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Research article Special Issues

On the composition operator with variable integrability

  • In this article, we considered a class of composition operators on Lebesgue spaces with variable exponents over metric measure spaces. Taking advantage of the compatibility between the metric-measurable structure and the regularity properties of the variable exponent, we provided necessary and sufficient conditions for this class of operators to be bounded and compact, respectively. In addition, we showed the usefulness of the variable change to study weak compactness properties in the framework of non-standard spaces.

    Citation: Carlos F. Álvarez, Javier Henríquez-Amador, John Millán G., Eiver Rodríguez. On the composition operator with variable integrability[J]. AIMS Mathematics, 2025, 10(2): 2021-2041. doi: 10.3934/math.2025095

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  • In this article, we considered a class of composition operators on Lebesgue spaces with variable exponents over metric measure spaces. Taking advantage of the compatibility between the metric-measurable structure and the regularity properties of the variable exponent, we provided necessary and sufficient conditions for this class of operators to be bounded and compact, respectively. In addition, we showed the usefulness of the variable change to study weak compactness properties in the framework of non-standard spaces.



    Let (X,d,μ) be a metric measure space equipped with a metric d and the Borel regular measure μ. If φ:XX is a non-singular map, i.e.,

    μ(φ1(E))=0,  for all Borelμ-measurable sets EX  with  μ(E)=0, (1.1)

    then we can define the composition operator

    Cφ:ffφ,  for every measurable functionfon  X.

    According to (1.1), the measure (μφ1)():=μ(φ1()) is absolutely continuous with respect to the measure μ. From the Radon-Nikodym theorem, there exists a measurable function uφ:X[0,+] such that

    μ(φ1(E))=Euφ(x) dμ,  for all Borel  μ-measurable sets EX with μ(E)=0. (1.2)

    The composition operator Cφ appears naturally in the context of variable change and has recently been applied to dynamical systems, partial differential equations, and data science. For more details, see [3,8,16,32]. For seminal applications, refer to [23,24].

    In Lp spaces, characterizing of the boundedness of composition operators is a fundamental problem (e.g., see [5,27,28,29]). For other function spaces, see [1,6,7,13,20,25,30,31]. It is well-known that Cφ continuously maps Lp(X) into itself if and only if the function uφ is essentially bounded on X. In such a case, φ is said to induce a composition operator on Lp(X).

    The first question that we address in this article is:

    Q.1 What kind of control should be imposed on the variable exponent p:XR such that the map φ induces a composition operator Cφ on Lp()(X)?

    A fruitful analysis of variable integrability spaces Lp()(X) is obtained when X is a Euclidean domain, e.g., [9,11,12]. Unfortunately, the same cannot be said for general metric measure spaces. However, the authors in [15] achieved boundedness of the maximal operator with a notion of "dimension" through a local uniformity condition:

    μ(B(x,r))rp(x),  xX, (1.3)

    where, B(x,r):={zX:d(z,x)<r}, r0, see also [22] by endowing X.

    An essential difficulty in proving the boundedness of Cφ over all Lp()(X) is that Cavalier's principle (see [4, Lemma 1.10]) does not hold. This motivates our question about appropriate control conditions (Q.1). A control on the variable exponent p() compatible with a condition like (1.3), which we propose in this article, is:

    infxBp(x)infxφ1(B)p(x)supxφ1(B)p(x)supxBp(x), (1.4)

    for every ball BX. Note that when p() is constant, the condition (1.4) is trivial. It seems natural to impose a "control" on the local supremum and infimum of the variable exponent as a new ingredient in our analysis.

    Another important point is that our boundedness result for Cφ over Lp()(X) can be extended in several directions including:

    n-dimensional Euclidean domains on Rn with Lebesgue measure and Euclidean distance.

    ● Complete Riemannian manifolds of positive Riemannian measure and distance.

    ● Locally compact and separable group equipped with a left-invariant metric and left-invariant Haar measure.

    Currently, the boundedness of Cφ on variable integrability spaces such as Lp()(X) is not fully understood, even for n-dimensional Euclidean domains. However, boundedness results for these operators are known in more regular function spaces, such as variable exponent Bergman spaces (see [26]) and, recently, in holomorphic function spaces [21]. Additionally, the inequality

    |Cφf(x)|p(x) dμ C |f(x)|p(x) dμ, (1.5)

    does not hold in Lp()(X) unless p(φ())=p() almost everywhere in X.

    Regarding compactness, it is well-known that Lp(X) with p1 does not support compact composition operators if X has no atoms. In this paper, we show that metric measure spaces satisfying a local uniform property as in (1.3) have no atoms. This allows us to provide a different proof from the constant exponent case, using recent developments on precompact sets on Lp()(X) obtained in [14].

    We also study a related class of operators:

    Tφ:ffφ,  D(Tφ):={fLp()(X):fφL(pφ)()(X)}.

