sawano and Shimomura7, Appendix], it was shown that the Euclidean space
$\mathbf {{R}}^N$
, endowed with
$\mu \equiv e^{|x|^2}\,dx$
, fails to satisfy
$(M1)$
.
The following lemma is known (see [Reference Sawano and Shimomura22, Lemma 2.1]).
Lemma 3.3 Let
$1<p_0<\infty $
and let
$\lambda \ge 1$
. Suppose that X satisfies (
$M \lambda $
). Then there exists a constant
$C>0$
such that
for all measurable functions f on X with
$\| f\|_{L^{p_0}(X)} \le 1$
.
Remark 3.4 As a classical result, it is well known that the boundedness of
$M_{1}$
on
$L^{p_0}(X)$
is proved by using (3.1) with
$\lambda =1$
(see Setin [Reference Stein23, Chapter 1 and Theorem 1] and Heinonen [Reference Heinonen9, Theorem 2.2]). Hence, (
$M \lambda $
) is the natural assumption to prove the boundedness of
$M_{\lambda }$
on
$L^{\Phi }(X)$
in our setting.
For
$p\ge 1$
and
$\lambda \ge 1$
, set
and
We show the following lemma instead of [Reference Ohno and Shimomura16, Lemma 3.3].
Lemma 3.5 Let
$\lambda \ge 1$
. Let
$\Phi (x,t)$
satisfy
$(\Phi 3;p)$
and
$(\Phi 5;Q)$
for
$p \ge 1$
. Then, given
$L \ge 1$
, there exist constants
$C_1 = C(L) \ge 2$
and
$C_2>0$
such that
for all
$x \in X$
,
$0<r\le d_X$
and for all nonnegative measurable functions f on X such that
$f(y) \ge 1$
or
$f(y)=0$
for each
$y \in X$
and
Proof Let f be as in the statement of this lemma and let
$x \in X$
and
$0<r\le d_X$
. For simplicity, we set
$I = I(f;x,r,\lambda )$
and
$J = J(f;x,r,p,\lambda )$
. Hölder’s inequality gives
Since
$\Phi \left ( y, f(y) \right )^{1/p} \ge (A_1 A_{2,p})^{-1/p} f(y)$
for all
$y \in X$
by
$(\Phi 3;p)$
,
$I \le (A_1 A_{2,p})^{1/p} J$
. Hence, if
$J \le 1$
, then in view of
$(\Phi 3;p)$
and
$(\Phi 2)$
whenever
$C_1 \ge (A_1 A_{2,p})^{1/p}$
.
Let us consider the case
$J>1$
. Noting from
$(\Phi 3;p)$
that
$\Phi (x,t)^{1/p} \to \infty $
as
$t \to \infty $
, we see that there exists
$K> 1$
such that
Using this K, it follows from
$(\Phi 3;p)$
that
$$ \begin{align*} \int_{B(x,r)} f(y)\, d\mu(y) &= \int_{B(x,r) \cap \{y\in X: f(y)\le \beta K\}} f(y)\, d\mu(y)\\& \quad +\int_{B(x,r) \cap \{y\in X : f(y)>\beta K\}} f(y)\, d\mu(y) \\&\le \beta K \mu(B(x,r)) + A_{2,p}^{1/p}\beta K \int_{B(x,r)} \frac{\Phi \left( y, f(y) \right)^{1/p} }{\Phi (y,\beta K)^{1/p} }\, d\mu(y). \end{align*} $$
Let
$\gamma = A_1A^{-1} L$
. Owing to (
$\Phi 5;Q$
), there is
$\beta =\beta (\gamma ) \ge 1$
, independent of f, x, r, such that
for
$y \in B(x,r)$
, since
$K>1$
and
by (3.4),
$(\Phi 2)$
, and (3.3). Therefore
Since
$J \Phi (x, K)^{-1/p} = \Phi (x,1)^{-1/p} \le A_1^{1/p}$
by (3.4) and
$(\Phi 2)$
, we obtain
The rest is proved in line with the proof of [Reference Ohno and Shimomura16, Lemma 3.3].
Using Lemma 3.5, as in the proof of [Reference Ohno and Shimomura16, Theorem 3.2], we can prove the boundedness of
$M_{\lambda }$
on
$L^{\Phi }(X)$
, which is an improvement of [Reference Ohno and Shimomura18, Lemma 3.1] ([Reference Ohno and Shimomura16, Theorem 3.2]).
Theorem 3.6 Let
$\lambda \ge 1$
. Let
$\Phi (x,t)$
satisfy
$(\Phi 3;p)$
and
$(\Phi 5;Q)$
for
$p>1$
. Suppose that X satisfies
$(M \lambda )$
. Then there is a constant
$C>0$
such that
for all
$f \in L^{\Phi }(X)$
.
