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Research article

Norms of some operators between weighted-type spaces and weighted Lebesgue spaces

  • Received: 21 October 2022 Revised: 09 November 2022 Accepted: 14 November 2022 Published: 01 December 2022
  • MSC : Primary 47B38, 47A30

  • We calculate the norms of several concrete operators, mostly of some integral-type ones between weighted-type spaces of continuous functions on several domains. We also calculate the norm of an integral-type operator on some subspaces of the weighted Lebesgue spaces.

    Citation: Stevo Stević. Norms of some operators between weighted-type spaces and weighted Lebesgue spaces[J]. AIMS Mathematics, 2023, 8(2): 4022-4041. doi: 10.3934/math.2023201

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  • We calculate the norms of several concrete operators, mostly of some integral-type ones between weighted-type spaces of continuous functions on several domains. We also calculate the norm of an integral-type operator on some subspaces of the weighted Lebesgue spaces.



    By R we denote the set of real numbers, by R+ the interval [0,+), the space of continuous functions on a set Ω we denote by C(Ω), whereas the space of continuously differentiable functions on Ω we denote by C1(Ω). A vector (x1,,xn)Rn we denote by x. If cR, then by c we denote the vector (c,c,,c) (for example, 1=(1,,1)). By x,y we denote the Euclidean inner product of vectors x,yRn, that is, x,y=nj=1xjyj. The Lebesgue measure on Rn we denote by dV(x), whereas by dσ(ζ) we denote the surface measure on the unit sphere SRn. A function w:ΩR is called a weight function or simply weight if it is positive and continuous. The class of all weights on Ω we denote by W(Ω).

    Let wW(Ω). The weighted-type space Cw(Ω) consists of all fC(Ω) such that

    fw:=suptΩw(t)|f(t)|<+. (1.1)

    By using a standard argument, which is applied to the space C(Ω), it is shown that Cw(Ω) is a Banach space. Various weighted-type spaces of continuous or analytic functions and operators on them have been investigated considerably for several decades (see, e.g., [1,2,12,19,25,32,33,34,35,38,42,43,48,50,51] and the related references therein).

    Let Lpw(Rn)=Lpw, where p1 and wW(Rn), be the weighted Lp space consisting of all measurable functions f such that

    fLpw:=(Rn|f(x)|pw(x)dV(x))1/p<+.

    With the norm Lpw the space Lpw is Banach.

    Let X and Y be normed spaces, and L:XY be a linear operator. We say that the operator is bounded if there is M0, such that

    LxYMxX,

    for every xX ([6,26,27,44,45]).

    Norm of the operator is defined by

    LXY=supxBXLxY,

    where BX denotes the unit ball in the space X.

    Finding norms of linear operators is one of the basic problems in operator theory. Many classical results can be found in books and surveys on functional analysis, operator theory and inequalities (see, for example, [6,7,9,10,16,23,26,27,44,45]; see also some of the original sources [13,14,28]). For some recent results in the topic, including some on multi-linear operators (for the definition and some examples see [52,p. 51–55]), see, for example, [4,9,11,20,33,34,35,36,38,40,41,42] and the related references therein.

    Let u be a function defined on Ω. Then by Mu we denote the multiplication operator

    Mu(f)(t)=u(t)f(t),tΩ, (1.2)

    where f is a function on Ω.

    There has been some interest in the multiplication operators on spaces of functions [35,49]. Motivated by some of our previous results on calculating and estimating norms of concrete operators and a problem in [45], here we present some formulas for norms of the multiplication and several integral-type operators between weighted-type spaces. We also calculate norm of an integral-type operator on some subspaces of Lpw(Rn) space. For various integral-type operators see, e.g., [3,4,5,7,8,9,10,16,19,20,21,22,24,29,30,31,32,37,39,40,41,42,43,46,47]. Some of the formulas we have got long time ago, but have never published them. Some of the formulas could be matters of folklore, but we could not found references.

    This section presents our main results and some analyses.

    The following result is a simple and basic one, and should be a matter of folklore. However, it is useful and instructive, because of which we give a proof.

    Theorem 1. Let w1,w2W(Ω). Then the operator Mu:Cw1(Ω)Cw1w2(Ω) is bounded if and only if

    uCw2(Ω). (2.1)

    Moreover, if (2.1) holds then

    MuCw1(Ω)Cw1w2(Ω)=uw2. (2.2)

    Proof. First, assume that condition (2.1) holds, that is, that

    uw2<+. (2.3)

    Then, we have

    Mu(f)w1w2=suptΩw1(t)w2(t)|u(t)f(t)|suptΩw2(t)|u(t)|suptΩw1(t)|f(t)|=uw2fw1

    from which by taking the supremum over the ball BCw1(Ω) we get

    MuCw1(Ω)Cw1w2(Ω)uw2. (2.4)

    From (2.3) and (2.4) the boundedness of the operator Mu:Cw1(Ω)Cw1w2(Ω) follows.