    This class Tφ represents the natural extension to the variable exponent case. Recent studies on boundedness, compactness, and closed-range properties for such operators have been conducted in [2,10] for bounded exponents defined on complete σ-finite spaces.

    In this paper, we study the boundedness of Tφ by providing a simple proof on Lp()(X), where X is a metric measure space with a doubling measure μ and unbounded exponents p(). On the other hand, the non-compactness of Tφ is obtained when X is a connected space. Particularly, in some cases, Tφ maps Lp()(X) to Lp()(X). For example, when

    Tφ:Lp()(X)L(pφ)()(X)andL(pφ)()(X)Lp()(X),

    the right-hand embedding implies, in particular, that p(φ(x))p(x) a.e. in xX. Moreover, this implies the right inequality in (1.4). In this sense, the results concerning the operator Cφ are obtained with a weaker hypothesis by replacing the embedding with regularity of log-continuous type, which we adapt to the environment of metric measure spaces.

    Finally, another property that has not been explored in the framework of spaces with variable integrability is the weak compactness of the operator Tφ, even in the Euclidean case. In this direction, we show that the operator Tφ behaves well on weakly compact sets in Lp()([0,1]), and some results are obtained in the non-reflexive setting p=1. In fact, our partial results allow us to state the following conjecture: Let p=1,

    Tφis weakly compact onLp()([0,1])if and only ifinfx[0,1]uφ(x)=0.

    Let us now describe the organization of the article. In Section 2, we fix the notations and recall the definitions and a few results that will be important in our work. In Section 3, we study continuity and compactness for the operator Cφ. Finally, we study some properties of the operator Tφ in Section 4.

    We assume throughout the paper that BX is the σ-algebra of Borel generated by μ-measurable open sets in X, the measure μ of every open nonempty set is positive, and the measure of every bounded set is finite on X.

    We define the property of doubling measure, which endows a metric measure space with good properties; for more details, see [4,17].

    Definition 1. A measure μ is said to satisfy the doubling condition if there exists a positive constant C such that

    μ(B(x,2r))C μ(B(x,r)),  foreveryball  B(x,r).

    Another fruitful property for a metric measure space is the regular Q-Ahlfors property, which in some cases is stronger than the doubling property (see [15]).

    Definition 2. We say that the measure μ is lower Ahlfors Q-regular if there exists a positive constant C such that μ(B)C diam(B)Q for every ball BX with diamB2 diamX. We say that μ is upper Ahlfors Q-regular if there exists a positive constant C such that μ(B)C diam(B)Q for every ball BX with diamB2 diamX. The measure μ is Ahlfors Q-regular if it is upper and lower Ahlfors Q-regular, i.e., if

    μ(B)diam(B)Q   for every ball BX with diam B2 diam X.

    The class of variable exponents, denoted by P(X), is defined by

    P(X):={p:X[1,):p() is Borel measurable}.

    Given AX and p()P(X), we put

    p+A:=esssupxAp(x)  and  pA:=essinfxAp(x).

    When the domain is clear, we simply write p+=p+(X) and p=p(X). Some properties of regularity at infinity, relative to variable exponent, are useful for studying composition operators within the framework of non-standard functional spaces. For Euclidean domains and metric measures spaces, these properties are provided in [9,11] and [14,15], respectively.

    Definition 3. Let p()P(X). We say that

    1. p() is locally log-Hölder continuous, denoted by p()LH0(X), if there exists a constant K0 such that for all x,yX, d(x,y)<12,

    |p(x)p(y)|K0log(d(x,y)).

    2. p() is log-Hölder continuous at infinity with point base x0X, denoted by p()LH(X), if there are constants K and p such that for all xX,

    |p(x)p|Klog(e+d(x,x0)).

    When p() is log-Hölder continuous both locally and at infinity, we denote this by p()LH(X).

    In this work, we introduce a class of exponents associated with the φ-map. Denote by B0 the set of all open balls in X.

    Definition 4. Let φ:XX be a Borel measurable map. We define the following kinds of exponents:

    Plogφ+(X):={p()LH(X):[φ]p+1},Plogφ(X):={p()LH0(X):[φ]p1},Plogφ(X):=Plogφ+(X)Plogφ(X),

    where

    [φ]p+:=inf{p+Bp+φ1(B):BB0},   [φ]p:=sup{pBpφ1(B):BB0}.

    In the following example, we show that [φ]p+1 for countable sub-covers, in fact, this is sufficient for the continuity result that we will obtain below (see Theorem 2).

    Example 1. Let X:=R+ and define p:R+[1,+) as variable exponent given by

    p(x):={1+x2,x(0,1)1+12x1,x1.

    It is not difficult to show that

    0p(x)1ln(1+e)ln(|x|+e),  forall  xR+.

    That is, p()LH(R+). In addition, it is easy to see that p()LH0(R+); for x(0,1) and y1 such that it follows that

    |p(x)p(y)|=|2x2yx212y1|2x2y2x22 (y1)2 (yx)=2 |xy|.