Remark 3.7 In [Reference Ohno and Shimomura16, Theorem 3.2], we showed the following boundedness of
$M_{\lambda }$
on
$L^{\Phi }(X)$
: Let
$\lambda \ge 1$
. Let
$\Phi (x,t)$
satisfy
$(\Phi 3;p)$
and
$(\Phi 5;\nu )$
for
$p>1$
and
$0<\nu \le p/Q^+$
. Suppose that X satisfies
$(M \lambda )$
. Then there is a constant
$C>0$
such that
for all
$f \in L^{\Phi }(X)$
.
Note from Remarks 2.1 and 5.4 that
$(\Phi 5;Q)$
is weaker than
$(\Phi 5;\nu )$
when
$0<\nu \le p/Q^+$
. Hence, Theorem 3.6 is an improvement of [Reference Ohno and Shimomura18, Lemma 3.1] [Reference Ohno and Shimomura16, Theorem 3.2].
Lemma 3.8 Let
$\lambda \ge 1$
. Let
$\Phi (x,t)$
satisfy
$(\Phi 3;p)$
and
$(\Phi 5;Q)$
for
$p>1$
. Suppose that X satisfies
$(M \lambda )$
. Then there is a constant
$C>0$
such that
for all
$0<\varepsilon \le 1$
,
$x\in X$
,
$0<r\le d_X$
and nonnegative
$f \in L^{\Phi }(X)$
with
$\|f\|_{L^{\Phi }(X)}\le 1$
.
Proof By Theorem 3.6, there exists a constant
$C_M \ge 1$
such that
Let f be a nonnegative measurable function with
$\|f\|_{L^{\Phi }(X)}\le 1/(2C_M)$
. Then we have by (2.2)
Let
$x\in X$
and
$0<r\le d_X$
. Set
$c_1= A_1A_2 \max \{1,d_X^{Q^{+}}\} \ (\ge 1)$
. Then we have by Lemma 3.1 (5)
$$ \begin{align*} \Phi^{-1}\left(x,c_1r^{-Q(x)}\right) &\ge \min \left\{1, (A_1 A_2)^{-1} c_1r^{-Q(x)}\right\} \\ &\ge \min \left\{1, (A_1 A_2)^{-1} c_1\min\left\{1,d_X^{-Q^{+}}\right\}\right\}= 1 \end{align*} $$
and by Lemma 3.1 (3)
so that, by
$(\Phi 5;Q)$
, there exists a constant
$\beta \ge 1$
such that
whenever
$y\in B(x,r)$
. We divide the integral into two parts as follows:
$$ \begin{align*} &\frac{1}{\mu(B(x,r))}\int_{B(x,r)} \{M_{\lambda}f(y)\}^{\varepsilon} \, d\mu(y) \\& \quad = \frac{1}{\mu(B(x,r))} \left( \int_{B(x,r) \cap \{y\in X: M_{\lambda}f(y)\le \beta\Phi^{-1}(x,c_1r^{-Q(x)})\}} \{M_{\lambda}f(y)\}^{\varepsilon}\, d\mu(y) \right. \\& \qquad\qquad\qquad\quad \left. +\int_{B(x,r) \cap \{y\in X : M_{\lambda}f(y)>\beta\Phi^{-1}(x,c_1r^{-Q(x)})\}} \{M_{\lambda}f(y)\}^{\varepsilon} \, d\mu(y) \right). \end{align*} $$
Since
$t \rightarrow t^{-\varepsilon } \Phi (y,t)$
is uniformly almost increasing on
$(0, \infty )$
by
$(\Phi 3)$
, we find from (1.2) and (3.5) that
$$ \begin{align*} &\frac{1}{\mu(B(x,r))}\int_{B(x,r)} \{M_{\lambda}f(y)\}^{\varepsilon} \, d\mu(y) \\& \quad \le \left\{\beta\Phi^{-1}\left(x,c_1r^{-Q(x)}\right)\right\}^{\varepsilon} +A_2\frac{1}{\mu(B(x,r))}\int_{B(x,r)}\{M_{\lambda}f(y)\}^{\varepsilon} \\& \qquad \times \frac{\{M_{\lambda}f(y)\}^{-\varepsilon}\Phi(y, M_{\lambda}f(y))} {\left\{\beta \Phi^{-1}\left(x,c_1r^{-Q(x)}\right)\right\}^{-\varepsilon}\Phi\left(y,\beta\Phi^{-1}\left(x,c_1r^{-Q(x)}\right)\right) } \, d\mu(y) \\& \quad \le C\Phi^{-1}\left(x,c_1r^{-Q(x)}\right)^{\varepsilon} \left\{1+\int_{X} \Phi(y, M_{\lambda}f(y))\, d\mu(y)\right\} \\& \quad \le C\Phi^{-1}\left(x,r^{-Q(x)}\right)^{\varepsilon}, \end{align*} $$
where C is independent of
$\varepsilon $
. Thus the proof is complete.
In view of Lemmas 3.8 and 3.1 (5), we obtain the following result.