    Now assume that the operator Mu:Cw1(Ω)Cw1w2(Ω) is bounded. Since w1 is a positive continuous function we see that 1/w1 is also such a function. Note that

    1/w1w1=suptΩw1(t)1w1(t)=1. (2.5)

    Further, we have

    Mu(1/w1)w1w2=suptΩw1(t)w2(t)|u(t)1w1(t)|=uw2. (2.6)

    From (2.5), (2.6) and the boundedness of the operator Mu:Cw1(Ω)Cw1w2(Ω) it follows that

    uw2MuCw1(Ω)Cw1w2(Ω)<+, (2.7)

    which means that (2.1) holds.

    If condition (2.1) holds, then from the inequalities in (2.4) and (2.7), we immediately obtain formula (2.2).

    Remark 1. Note that the simple fact in (2.5) plays one of the decisive roles in finding the norm of the operator Mu:Cw1(Ω)Cw1w2(Ω). Related facts are very useful in finding norms of concrete operators acting from weighted-type spaces and will be also used further in this paper.

    Consider the initial value problem

    y(t)=β(t)y(t)+f(t), (2.8)
    y(0)=0, (2.9)

    where f,βC(R+).

    By using the Euler multiplier et0β(ζ)dζ from (2.8) we have

    (y(t)et0β(ζ)dζ)=f(t)et0β(ζ)dζ.

    By integrating the last relation and using condition (2.9), after some calculation, we obtain

    y(t)=t0estβ(ζ)dζf(s)ds. (2.10)

    Note that formula (2.10) presents a linear operator, say, L which is defined as follows

    y(t)=L(f)(t),tR+,

    and acts from C(R+) into the subspace of C1(R+) consisting of all gC1(R+) such that g(0)=0.

    Consider the operator from Cw1(R+) to Cw2(R+). Using the definitions of the spaces Cw1(R+) and Cw2(R+), we have

    L(f)w2=suptR+w2(t)|t0estβ(ζ)dζf(s)ds|fw1suptR+w2(t)t0estβ(ζ)dζdsw1(s),

    from which it follows that

    LCw1(R+)Cw2(R+)suptR+w2(t)t0estβ(ζ)dζdsw1(s). (2.11)

    From (2.5) and since

    L(1/w1)w2=suptR+w2(t)t0estβ(ζ)dζdsw1(s),

    we have

    LCw1(R+)Cw2(R+)suptR+w2(t)t0estβ(ζ)dζdsw1(s). (2.12)

    From (2.11) and (2.12) we obtain

    LCw1(R+)Cw2(R+)=suptR+w2(t)t0estβ(ζ)dζdsw1(s). (2.13)

    From the analysis that we have just conduced it follows that the following result holds.

    Theorem 2. Let w1,w2W(R+), βC(R+) and

    L(f)(t)=t0estβ(ζ)dζf(s)ds. (2.14)

    Then the operator L:Cw1(R+)Cw2(R+) is bounded if and only if

    M:=suptR+w2(t)t0estβ(ζ)dζdsw1(s)<+. (2.15)

    Moreover, if the operator is bounded then

    LCw1(R+)Cw2(R+)=M.

    Let

    fδ:=suptR+eδt|f(t)|,

    where δR+, and let

    Cδ(R+)={fC(R+):fδ<+}.

    The following example shows that for some functions w1,w2 and β the norm of the operator L:Cw1(R+)Cw2(R+) can be explicitly calculated ([45,Problem 7.31]).

    Corollary 1. Let w1(t)=eαt, α0, w2(t)=eγt, β(t)=β, and β>αγ. Then the operator L:Cα(R+)Cγ(R+) is bounded and the following statements hold.

    (a) If α=γ, then

    LCα(R+)Cα(R+)=1βα. (2.16)

    (b) If α>γ, then

    LCα(R+)Cγ(R+)=((αγ)αγ(βγ)βγ)1βα. (2.17)

    Proof. By Theorem 2, we have that formula (2.15) holds with w1(t)=eαt, w2(t)=eγt and β(t)=β, that is,

    LCα(R+)Cγ(R+)=suptR+eγtt0eβ(st)eαsds. (2.18)

    (a) Since α=γ from (2.18) we have

    LCα(R+)Cα(R+)=suptR+e(αβ)tt0e(βα)sds=suptR+1e(βα)tβα=1βα.