    Similarly, for x1 and y(0,1). This is sufficient to show that p() is Lipschitz continuous on R+ and, therefore, p()LH0(R+). Now, consider φ:R+R+ to be a non-singular map such that 0φ(x)x for all xR+. On the other hand, let ϵ(0,+) and we consider

    A:={(xϵ,x+ϵ):xR+}.

    Let {qj}jQ+ be such that

    qj+  as  j+,  and  R+=jIj,  Ij:=(qj5ϵ,qj+5ϵ).

    Then, by using LH-regularity, we have

    supxφ1(Ij)p(x)supxφ1(Ij)|p(x)pφ(x)|+supxφ1(Ij)pφ(x)supxφ1(Ij)Cln(e+φ(x))+p+IjCln(e+qjϵ)+p+Ij.

    Hence, since qj+ as j+

    lim supjp+φ(Ij)lim supjp+(Ij)<+,  as  j+.

    Therefore,

    0p+(Iqnj)p+φ(Iqnj),  formanyinfinite  njN.

    Finally, in particular, note that Lp()(R+) is not embedded in Lpφ()(R+) and p()Plogφ+(R+) (in the sense of accounting coverages).

    The space Lp()(X) is the classical variable Lebesgue space on X. Some of its basic properties have been studied, for instance, in [15].

    Definition 5. Let p()P(X) and L0(X) be the set of measurable functions on X. The Lebesgue space with variable exponent Lp()(X) is defined by

    Lp()(X):={fL0(X):ρ(fη)< for someη>0},

    where

    ρ(f):=X|f(x)|p(x)dμ,

    is called the associated modular with p(). It is known that Lp()(X) is a Banach space equipped with the Luxemburg-Nakano norm

    fp():=inf{η>0:ρ(fη)1}.

    Additionally, when p() is bounded, we obtain the inequality that provides a relation between the norm and the modular:

    min{fp+p(),fpp()}ρ(f)max{fp+p(),fpp()}, (2.1)

    for fLp()(X). Also, in the case p+<+, the space Lp()(X) can be defined as all measurable functions f:XR such that ρ(f)<+, and the dual space is identified with Lp()(X), where p() is the conjugate exponent relative to p(), that is,

    1p(x)+1p(x)=1,  xX{x:p(x)=1}.

    It is well-know that the space of essentially bounded functions with compact support Lp()c(X) is dense in Lp()(X).

    In this section, we start analyzing the behavior and properties of the operator Cφ on Lp()(X) based on the following results in the space Lp(X):

    P.1 Cφ:Lp(X)Lp(X) is bounded if and only if uφL(X). In particular,

    X|(Cφf)(x)|p dμ uφ X|f(x)|p dμ, for all fLp(X).

    In the second part, we completely characterize the continuity and compactness of operator Cφ on Lp()(X).

    Our first result shows that the integral inequality does not hold in general for any variable exponent, unless the exponent is both bounded and invariant under dilations or contractions induced by φ. The variable exponent induced by φ is denoted by pφ():=p(φ()). Additionally, we associate φ with the number

    U(φ):=supBB0μ(φ1(B))μ(B).

    Theorem 1. Assume p()P(X) with p+<+ and let φ:XX be a non-singular measurable transformation. Then, the following statements are equivalent:

    M.1 There exists a constant C>0 such that

    X|(Cφf)(x)|p(x) dμ C X|f(x)|p(x) dμ, forall fLp()(X). (3.1)

    M.2 The function uφ:XR is essentially bounded on X, and

    p(x)=pφ(x),  a.e.inxX.

    Proof. It is clear that (M2)(M1) with C:=uφ. To prove (M1)(M2), first suppose that p+<; since φ is non-singular, we have pφL(X) so

    pφ()p()L(X).

    Assume that (M.1) holds, so for BB0, with μ(B)<+. Considering the function f=XBLp()(X), from inequality (3.1), we deduce that

    C μ(B)μ[φ1(B)]1. (3.2)

    Now, let Ωφ:={xX:p(x)pφ(x)} and suppose that μ(Ωφ)>0. Thus, if Eφ:={xX:p(x)>pφ(x)}B, then by σ-additivity, we have

    μ(Eφ)>0  or  μ(ΩφEφ)>0.

    So, we see only the case μ(Eφ)>0 because the case μ(ΩφEφ)>0 is analogue with minor settings. In fact, since μ(Eφ)>0, then by [17, Lemma 3.3.31], we can take yEφ such that it satisfies

    μ(EφBy)>0, for every ball  ByB0.

    Hence, since φ1(X)=X from (3.2), we can choose ByB0 (sufficiently large rate) such that

    0<μ(Eφφ1(By))<+. (3.3)

    Hence, using (3.1) with the functions fn()=n1p()XBy()Lp()(X), we obtain that

    Eφφ1(By)|n|p(x)pφ(x) dμ=X|(fnφ)(x)|p(x) dμC X|fn(x)|p(x) dμ=C n μ(By).