Corollary 3.9 Let
$\lambda \ge 1$
and
$0<\varepsilon _1\le 1$
. Let
$\Phi (x,t)$
satisfy
$(\Phi 3;p)$
and
$(\Phi 5;Q)$
for
$p>1$
. Suppose that X satisfies
$(M \lambda )$
. Then there exist constants
$0<\varepsilon _2<\varepsilon _1$
and
$C>0$
independent of
$\varepsilon _1$
and
$\varepsilon _2$
such that
for all
$x\in X$
,
$0<r\le d_X$
and nonnegative
$f \in L^{\Phi }(X)$
with
$\|f\|_{L^{\Phi }(X)}\le 1$
.
Proof Let
$0<\varepsilon _1\le 1$
,
$x\in X$
and
$0<r\le d_X$
. Taking
$\varepsilon _2=\varepsilon _1/(1+Q^+)$
, by Lemma 3.1 (5), we find
4 Trudinger-type inequalities
Let E be a measurable subset of X. We set
$s_0 = \min \{1, 1/d_X\}$
. As in [Reference Ohno and Shimomura18], we consider a function
satisfying
-
(Γ1)
$s \mapsto \Gamma (x,s)$
is uniformly almost increasing on
$[s_0, \infty )$
, that is, there exists a constant
$c_{\Gamma 1}\ge 1$
such that for all
$$\begin{align*}\Gamma(x,s_1)\le c_{\Gamma 1}\Gamma(x,s_2) \end{align*}$$
$x\in E$
and
$s_0 \le s_1<s_2$
;
-
(Γ2) there exists a constant
$c_{\Gamma 2}\ge 1$
such that
$$\begin{align*}\Gamma(x,2)\le c_{\Gamma 2}\Gamma(x, s_0) \quad \text{for all} \ x \in E; \end{align*}$$
-
(Γlog) there exists a constant
$c_{\Gamma \ell }\ge 1$
such that for all
$$ \begin{align*} \Gamma(x,s^2) \le c_{\Gamma \ell}\Gamma (x,s) \end{align*} $$
$x\in E$
and
$s \ge 1$
.
We borrow the following lemma from [Reference Maeda, Mizuta, Ohno and Shimomura12, Lemma 3.1] to collect properties of the function
$\Gamma $
from (4.1).
Lemma 4.1
-
(1)
$\Gamma (x,\cdot )$
has uniform doubling property on
$[s_0, \infty );$
namely, there exists a constant
$C>0$
such that
$ \Gamma (x,2s)\le C\Gamma (x,s) $
for all
$x \in E$
and
$s \ge s_0$
. -
(2) For
$a>0$
, there exists a constant
$C\ge 1$
such that for all
$$\begin{align*}C^{-1}\Gamma(x,s)\le \Gamma(x,s^a)\le C\Gamma(x,s) \end{align*}$$
$x \in E$
and
$s \ge 1$
.
-
(3) There exists a constant
$C>0$
such that for all
$$\begin{align*}\Gamma(x,s) \le C s \Gamma(x,s_0) \end{align*}$$
$x \in E$
and
$s \ge s_0$
.
Further, we assume the following condition:
-
(ΓΦαQ) there exists a constant
$c^{**}_1 \ge 1$
such that for all
$$\begin{align*}\int_{\delta}^{d_X}\rho^{\alpha(x)}\Phi^{-1}\left(x,\rho^{-Q(x)}\right)\, \frac{d\rho}{\rho} \le c^{**}_{1} \Gamma(x,1/\delta) \end{align*}$$
$x \in E$
whenever
$0 < \delta \le d_X/2$
.
Notice that there exists a constant
$c_{\Gamma 3}>0$
such that
by
$(\Gamma \Phi \alpha Q)$
, (1.1) and Lemma 3.1 (5).
Here we prepare the following lemma using
$\Gamma $
.
Lemma 4.2 Let
$\tau \ge 1$
. Let
$\Phi (x,t)$
satisfy
$(\Phi 5;Q)$
. Suppose that
$(\Gamma \Phi \alpha Q)$
holds. Then there exists a constant
$C>0$
such that
$$ \begin{align} \sum_{2\delta<2^i\le 2 d_X} \frac{2^{i\alpha(x)}}{\mu(B(x,\tau 2^i))} \int_{B(x,2^i)} f(y)\, d\mu(y) \le C \Gamma(x,1/\delta) \end{align} $$
for all
$x\in E$
,
$0<\delta <d_{X}/2$
and nonnegative
$f \in L^{\Phi }(X)$
with
$\|f\|_{L^{\Phi }(X)}\le 1$
.
Proof Let f be a nonnegative measurable function with
$\|f\|_{L^{\Phi }(X)}\le 1/2$
. Let
$x\in E$
and
$0<\delta <d_{X}/2$
. Set
$c_1= A_1A_2 \max \{1,d_X^{Q^{+}}\} \ (\ge 1)$
. Just as we obtained (3.5), by
$(\Phi 5;Q)$
, we have
whenever
$0<t\le d_X$
and
$y\in B(x,t)$
.