    (b) In this case from (2.18) we have

    LCα(R+)Cγ(R+)=suptR+e(γβ)tt0e(βα)sds=suptR+e(γα)te(γβ)tβα. (2.19)

    Let g(t):=e(γα)te(γβ)t, then we have g(0)=0, limt+g(t)=0 (since γ<α<β), and g(t)=e(γβ)t(e(βα)t1)0, tR+. Since

    g(t)=(γα)e(γα)t(γβ)e(γβ)t

    we have that g(t)=0 if and only if

    et=(αγβγ)1αβ.

    Hence,

    suptR+(e(γα)te(γβ)t)=(αγβγ)γααβ(αγβγ)γβαβ=βαβγ(αγβγ)αγβα

    from which together with (2.19) and some calculation, formula (2.17) follows.

    Let

    L(f)(t)=h(t)t10tn0g(s)f(s)ds1dsn, (2.20)

    where t=(t1,,tn), s=(s1,,sn), sj,tjR+, j=¯1,n, and g,hC(Rn+).

    The following theorem is an extension of Theorem 2.

    Theorem 3. Let v,w,h,gW(Rn+) and operator L be given in (2.20). Then the operator L:Cw(Rn+)Cv(Rn+) is bounded if and only if

    ˜M:=suptRn+v(t)h(t)t10tn0g(s)w(s)ds1dsn<+, (2.21)

    and if it is bounded then the norm of the operator is equal to ˜M.

    Proof. Assume that (2.21) holds. Then we have

    L(f)v=suptRn+v(t)h(t)|t10tn0g(s)f(s)ds1dsn|fwsuptRn+v(t)h(t)|t10tn0g(s)w(s)ds1dsn|

    from which along with (2.21) the boundedness of the operator L:Cw(Rn+)Cv(Rn+) follows. Moreover, we have

    LCw(Rn+)Cv(Rn+)˜M. (2.22)

    If the operator L:Cw(Rn+)Cv(Rn+) is bounded, then since the function f0(t)=1w(t) belongs to Cw(Rn+) and f0w=1, we have

    LCw(Rn+)Cv(Rn+)L(f0)v=suptRn+v(t)h(t)|t10tn0g(s)w(s)ds1dsn|, (2.23)

    from which together with the boundedness of the operator L:Cw(Rn+)Cv(Rn+) and positivity of functions g and w we obtain (2.21). From (2.22) and (2.23) we obtain

    LCw(Rn+)Cv(Rn+)=˜M,

    completing the proof.

    The following corollary is an extension of Corollary 1.

    Corollary 2. Let v,wW(Rn+), j=¯1,n, βjC(R+), j=¯1,n, and

    L(f)(t)=t10tn0enj=1sjtjβj(ζj)dζjf(s)ds1dsn. (2.24)

    Then the operator L:Cw(Rn+)Cv(Rn+) is bounded if and only if

    ˆM:=suptRn+v(t)t10tn0enj=1sjtjβj(ζj)dζjds1dsnw(s)<+. (2.25)

    Moreover, if the operator is bounded then

    LCw(Rn+)Cv(Rn+)=ˆM.

    The following integral-type operator is a special case of operator (2.24)

    ˜L(f)(t)=t10tn0enj=1βj(sjtj)f(s)ds1dsn. (2.26)

    Let Cδ, δj0, j=¯1,n, be the class of all fC(Rn+) such that

    fδ=suptRn+enj=1δjtj|f(t)|=suptRn+et,δ|f(t)|<+. (2.27)

    The following consequence of Corollary 2 is an ultimate extension of Corollary 1.

    Corollary 3. Let wj(t)=eαjtj, βj(t)=βj, and βj>αjγj, j=¯1,n. Then the operator ˜L:Cα(Rn+)Cγ(Rn+) is bounded and

    ˜LCα(Rn+)Cγ(Rn+)=αjγj((αjγj)αjγj(βjγj)βjγj)1βjαjαj=γj(1βjαj). (2.28)

    Proof. By using (2.26), (2.27), Corollary 1 and Corollary 2, we have

    ˜LCα(Rn+)Cγ(Rn+)=suptRn+enj=1γjtj|t10tn0enj=1βj(sjtj)ds1dsnnj=1eαjsj|=nj=1suptjR+e(γjβj)tjtj0e(βjαj)sjdsj=αjγj((αjγj)αjγj(βjγj)βjγj)1βjαjαj=γj(1βjαj),

    as desired.

    Remark 2. The norm in formula (2.28) is achieved for the function

    fα(t):=et,α.