    Thus,

    Eφφ1(By)|n|p(x)pφ(x)1 dμC μ(By).

    By the classical Jensen's inequality we have

    Eφφ1(By)(p(x)pφ(x)1) dμlog1(n) μ(Eφφ1(By))log(C μ(By)μ(Eφφ1(By)))

    so, taking n+

    Eφφ1(By)(p(x)pφ(x)1) dμ=0.

    Therefore, μ(Eφφ1(By))=0, which is in contradiction with (3.3). Consequently, μ(Eφ)=0. In addition, uφL+(X) follows from (3.2) with B=EBX.

    In this section, we extend the classical continuity result in standard Lp spaces to function spaces with variable integrability Lp()(X). The proof strategy is inspired by the argument given by Cruz-Uribe and Fiorenza on the boundedness of the maximal operator in Lp()(X) when X is a Euclidean domain (see [9, Theorem 3.16]). For this purpose, we adapt [9, Lemmas 3.26 and 3.24] to the setting of metric measure spaces with Ahlfors regularity; see also [15].

    Lemma 1. Let φ:XX be a non-singular Borel map. Then,

    (i) If p()LH0(X) and μ is lower Ahlfors Q-regular, then there exists a positive constant C such that

    μ(B)p(φ(x))p+BC,  forall  BB0 and xφ1(B).

    (ii) If p()LH(X) and μ is upper Ahlfors Q-regular, then there are positive constants C1,C2 such that for every function f with 0f1 on EB, we have

    φ1(E)|f(φ(x))|p dμC1φ1(E)|f(φ(x))|p(x) dμ+C2.

    Similarly,

    φ1(E)|f(φ(x))|p(x) dμC1φ1(E)|f(φ(x))|p dμ+C2.

    Proof. (i) Since p(φ(x))p+B0 for xφ1(B), it suffices to check (i) for balls B:=B(v,r) with r1/2. For y0B such that

    p+Bp(y0)+1log(1/2r),

    from p()LH(X), it follows that

    p+Bp(φ(x))|p(φ(x))p(y0)|+1C0logd(φ(x),y0)C0log(1/2r).

    So,

    log(2r)p(φ(x))p+BC0,  xφ1(B).

    Therefore, since μ is lower Ahlfors Q-regular and p(φ(x))p+B0, we have

    μ(B)p(φ(x))p+B(CrQ)p(φ(x))p+BC rQ[p(φ(x))p+B]CQ.

    (ii) For x0X, define the function hx0:XR given by hx0(x):=(e+d(x,x0))r,  xX. First, we show that

    hpx0L1(X)  provided that  rp(q,+).

    Indeed, for the base point x0X, we consider the countable collection {Cj:jN} where,

    Cj:=B(x0,2j)B(x0,2j1)B0,  for each  jN.

    Hence,

    X|hx0(x)|p dμ=+j=1Cj|hx0(x)|p dμ=+j=1B2jB2j1(1e+d(x,x0))rp dμ+j=1B2jB2j12jrpdμ+j=1μ(B2j) 2jrp4q+j=12(qrp)j<+   (rp(q,+)).

    On the other hand, decompose φ1(E):=F1F2 where

    F1:={x:f(φ(x))hx0(x)},    F2:={x:f(φ(x))>hx0(x)}.

    On F1 we have,

    F1f(φ(x))p dμF1f(φ(x))p dμF1hx0(x)p dμ.

    By the LH-regularity,

    hx0(x)|p(x)p|exp(rlog(e+d(x,x0))|p(x)p|)exp(rC).

    Finally, since f(φ(x))1, we get

    F1f(φ(x))p dμF1f(φ(x))p(x) hx0(x)|p(x)p| dμexp(rC)F1f(φ(x))p(x) dμ.

    With the previous lemma, the main result of this work in response to (Q.1) is the following:

    Theorem 2. Assume that μ is a Q-Ahlfors regular measure on X, let φ:XX be a non-singular map. Then:

    (C1) Let p()Plogφ+(X). If the map uφ is essentially bounded on X, then the operator Cφ maps Lp()(X) into itself.

    (C2) Let p()Plogφ(X). If the operator Cφ maps Lp()(X) into itself, then there exists a positive constant C such that μ(φ1(B))Cμ(B) for every ball BB0, i.e.,

    U(φ)<+.

    (C3) Assume p()Plogφ(X). If, in addition, μ is a doubling measure on X, then (C1) and (C2) are equivalent.

    Proof. (C1). Suppose that uφL(X). Since p+<+, by density it is sufficient to show that

    Cφ:Lc(X)Lp()(X)Lp()(X).