By
$(\Phi 3)$
, (4.4), and (1.2)
$$ \begin{align} &\frac{t^{\alpha(x)}}{\mu(B(x,\tau t))}\int_{B(x,t)} f(y)\, d\mu(y) \nonumber \\& \quad \le \frac{t^{\alpha(x)}}{\mu(B(x,\tau t))}\int_{B(x,t)} \beta\Phi^{-1}\left(x,c_1t^{-Q(x)}\right) \, d\mu(y) \nonumber \\& \qquad + A_2\frac{t^{\alpha(x)}}{\mu(B(x,\tau t))}\int_{B(x,t)} f(y) \frac{f(y)^{-1}\Phi(y,f(y))}{\left\{\beta\Phi^{-1}\left(x,c_1t^{-Q(x)}\right)\right\}^{-1} \Phi\left(y, \beta\Phi^{-1}\left(x,c_1t^{-Q(x)}\right)\right)}\, d\mu(y) \nonumber \\& \quad \le C\left\{t^{\alpha(x)}\Phi^{-1}\left(x,c_1t^{-Q(x)}\right) +t^{\alpha(x)}\Phi^{-1}\left(x,c_1t^{-Q(x)}\right)\int_{B(x,t)} \Phi(y,f(y))\, d\mu(y)\right\} \nonumber \\& \quad \le Ct^{\alpha(x)}\Phi^{-1}\left(x, t^{-Q(x)}\right)\nonumber\\ \end{align} $$
for all
$0<t\le d_X$
. It follows that
$$ \begin{align*} & \sum_{2\delta<2^i\le 2d_X} \frac{2^{i\alpha(x)}}{\mu(B(x,\tau 2^i))} \int_{B(x,2^i)} f(y)\, d\mu(y) \\& \quad \le \sum_{2\delta<2^i < d_X} \frac{2^{i\alpha(x)}}{\mu(B(x,\tau 2^i))} \int_{B(x,2^i)} f(y)\, d\mu(y) + C \frac{d_X^{\alpha(x)}}{\mu(B(x,\tau d_X))} \int_{B(x,d_X)} f(y)\, d\mu(y). \end{align*} $$
As for the rest of the proof, we obtain (4.3) in view of (4.5), Lemma 3.1 (1) and
$(\Gamma \Phi \alpha Q)$
, as in the proof of [Reference Ohno and Shimomura18, Lemma 3.5].
As in [Reference Ohno and Shimomura18], we consider a function
satisfying the following properties:
-
(Ψ1)
$\Psi (\cdot , t)$
is measurable on E for each
$t \in [0, \infty )$
and
$\Psi (x, \cdot )$
is continuous on
$[0, \infty )$
for each
$x \in E$
; -
(Ψ2) there is a constant
$\widetilde {Q}_1 \ge 1$
such that
$\Psi (x,t_1) \le \Psi (x, \widetilde {Q}_1t_2)$
for all
$x \in E$
whenever
$0 < t_1 < t_2$
; -
(ΨΓ) there are constants
$\widetilde {Q}_2,\ \widetilde {Q}_3 \ge 1$
and
$s_0^* \ge s_0$
such that
$\Psi (x, \Gamma (x,s)/\widetilde {Q}_2) \le \widetilde {Q}_3 s$
for all
$x \in E$
and
$s\ge s_0^*$
.
In line with the proof of [Reference Ohno and Shimomura18, Theorem 3.6], using Corollary 3.9, we prove Trudinger-type inequalities, which is an extension of [Reference Ohno and Shimomura18, Theorem 3.6].
Theorem 4.3 Let
$1\le \lambda \le \tau $
and
$0<\varepsilon \le 1$
. Let
$\Phi (x,t)$
satisfy
$(\Phi 3;p)$
and
$(\Phi 5;Q)$
for
$p>1$
. Suppose that X satisfies
$(M \lambda )$
and
$(\Gamma \Phi \alpha Q)$
holds. Then there exist constants
$c_1=c_1(\varepsilon )>0$
and
$c_2>0$
independent of
$\varepsilon $
such that
$$ \begin{align} \frac{r^{\varepsilon}}{\mu(B(z,r))}\int_{E\cap B(z,r)} \Psi \left(x, \frac{|J_{\alpha(\cdot), \tau}f(x)|}{c_1}\right)\, d\mu(x) \le c_2 \end{align} $$
for all
$z\in X$
,
$0<r\le d_X$
and
$f \in L^{\Phi }(X)$
with
$\|f\|_{L^{\Phi }(X)}\le 1$
.
Proof Let f be a nonnegative measurable function on X with
$\|f\|_{L^{\Phi }(X)}\le 1$
. Then Corollary 3.9 implies that there exist constants
$0<\varepsilon _2<\varepsilon $
and
$C>0$
independent of
$\varepsilon $
and
$\varepsilon _2$
such that
for all
$z\in X$
and
$0<r\le d_X$
. Let
$x \in E$
. For
$0 < \delta \le d_X/2$
, Lemma 4.2 and
$\lambda \le \tau $
imply
with a constant
$C>0$
independent of x.