    Indeed, we have fαC(Rn+),

    fαα=1, (2.29)

    and

    ˜L(fα)=nj=1suptjR+e(γjβj)tjtj0e(βjαj)sjdsj=αjγj((αjγj)αjγj(βjγj)βjγj)1βjαjαj=γj(1βjαj), (2.30)

    From (2.28)–(2.30) the claim follows.

    Let gC([0,1)n) and

    Tg(f)(x)=nj=1xj1010f(t1x1,,tnxn)g(t1x1,,tnxn)nj=1dtj, (2.31)

    where x[0,1)n. The operator on the polydisk was studied in [32].

    From now on, for the operator in (2.31) we use the notation

    Tg(f)(x)=nj=1xj1010f(tx)g(tx)nj=1dtj.

    By Qγ we denote the space of all fC([0,1)n) such that

    fQγ=supx[0,1)nnj=1(1xj)γj|f(x)|<+,

    where γ=(γ1,,γn) is such that γj>0, j=¯1,n. The quantity Qγ is a norm on the space.

    In the theorem which follows we estimate norm of the operator Tg:QαQα+β1, under some conditions posed on the vectors α and β, and calculate it for a concrete function g.

    Theorem 4. Let α,βRn+ be such that αj+βj>1, j=¯1,n, and

    gQβ<+. (2.32)

    Then the operator Tg:QαQα+β1 is bounded and

    TgQαQα+β1gQβnj=1(αj+βj1). (2.33)

    If additionally

    g(x)=nj=11(1xj)βj (2.34)

    then

    TgQαQα+β1=1nj=1(αj+βj1). (2.35)

    Proof. Suppose that relation (2.32) holds. Let f be an arbitrary function in Qα and x be an arbitrary point in the cube [0,1)n. Then by using the definition of the spaces Qα and Qβ, some known inequalities, as well as some calculations it follows that

    |Tgf(x)|nj=1xj1010|f(tx)g(tx)|nj=1dtjnj=1xj1010|f(tx)|nj=1(1tjxj)αjnj=1(1tjxj)αj+βj|g(tx)|nj=1(1tjxj)βjdtjfQαgQβnj=1xj1010dt1dtnnj=1(1tjxj)αj+βj=fQαgQβnj=110xjdtj(1tjxj)αj+βj=fQαgQβnj=1(αj+βj1)nj=11(1xj)αj+βj1(1xj)αj+βj1,

    from which it follows that

    nj=1(1xj)αj+βj1|Tgf(x)|fQαgQβnj=11(1xj)αj+βj1αj+βj1, (2.36)

    for every x[0,1)n and fQα.

    By taking the supremum in (2.36) over the set [0,1)n, it follows that the following inequality holds

    Tg(f)Qα+β1gQβnj=1(αj+βj1)fQα, (2.37)

    for every fQα.

    By taking the supremum in (2.37) over the unit ball BQβ the boundedness of the operator Tg:QαQα+β1 follows.

    Moreover, from inequality (2.37) we obtain the following estimate for the norm of the operator

    TgQαQα+β1gQβnj=1(αj+βj1). (2.38)

    Now, assume that the operator Tg:QαQα+β1 is bounded and that function g is defined as in (2.34).

    Let

    f0(x)=1nj=1(1xj)αj, (2.39)

    then

    f0Qα=1. (2.40)

    By using (2.34), (2.39) and (2.40), as well as some standard calculations it follows that

    TgQαQα+β1Tg(f0)Qα+β1=supx[0,1)nnj=1xj(1xj)αj+βj1|1010g(tx)nj=1(1tjxj)αjnj=1dtj|=supx[0,1)nnj=1(1xj)αj+βj110xjdtj(1tjxj)αj+βj=supx[0,1)nnj=11(1xj)αj+βj1αj+βj1=nj=11αj+βj1. (2.41)

    From (2.38), (2.41), and since in this case gQβ=1, we have

    TgQαQα+β1=1nj=1(αj+βj1),

    finishing the proof of the theorem.

    Generally speaking operator (2.31) can be considered on functions defined on any set of the form

    nj=1[0,cj)ornj=1[0,cj], (2.42)

    where cj[0,+], j=¯1,n, and where we exclude the case nj=1[0,+].

    Our next result considers the boundedness of operator (2.31) between such spaces.

    Theorem 5. Let u,v,wW(I), gCv(I), where the set I has one of the forms in (2.42). If

    supxIu(x)x10xn0ds1dsnw(s)v(s)<+, (2.43)

    then the operator Tg:Cw(I)Cu(I) is bounded.