    Indeed, let fLc(X)Lp()(X) with fp()1 and consider the decomposition |f|=f1+f2 where f1:=|f|χ{|f|>1} and f2:=|f|χ{|f|1}. We will divide the test into two steps:

    Step 1. Let us see that there exists a constant C>0 independent of f1 such that

    X|(f1φ)(x)|p(x) dμC. (3.4)

    Since f1L(R) and X is separable, it follows that the open cover of X

    {B(x,5rQ):xX},

    with K:=esssupxX(f1φ)(x)>1 and rQ:=K1Q, admits a pairwise disjoint countable open sub-cover {Bj5rQ:jN} such that

    XjNBjrQ.

    From the μ-regularity, μ(BjrQ)CQ K1 for all jN. In addition, since p()LH0(X), by using Lemma 1 there exists M>0 such that for BB0 and xφ1(B), we have μ(B)pφ(x)p+(B)M; also, by the fact that K(1,+) taking r():=p()pφ() for xX, we get

    |(f1φ)(x)|p(x)=|(f1φ)(x)|r(x) |(f1φ)(x)|pφ(x)(|(f1φ)(x)|r(x) X{r(x)0}+1) |(f1φ)(x)|pφ(x)(Kr(x)X{r(x)0}+1) |(f1φ)(x)|pφ(x)=(μ(BjrQ)r(x)X{r(x)0}+1) |f1φ)(x)|pφ(x).

    So,

    |(f1φ)(x)|p(x)(μ(BjrQ)r(x)X{r(x)0}+1) |(f1φ)(x)|pφ(x), for  xX.

    From [φ]p+1,

    p+φ(BjrQ)p+(BjrQ),  for all  jN.

    Hence,

    X|(f1φ)(x)|p(x) dμ=jφ1(BjrQ)|(f1φ)(x)|p(x) dμjφ1(BjrQ)(Kp(x)pφ(x)+1)|(f1φ)(x)|pφ(x) dμjφ1(BjrQ)(μ(BjrQ)pφ(x)p+Bj+1)|(f1φ)(x)|pφ(x) dμ(M+1)jφ1(BjrQ)|(f1φ)(x)|pφ(x) dμ(M+1)uφ.

    Therefore, the inequality (3.4) is obtained with C1:=(M+1)U(φ). Now, we estimate the size of Cφf2.

    Step 2. There exists a constant C2>0 independent of f2 such that

    X|(f2φ)(x)|p(x) dμC2+Xhx0(x)p dμ. (3.5)

    Since p()LH(X), we get f2Lp(X) and uφL(X) implies also that Cφf2Lp(X). Hence, for some C>0 independent of f2, we obtain

    X|(f2φ)(x)|p(x) dμC X|(f2φ)(x)|p dμ+Xhx0(x)p dμC uφX|f2(x)|p dμ+ Xhx0(x)p dxC1+Xhx0(x)p dμ,

    this last integral is finite by Lemma 1. Therefore, from (3.4) and (3.5), we obtain

    fφp()Cφ,p() fp(),  for all  fLc(X)Lp()(X).

    (C2). Suppose that

    Cφ:Lp()(X)Lp()(X).

    By the inequality (2.1) and the relation given by (1.2), it is sufficient to consider the case when BB0 is such that

    Xφ1(B)p(),XBp()1.

    In this case, since p()LH0(X) and [φ]p1, applying Lemma 1, we can find a constant C>0 such that,

    μ(φ1(B))Xφ1(B)pφp()C XBpφp()C μ(B)pφp+C μ(B)1p+B(pBp+B)μ(B)=C μ(B)1p+(pBp(x)) μ(B)1p+(p(x)p+B) μ(B)C μ(B).

    Finally, in order to obtain (C3) by assuming the doubling property of μ, note that

    μ(φ1(B))μ(B)=1μ(B)Buφ(x) dμ(x),  for every ball  B.

    Hence, by differentiation, it is easy to see that U(φ) is finite if and only if uφ is in L(X).

    Remark 1. According to the proof of the above theorem:

    Another hypothesis to obtain (C1) is pφ()p() a.e. in X and p()LH(X). Note that in our result, we replace pφ()p() by hypothesis p()LH0(X) and [φ]p+1, which also replaces the embedding Lpφ()(X)Lp()(X) proposed in [2, Theorem 3.4].

    In the proof of the above theorem, note that the condition (1.4) applies to a uniform Vitali cover of the space. In this sense, control over the inductor map φ and the exponent p() can be relaxed as shown in Example 1. In fact, note that for a suitable φ (e.g., φ(x):=Ax, xR+), it suffices to note that

    R+(f1φ)(x)p(x) dxφ1(IqnJ)(f1φ)(x)p(x) dx,  as  j+.

    We start this section by showing that Lp()(X) does not support non-trivial compact composition operators Cφ. In addition, we approach recent results related to weak compactness in variable Lebesgue spaces and provide some properties for Cφ.