When
$M_{\lambda }f(x) \le 2/d_X$
, we take
$\delta = d_X/2$
. By (4.2) and Lemma 4.1 (1), we see that there exists a constant
$C>0$
independent of x such that
Next, consider the case when
$2/d_X < M_{\lambda }f(x) < \infty $
. By Lemma 4.1 (3) and
$(\Gamma 1)$
, there exists a constant
$m>0$
such that
$\Gamma (x,s)/s\le m \Gamma (x,2/d_X)$
for
$s \ge 2/d_X$
. Let
$$\begin{align*}\delta = (d_X/2) \left[ \frac{\Gamma (x, M_{\lambda}f(x))}{m\Gamma(x,2/d_X)M_{\lambda}f(x)} \right]^{1/\alpha(x)}. \end{align*}$$
As in the proof of [Reference Ohno and Shimomura18, Theorem 3.6], by (4.2)
and by
$(\Gamma 1)$
and Lemma 4.1 (1) and (2),
where C is dependent of
$\varepsilon $
and
$\varepsilon _2$
. Hence, there exists a constant
$C>0$
independent of x such that
It follows from (4.8) and (4.9) that there exists a constant
$C^*>0$
such that
for a.e.
$x \in E$
.
Letting
$c_1 = \widetilde {Q}_1 \widetilde {Q}_2 C^*$
, using
$(\Psi 2)$
and
$(\Psi \Gamma )$
, we have
$$\begin{align*}\begin{aligned} \Psi \left( x, \frac{J_{\alpha(\cdot), \tau}f(x)}{c_1} \right) & \le \Psi \Big( x, \Gamma \big( x, \max\left\{s_0^*, \{M_{\lambda}f(x)\}^{\varepsilon_2}\right\} \big)/\widetilde{Q}_2 \Big) \\ & \le \widetilde{Q}_3 \max \{ s_0^*, \{M_{\lambda}f(x)\}^{\varepsilon_2} \} \le \widetilde{Q}_3(s_0^* + \{M_{\lambda}f(x)\}^{\varepsilon_2}) \end{aligned} \end{align*}$$
for a.e.
$x \in E$
, so that by (4.7)
$$ \begin{align*} &\frac{1}{\mu(B(z,r))}\int_{E\cap B(z,r)} \Psi \left(x, \frac{J_{\alpha(\cdot), \tau}f(x)}{c_1}\right)\, d\mu(x) \\ & \le \widetilde{Q}_3 s_0^* + \widetilde{Q}_3 \frac{1}{\mu(B(z,r))} \int_{E\cap B(z,r)} \{M_{\lambda}f(x)\}^{\varepsilon_2}\, d\mu(x)\\ & \le c_2r^{-\varepsilon} \end{align*} $$
for all
$z\in X$
and
$0<r\le d_X$
, as required.
Remark 4.4 First, thanks to Remark 2.1,
$(\Phi 5;Q)$
in Theorem 4.3 is better than
$(\Phi 5;\nu )$
in [Reference Ohno and Shimomura18]. Second, the conclusion in [Reference Ohno and Shimomura18, Theorem 3.6] follows immediately from (4.6) when
$r=d_X$
. Hence, Theorem 4.3 extends [Reference Ohno and Shimomura18, Theorem 3.6].
5 Double phase functionals
Let
$p(\cdot )$
and
$q(\cdot )$
be real valued measurable functions on X such that
-
(P1)
$1 \le p^- \le p^+ < \infty ,$
-
(Q1)
$1 \le q^- \le q^+ < \infty .$
Suppose that
$p(\cdot )$
and
$q(\cdot )$
satisify
-
(P2)
$p(\cdot )$
is log-Hölder continuous, that is, with a constant
$$ \begin{align*}|p(x) - p(y)| \le \frac{C_{p}}{\log (e+1/d(x,y))} \quad (x,\, y \in X)\end{align*} $$
$C_{p} \ge 0$
, and
-
(Q2)
$q(\cdot )$
is log-Hölder continuous, that is, with a constant
$$ \begin{align*}|q(x) - q(y)| \le \frac{C_{q}}{\log (e+1/d(x,y))} \quad (x,\, y \in X)\end{align*} $$
$C_{q} \ge 0$
.
In this section, we consider a double phase functional
$\Phi (x,t)$
with variable exponents given by
where
$p(x)<q(x)$
for
$x\in X$
,
$a(\cdot )$
is non-negative, bounded and Hölder continuous of order
$\theta \in (0,1]$
and
$b(x)=a(x)^{1/q(x)}$
([Reference Maeda, Mizuta, Ohno and Shimomura11, Reference Ragusa and Tachikawa19], cf. [Reference Baroni, Colombo and Mingione1, Reference Colombo and Mingione3]). Notice that
$\Phi (x,t)$
satisfies (
$\Phi $
1)–(
$\Phi $
3) and that
$\Phi (x,t)$
satisfies
$(\Phi 5;Q)$
for
$\theta \ge \sup _{x\in X_0}\{Q(x)(q(x)/ p(x)-1)\}$
, where
$X_0=\left \{x\in X : a(x)>0\right \}$
(see [Reference Ohno and Shimomura17, Lemma 6.1]).
Set
and
$E = E_1 \cup E_2$
. Let us define
$$\begin{align*}\Gamma(x,s)= \left\{ \begin{array}{@{}ll} \log(e+s), & x \in E_1 \\ b(x)^{-1}\log(e+s), & x \in E_2 \end{array} \right. \end{align*}$$
for
$s \ge s_0$
. Here note from [Reference Ohno and Shimomura18, Lemma 4.1] that
$\Gamma (x,s)$
satisfies
$(\Gamma 1)$
,
$(\Gamma 2)$
,
$(\Gamma _{\mathrm {log}})$
and
$(\Gamma \Phi \alpha Q)$
.
Consider the function
$$ \begin{align*} \Psi(x,t)=\left\{ \begin{array}{@{}ll} \exp t, & x \in E_1 \\ \exp\left(b(x)t\right) & x \in E_2 \\ \end{array} \right. \end{align*} $$
for
$t>0$
. Notice that
$\Psi (x,t)$
satisfies
$(\Psi 1)$
,
$(\Psi 2)$
, and
$(\Psi \Gamma )$
with
$s_0^*=2/d_X$
.
By Theorem 4.3, we obtain the following Trudinger’s inequality, which is an extension of [Reference Ohno and Shimomura18, Corollary 4.2].
Corollary 5.1 Let
$1\le \lambda \le \tau $
and
$0<\varepsilon \le 1$
. Assume that
$p^->1$
and
$\theta \ge \sup _{x\in X_0}\{Q(x) (q(x)/p(x)-1)\}$
. Suppose that X satisfies
$(M \lambda )$
. Then there exist constants
${c_1=c_1(\varepsilon )>0}$
and
$c_2>0$
independent of
$\varepsilon $
such that
$$ \begin{align} & \frac{r^{\varepsilon}}{\mu(B(z,r))}\int_{E_1\cap B(z,r)} \exp\left(\frac{|J_{\alpha(\cdot), \tau}f(x)|}{c_1}\right)\, d\mu(x) \nonumber \\& \quad + \frac{r^{\varepsilon}}{\mu(B(z,r))}\int_{E_2\cap B(z,r)} \exp\left(\frac{b(x)|J_{\alpha(\cdot), \tau}f(x)|}{c_1}\right)\, d\mu(x) \le c_2 \end{align} $$
for all
$z\in X$
,
$0<r\le d_X$
and
$f \in L^{\Phi }(X)$
with
$\|f\|_{L^{\Phi }(X)}\le 1$
.
Remark 5.2 In [Reference Ohno and Shimomura18, Corollary 4.2], we showed the following result: Let
$1\le \lambda \le \tau $
. Assume that
$p^->1$
and
$\sup _{x\in X_0}(q(x)-p(x))/\theta \le p^-/Q^+$
. Suppose that X satisfies
$(M \lambda )$
. Then there exist constants
$c_1, c_2>0$
such that
$$ \begin{align} \int_{E_1} \exp\left(\frac{|J_{\alpha(\cdot), \tau}f(x)|}{c_1}\right)\, d\mu(x) + \int_{E_2} \exp\left(\frac{b(x)|J_{\alpha(\cdot), \tau}f(x)|}{c_1}\right)\, d\mu(x) \le c_2 \end{align} $$
for all
$f \in L^{\Phi }(X)$
with
$\| f \|_{L^{\Phi }(X)} \le 1$
.
Note that the assumption
$\theta \ge \sup _{x\in X_0}\{Q(x)(q(x)/p(x)-1)\}$
in Corollary 5.1 is better than the assumption
$\sup _{x\in X_0}(q(x)-p(x))/\theta \le p^-/Q^+$
in [Reference Ohno and Shimomura18, Corollary 4.2] since
for all
$x\in X_0$
. Furthermore, (5.1) implies (5.2) when
$r=d_X$
since
$0<d_X^{\varepsilon }/\mu (z,d_X)=d_X^{\varepsilon }/\mu (X)<\infty $
and
$E_j\cap B(z,d_X)=E_j$
for all
$z\in X$
and
$j=1,2$
. Therefore, Corollary 5.1 extends [Reference Ohno and Shimomura18, Corollary 4.2].