    Lemma 2. Let μ be a Q-Ahlfors regular measure on X, φ:XX be a non-singular Borel map, and p()LH0(X) such that [φ]p=1. There exists a positive constant C0 such that, given AB0 with μ(A)>0, if for any ball B with AB and μ(B)<1, then

    μ(B)1p(x)pφ(x)C0,forallxφ1(AB).

    Proof. On one hand,

    supxφ1(AB)pφ(x)supxABp(x)supxBp(x)=p+B.

    On the other hand, since [φ]p=1

    infxφ1(AB)p(x)infxφ1(B)p(x)infxBp(x)=pB.

    Therefore, for xφ1(AB), it follows that μ(B)p(x)pφ(x)μ(B)p(B)p+(B). Hence, since p()LH0(X) by [15, Lemma 3.6], there exists C0>0 such that

    μ(B)1p(x)pφ(x)μ(B)1pBp+B=μ(B)p+BpBp+BC0.

    Theorem 3. Let μ be a Ahlfors Q-regular and doubling measure on X. The non-trivial bounded composition operator Cφ is not compact on Lp()(X).

    Proof. Note initially that the space (X,d,μ) does not contain atoms. Indeed, if EBX is an atom, then μ(E)>0, so there exists aE such that μ(EB(a,r))>0 for all r>0. Hence, if

    μ(EB(a,r))<μ(E),  for some   r>0,

    then the atomicity of E implies that μ(EB(a,r))=0, a contradiction. On the other hand, if μ(EB(a,r))=μ(E) for all r>0, then by using the Q-Ahlfors property of μ, we obtain 0<μ(E)C(2r)Q, thus μ(E)=0 as r0+ which is also a contradiction. Besides, suppose that Cφ is compact on all Lp()(X) and we consider for ϵ(0,+) the set

    Uϵ:={xX:uφ(x)>ϵ}.

    If μ(Uϵ)>0 for some ϵ>0, then from the non-atomicity of μ it follows that there exists a decreasing sequence {Un} such that

    {Un}Uϵ  with  0<μ(Un)<1/n  for any,   nN.

    Let's construct a bounded sequence in Lp()-norm that is not equi-integrable in Lp(); given δ>0, since φ:XX is non-singular, choose ρ>0 such that

    μ(φ1(S))<δ,  whenever  μ(S)<ρ.

    For this ρ>0, there exists N>0 which 1/Nρ. Now, since μ(Un)>0 for all nN by [17, Lemma 3.3.31] we can fix xnUn satisfying μ(UnB(xn,δ))>0. Consider the set AδB0, given by

    Aδ:=φ1(UNB(xN,δ)),

    it is clear that μ(Aδ)<δ. Moreover, by using Lemma 2, the function fN:XR given by

    fN:=μ(B(xN,δ))1p()XUNB(xN,δ)()BLp(),

    is such that

    Aδ(CφfN)(x)p(x) dμ φ1(UNB(xN,δ))(1μ(B(xN,δ)))p(x)pφ(x) dμμ(B(xN,δ))p+BpBp+BUNB(xN,δ) uφ(x)μ(B(xN,δ)) dμ(x)ϵ C0 μ(UNB(xN,δ))μ(B(xN,δ)).

    By differentiation,

    limr0+μ(UNB(xN,r))μ(B(xN,r))=1.

    Therefore, taking δ(0,+) small enough, we can suppose that we have the following lower bound:

    μ(UNB(xN,δ))μ(B(xN,δ))12.

    Thus,

    Aδ(CφfN)(x)p(x) dμ ϵ C0/2,  for  δ  small enough.

    By switching to a subsequence if necessary, we have that the sequence {Cφfn} is not equi-integrable in Lp()(X). Thus, by virtue of [14, Theorem 1], this contradicts the compactness of Cφ. Consequently, μ(Uϵ)=0 for all ϵ(0,+) or equivalently uφ(x)=0 a.e. in xX. This implies that,

    φ1(B)|Cφf|p(x) dμj=1,2φ1(B)|Cφfj|p± dμj=1,2B|fj(x)|p± uφ(x) dμ=0,

    that is, Cφf=0 on φ1(B) for all BB0 and it is enough for to get Cφ=0.

    In this second part, we provide a complete characterization of the continuity for composition operators in the framework of variable Lebesgue spaces.

    Theorem 4. Let μ with doubling property on X, p()P(X), and φ:XX be a non-singular Borel measurable map. Then, the composition operator Tφ maps space Lp()(X) into Lpφ()(X) if and only if the function xuφ(x)1/p(x) is essentially bounded, that is, uφ()1/p()L(X). Moreover,

    Tφ=esssupxX{uφ(x)1p(x)}.

    Remark 2. Theorem 4 generalizes the well-known result in the framework of Lebesgue spaces with constant exponent. More precisely, when p()=p1, then both the induced exponent and the space induced by the measurable map φ remain invariant, that is,

    pφ()=p  and Lpφ()(X)=Lp(X).