Remark 5.3 We give examples of functions
$a(\cdot )$
,
$\alpha (\cdot )$
,
$p(\cdot )$
, and
$q(\cdot )$
that satisfy the assumptions in Corollary 5.1 but not the assumption
$\sup _{x\in X_0}(q(x)-p(x))/\theta \le p^-/Q^+$
in the previous paper [Reference Ohno and Shimomura18]. This shows the significance of considering variable order
$Q(\cdot )$
.
Let X and
$Q(\cdot )$
be as in Example 1.1. Then note from [Reference Nazarov, Treil and Volberg13] that X satisfies
$(M 3)$
. We assume that
$a(\cdot )$
is non-negative, bounded and Hölder continuous of order
$\theta \in (0,1]$
such that
$a(x)>0$
for all
$x\in X_1$
and
$a(x)=0$
for all
$x\in X_2$
, that is,
$X_1=X_0=\{ x \in X: a(x)>0 \}$
. For an examples of
$a(\cdot )$
,
$$\begin{align*}a(x)= \left\{\begin{array}{@{}ll} x_1^{\theta} & \text{for }x=(x_1,x_2)\in X_1 \\ 0 & \text{for }x\in X_2. \end{array} \right. \end{align*}$$
Let
$1<p_0<\infty $
and
$q_0= (\theta +1)p_0$
. We consider
and
$$\begin{align*}q(x)=q_0-\frac{c_0(\theta+1)}{\log(e+1/|x|)} \end{align*}$$
for
$x\in X$
, where
$c_0$
is a constant satisfying
Further we consider a function
$$\begin{align*}\alpha(x)= \left\{\begin{array}{@{}ll} 1/q(x) & \text{for }x\in X_1 \\ 2/p(x) & \text{for }x\in X_2. \end{array} \right. \end{align*}$$
Then
$p(\cdot )$
satisfies (P1) and (P2) since
$0<c_0<p_0-1$
,
$q(\cdot )$
satisfies (Q1) and (Q2) since
$0<c_0<(q_0-1)/(\theta +1),$
and
$p(x)<q(x)$
holds for all
$x\in X$
since
$0<c_0<(q_0-p_0)/\theta $
. Further, we can show that
$$ \begin{align*} E_1 &= \{ x \in X :a(x)=0, Q(x)= \alpha(x)p(x) \}=X_2, \\ E_2 &= \{ x \in X :a(x)>0, Q(x)= \alpha(x)q(x) \}=X_1 \end{align*} $$
and
$\sup _{x\in X_0}\{Q(x)(q(x)/p(x)-1)\} = \theta $
since
$q_0= (\theta +1)p_0$
. However,
$\sup _{x\in X_0} (q(x)-p(x))/\theta \le p^-/Q^+$
does not hold since
$$ \begin{align*} q(x)-p(x) =\theta\left(p_0-\frac{c_0}{\log(e+1/|x|)}\right) =\frac{\theta p(x)}{Q(x)}>\frac{\theta p^-}{Q^+} \end{align*} $$
for all
$x\in X_0=X_1$
since
$Q^+=2$
.
Remark 5.4 In general, if
$\Phi (x,t)$
satisfies
$(\Phi 5;\nu )$
with
$\nu>0$
satisfying
$\nu \le p^-/Q^+$
, then it satisfies
$(\Phi 5;Q)$
(see Remark 2.1). In this remark, we show that
$(\Phi 5;Q)$
is weaker than
$(\Phi 5;\nu )$
when
$0<\nu \le p^-/Q^+$
. For this purpose, let X,
$a(\cdot )$
,
$p(\cdot )$
, and
$q(\cdot )$
be as in Remark 5.3. First, Remark 5.3 implies that
$\Phi (x,t)$
satisfies
$(\Phi 5;Q)$
. Next, we show that
$\Phi (x,t)$
does not satisfy
$(\Phi 5;\nu )$
for
$0<\nu \le p^-/Q^+$
. Let
$x=(t^{-\nu },0)$
and
$y=(0,0)$
for
$t\ge 1$
. Then we find that
$x,y\in X$
,
$d(x,y)=t^{-\nu }$
and
$$ \begin{align*} \lim_{t\to \infty}\frac{\Phi(x,t)}{\Phi(y,t)} &=\lim_{t\to \infty} \frac{t^{p_0-c_0/\log(e+1/|x|)}+x_1^{\theta}t^{q_0-c_0(\theta+1)/\log(e+1/|x|)}}{t^{p_0}} \\ &=\lim_{t\to \infty}\left(t^{-c_0/\log(e+t^{\nu})} +t^{\theta (p_0-\nu)-c_0(\theta+1)/\log(e+t^{\nu})}\right)\\ &=\infty \end{align*} $$
for all
$0<\nu <p_0$
since
$q_0= (\theta +1)p_0$
. Hence,
$\Phi (x,t)$
does not satisfy
$(\Phi 5;\nu )$
for all
$0<\nu <p_0$
, so that
$\Phi (x,t)$
does not satisfy
$(\Phi 5;\nu )$
for
$0<\nu \le p^-/Q^+$
since
$p^-/Q^+=p^-/2<p_0/2<p_0$
.