    Remark 3. Since fLp()(X) if and only if fp()1Lp()(X) (the same is true for p()), by Theorem 4, it follows that Tφ maps Lp()(X) into Lpφ()(X) if and only if Tφ maps Lp()(X) into Lpφ()(X). An interesting question is whether this is true for the operator Cφ acting on Lp() and Lp().

    Remark 4. In the case that

    Lpφ()(X)Lp()(X). (4.1)

    Theorem 4 provided a sufficient condition for the operator Tφ to map Lp()(X) into itself. In fact, the embedding (4.1) provided a class of maps φ:XX induced composition operators on Lp()(X).

    Remark 5. Note that from Remark 4, the embedding condition (4.1) can be modified by assuming that the variable exponent decays to infinity; for example, assume pφ(x)p(x) a.e. in xX (e.g., see [9, Theorem 2.45]) and p()LH(X).

    Remark 6. If the function xuφ(x) is bounded, then for any p()P(X) the function xuφ(x)1/p(x) is also bounded. So, by Theorem 4, we obtain the following weak inequality: there exists C>0 depending of φ such that for each t>0 and fLp()(X),

    t X{x:(fφ)(x)>t}pφ()C fφpφ()C fp().

    Proof. (Proof of Theorem 4) Suppose that Tφ maps Lp()(X) into Lpφ()(X). From closed graph theorem there exists C>0 such that TφC. Let us show that uφ()1/p()L(X); note first that uφ()1/p()L1loc(X), so let BB0 and define the function f:XR by

    f(x)=μ(B)1p(x) XB(x),  xR. (4.2)

    Hence, it is clear that ρ(f/λ)1 for all λ1 so fLp()(X) and fp()=1. This implies fφLpφ()(X) and fφpφ()C, that is, there exists λ0>0, which λ0<C and

    φ1(B)λpφ(x)0 μ(B)pφ(x)pφ(x) dμ1.

    Consequently,

    1μ(B)BCp(x) uφ(x) dμ=1μ(B)φ1(B)Cpφ(x) dμφ1(B)λpφ(x)0 μ(B)pφ(x)pφ(x) dμ1,

    by differentiation, it follows that the map xCp(x)uφ(x) is essentially bounded. Reciprocally, denote by Mφ the multiplication operator with symbol uφ()1/p() so if uφ()1/p()L(X), then for each fLp()(X),

    |(Muφf)(x)| ess sup y{uφ(y)1/p(y)} |f(x)|,  a.e. in xX.

    Since Lp()(X) is a lattice,

    Mφfp() ess sup y{uφ(y)1/p(y)}fp().

    Hence,

    fφpφ()=inf{λ>0:Xλp(φ(x)) |f(φ(x))|p(φ(x)) dμ1}=inf{λ>0:Xλp(x) |f(x)|p(x) uφ(x) dμ1}=inf{λ>0:Xλp(x) |(Muφf)(x)|p(x) dμ1}=Muφfp() ess sup y{uφ(y)1/p(y)}fp()

    that is, Tφ maps Lp()(X) into Lpφ()(X) and Tesssupy{uφ(y)1/p(y)}, computing with the normalized functions given in the equality of the norm (4.2).

    In the study of the compactness of Cφ over Lp(), the presence of non-atomic sets was a consequence of the regular Ahlfors structure of the space, which was necessary to have at least one continuous composition operator. For the case of the operator Tφ, continuity only requires that the space admits a doubling measure, which is a weaker hypothesis than the Ahlfors regularity. Therefore, to guarantee no atomic sets, we assume that the space is connected.

    Lemma 3. Every connected doubling metric measure space (X,d,μ) does not contain atoms.

    Proof. Assume that EB0 is an atom, then μ(E)>0, which implies μ(EB(w,r))>0 for some wE and all r>0. Hence, in the case μ(EB(w,r))=μ(E) by using [4, Lemma 3.7], there are constants C,σ>0 such that

    μ(E)μ(B(w,r))C rσ Rσ μ(B(w,R)), R>r>0,

    from here that, μ(E)=0 as r0+, which is a contradiction. On another case, μ(EB(w,r))<μ(E), but the atomicity of E implies that μ(EB(w,r))=0, which is a contradiction.

    As a consequence of Lemma 3, the following result is well-know in the framework of non-atomic metric measure spaces (see, [2, Theorem 4.2] and [10, Theorems 5.2 and 5.3]).

    Theorem 5. Assume that (X,d,μ) is a metric measure space with doubling measure, r()P(X) such that 1pp+<+, and φ:XX Borel non-singular map. If X is connected, then the space Lr()(X) does not admit compact composition operators Tφ.

    In the case 1<pp+<+, it is well-know that Lp() is a reflexive space, so every composition operator on Lp() is weakly compact. The non-reflective case (p=1) is different and has been explored in [29] for the constant exponent case. In the following theorem, we provide some results in this direction.