6 Sobolev functions
In this section, we consider the case when
$\mu $
is doubling. Given
$u\in L^{1}_{loc}(X)$
and g be a nonnegative measurable function on X, we say that the pair
$u, g$
satisfies a Poincaré inequality in X if there exist constants
$A_0>0$
and
$\sigma \ge 1$
such that
for all
$x\in X$
and
$r>0$
, where
$u_{B(x,r)}=\int _{B(x,r)} u(y)\, d\mu (y)/\mu (B(x,r))$
.
As in [Reference Ohno and Shimomura14], we consider Musielak–Orlicz–Hajłasz–Sobolev spaces
$M^{1,\Phi }(X)$
. We say that a function
$u\in L^{\Phi }(X)$
belongs to
$M^{1,\Phi }(X)$
if there exists a nonnegative function
$g\in L^{\Phi }(X)$
, called a Hajłasz gradient of u, such that
for
$\mu $
-almost every
$x,y\in X$
. Notice that the Poincaré inequality holds if we integrate both sides in (6.1) over y and x.
When
$\mu $
satisfies the doubling condition and the pair
$u, g$
satisfies a Poincaré inequality in X, it follows from [Reference Hajłasz and Koskela4, Theorem 5.2] that
for a.e.
$x \in B$
. Thanks to this estimate, Theorem 4.3 gives the following theorem.
Theorem 6.1 Given
$u\in L^{1}_{loc}(X)$
and
$g\in L^{\Phi }(X)$
be a nonnegative measurable function on X, suppose that the pair
$u, g$
satisfies a Poincaré inequality in X. Let
$0<\varepsilon \le 1$
. Let
$\Phi (x,t)$
satisfy
$(\Phi 3;p)$
and
$(\Phi 5;Q)$
for
$p>1$
. Assume that
$(\Gamma \Phi \alpha Q)$
with
$\alpha (\cdot )\equiv 1$
holds. Then there exist constants
$c_1=c_1(\varepsilon )>0$
and
$c_2>0$
independent of
$\varepsilon $
such that
$$\begin{align*}\frac{r^{\varepsilon}}{\mu(B(z,r))}\int_{E\cap B \cap B(z,r)} \Psi \left(x, \frac{|u(x)-u_B|}{c_1}\right)\, d\mu(x) \le c_2 \end{align*}$$
for all
$z\in X$
,
$0<r\le d_X$
and balls B.
Remark 6.2 Theorem 6.1 extends [Reference Ohno and Shimomura18, Theorem 5.1] as well as Remark 4.4. For the
$L^p$
case, see [Reference Hajłasz and Koskela4, Theorem 5.1].
Corollary 5.1 gives the following corollary for double phase case, as an extension of [Reference Ohno and Shimomura18, Corollary 5.2].
Corollary 6.3 Let
$p(\cdot )$
,
$q(\cdot )$
,
$a(\cdot )$
,
$E_1$
, and
$E_2$
with
$\alpha (\cdot )\equiv 1$
be as in Section 5 and let
for
$x \in X$
and
$t \ge 0$
. Given
$u\in L^{1}_{loc}(X)$
and
$g\in L^{\Phi }(X)$
be a nonnegative measurable function on X, suppose that the pair
$u, g$
satisfies a Poincaré inequality in X. Let
$0<\varepsilon \le 1$
. If
$p^->1$
and
$\theta \ge \sup _{x\in X_0}\{Q(x)(q(x)/p(x)-1)\}$
, then there exist constants
$c_1=c_1(\varepsilon )>0$
and
$c_2>0$
independent of
$\varepsilon $
such that
$$ \begin{align} & \frac{r^{\varepsilon}}{\mu(B(z,r))}\int_{E_1\cap B\cap B(z,r)} \exp\left(\frac{|u(x)-u_B|}{c_1}\right)\, d\mu(x) \nonumber \\ &+ \frac{r^{\varepsilon}}{\mu(B(z,r))}\int_{E_2\cap B\cap B(z,r)} \exp\left(\frac{b(x)|u(x)-u_B|}{c_1}\right)\, d\mu(x) \le c_2 \end{align} $$
for all
$z\in X$
,
$0<r\le d_X$
and balls B.
Remark 6.4 As well as Remark 5.2, the assumption
$\theta \ge \sup _{x\in X_0}\{Q(x)(q(x)/ p(x)-1)\}$
in Corollary 6.3 is better than the assumption
$\sup _{x\in X_0}(q(x)-p(x))/\theta \le p^-/Q^+$
in [Reference Ohno and Shimomura18, Corollary 5.2] and the conclusion in [Reference Ohno and Shimomura18, Corollary 5.2] follows from (6.2) when
$r=d_X$
. Thus, Corollary 6.3 is an extension of [Reference Ohno and Shimomura18, Corollary 5.2].
Acknowledgements
The authors would like to thank the referee for giving useful comments.