    Denote by λ the Lebesgue measure on [0,1] or R and Ω1:=p1({1}) for an exponent p().

    Theorem 6. Let r()P([0,1]) with λ(Ω1)=0 and r+<. Let φ:[0,1][0,1] be a non-singular map such that

    Tφ:Lr()([0,1])Lrφ()([0,1]).

    Then, the following properties hold:

    (w.1) Tφ maps relatively weakly compact subsets into relatively weakly compact subsets.

    (w.2) Let vφ():=r()1/p(). The operator Tφ is relatively weakly compact if and only if the multiplication operator Mvφ is relatively weakly compact.

    (w.3) Let r=1. If

    M:=infzΩΩ1uφ(z)>0,

    then the operator Tφ:Lr()([0,1])Lrφ()([0,1]) is not weakly compact.

    Proof. To prove (w1), assume that M>0; then since r=1, we may choose a sequence (zn)[0,1]Ω1 satisfying r(zn)1 when n+. So, denote by

    B:=BLr()={fLr()([0,1]):fr()1}.

    Let us reason by contradiction that if Tφ is weakly compact, then the subset Tφ(B) is relatively weakly compact in Lrφ()([0,1]). Hence, by [18, Theorem 4.3] we have

    limλ0+supfBλ1[0,1]|λ|rφ(z) |(Tφf)(z)|rφ(z) dz=0. (4.3)

    Since,

    λ1[0,1]|λ|rφ(z) |(Tφf)(z)|rφ(z) dz=λ1[0,1]|λ|r(z) |f(z)|r(z) uφ(z) dz, (4.4)

    by (4.3) we get

    limλ0+supfBλ1[0,1]|λ|r(z) |f(z)|r(z) uφ(z) dz=0. (4.5)

    Now, let I0:={[a,b]I0:[a,b][0,1]} and we consider the functions f:ΩR given by

    f(x):=fab(x):=(ba)1/r(x) X[a,b](x),  x[0,1].

    So, it is clear that {fab:[a,b]I0}B and thus from (4.5), given ϵ>0, there exists λ0>0 small such that

    1babaλr(z)10  uφ(z) dz<ϵ,   [a,b]I0

    by differentiation,

    λr(z)10 uφ(z)<ϵ,  a.e. in  z[0,1]Ω1.

    In particular, taking z=zn and n+, we obtained M<lim infuφ(zn)=0 because ϵ is taken arbitrarily so M<0, which is a contradiction. The property (w2) follows from (4.4), [18, Theorem 4.3] and from the fact U(φ)<. Finally, the property w3 follows from 4.4 and [18, Theorem 4.3].

    Remark 7. The proof of Theorem 6 can be easily extended to Lr()(R) by applying results recently obtained in [19, Section 5] under the restriction that Ω1 be a null-set.

    The case λ(Ω1)>0 and r=1: Suppose that φ1(Ω1)Ω1, let us choose z0R such that p(z0)=1 and for each nN define In:=(z01/2n,z0+1/2n) so InΩ1 for each nN. We show that Tφ(B) is not relatively weakly compact provided that M>0; define the sequence of measurable functions {fn} by

    fn(x):=1λ(In) XInΩ1(x),  xR.

    It is clear that fnB for every nN. However, from uφ(x)M a.e. xR, we obtain

    φ1(In)Ω1(fnφ)(x) dxInΩ1fn(x) uφ(x) dxM λ(InΩ1)λ(In).

    Taking a subsequence if necessary, let us make λ(In)0, this means λ(φ1(In))0 and by differentiation

    λ(InΩ1)λ(In)1,   n+.

    Therefore,

    lim infφ1(In)Ω1(fnφ)(x) dxM>0,   μ(φ1(In))0.

    Applying [19, Proposition 5.11], we yields the assertion for Tφ(B).

    Lebesgue spaces with variable integrability have proven to be an excellent framework for partial differential equations with non-standard growth. In particular, eigenvalue problems have been analyzed in Sobolev spaces with a constant exponent, where the composition operator has revealed connections with eigenvalue estimates. In this direction, one can not only study the applicability of the composition operator on Sobolev spaces of variable integrability in an n-dimensional Euclidean domain but also extend these techniques when defining such spaces on a complete Riemannian manifold. Therefore, in this work, we outline a possible direction of study within the framework of non-standard function spaces.

    Javier Henríquez-Amador and Carlos Álvarez: Writing-original draft, formal analysis and commenting; Eiver Rodríguez and John Millán: Commenting and review. All authors have read and approved the final version of the manuscript for publication.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The authors thank the anonymous referees for the useful suggestions to improve this article. Carlos F. Álvarez and Jhon Millán were partially supported by inner project BASEX-PD/2024-02 of University of Sinu, Cartagena.

    We declare there are no conflicts of interest associated with this work



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