    If additionally

    g(x)=1v(x) (2.44)

    then

    T1/vCw(I)Cu(I)=supxIu(x)x10xn0ds1dsnw(s)v(s). (2.45)

    Proof. Using the definitions of the spaces Cw(I) and Cu(I), and the change of variables sj=xjtj, j=¯1,n, we have

    |Tgf(x)|=|nj=1xj1010f(tx)g(tx)nj=1dtj|=|nj=1xj1010w(tx)f(tx)v(tx)g(tx)w(tx)v(tx)nj=1dtj|nj=1xj1010fwgvw(tx)v(tx)nj=1dtj=x10xn0fwgvw(s)v(s)nj=1dsj, (2.46)

    for every xI and fCw(I).

    Multiplying (2.46) by u(x), then taking the supremum over the set I we have

    supxIu(x)|Tgf(x)|fwgvsupxIu(x)x10xn0ds1dsnw(s)v(s)

    from which it follows that

    TgCw(I)Cu(I)gvsupxIu(x)x10xn0ds1dsnw(s)v(s). (2.47)

    Using the assumption gCv(I), (2.43) and (2.47) the boundedness of Tg:Cw(I)Cu(I) follows.

    If (2.44) holds, then

    gv=1. (2.48)

    Now, note that for ˜f0(x)=1w(x) we have

    ˜f0w=1. (2.49)

    Further, we have

    T1/v(˜f0)u=supxIu(x)|T1/v(˜f0)(x)|=supxIu(x)|nj=1xj1010˜f0(tx)g(tx)nj=1dtj|=supxIu(x)|nj=1xj1010dt1dtnw(tx)v(tx)|=supxIu(x)x10xn0ds1dsnw(s)v(s). (2.50)

    From (2.49) and (2.50) we obtain

    supxIu(x)x10xn0ds1dsnw(s)v(s)T1/vCw(I)Cu(I). (2.51)

    Combining (2.47), (2.48) and (2.50) we get (2.45).

    Remark 3. Note that in the case

    w(x)=ex,α and v(x)=ex,β,

    we have

    |Tgf(x)|=|nj=1xj1010f(tx)g(tx)nj=1dtj|=|nj=1xj1010etx,αf(tx)etx,βg(tx)etx,αetx,βnj=1dtj|nj=1xj1010fαgβetx,α+βnj=1dtj=fαgβnj=1xj0e(αj+βj)sjdsj=fαgβnj=11e(αj+βj)xjαj+βj, (2.52)

    from which by taking the supremum in (2.52) over the set Rn+ it follows that

    Tgffαgβ.

    Here, as usual

    h=supxRn+|h(x)|,

    the standard supremum norm.

    Let gC([0,1)n) and

    ˆTg(f)(x)=1010f(t1x1,,tnxn)g(t1,,tn)nj=1dtj, (2.53)

    where xRn. From now on, for the operator in (2.53) we use the notation

    ˆTg(f)(x)=1010f(tx)g(t)nj=1dtj.

    Let uW(Rn) and

    fu=supxRnu(x)|f(x)|.

    The following theorem holds.

    Theorem 6. Let gC([0,1)n), g(x)0, xRn, u,vW(Rn), such that

    u(tx)=nj=1tαjju(x), (2.54)

    for some αjR+, j=¯1,n.

    Then the operator ˆTg:Cu(Rn)Cv(Rn) is bounded if and only if

    supxRn{0}v(x)u(x)1010g(t)nj=1tαjjnj=1dtj<. (2.55)

    Moreover, if the operator ˆTg:Cu(Rn)Cv(Rn) is bounded then

    ˆTgCu(Rn)Cv(Rn)=supxRn{0}v(x)u(x)1010g(t)nj=1tαjjnj=1dtj. (2.56)

    Proof. Assume that (2.55) holds. Let fCu(Rn). Then by using the definition of the norm in Cu(Rn) and (2.54) we have

    |ˆTgf(x)|1010|f(tx)g(t)|nj=1dtjfu1010g(t)u(tx)nj=1dtj=fuu(x)1010g(t)nj=1tαjjnj=1dtj,

    from which it follows that

    v(x)|ˆTgf(x)|fuv(x)u(x)1010g(t)nj=1tαjjnj=1dtj. (2.57)

    By taking the supremum in (2.57) over the set Rn{0}, it follows that the following inequality holds

    ˆTg(f)vfusupxRn{0}v(x)u(x)1010g(t)nj=1tαjjnj=1dtj. (2.58)

    By taking the supremum in (2.58) over the unit ball BCu(Rn) the boundedness of the operator ˆTg:Cu(Rn)Cv(Rn) follows. Moreover, we have

    ˆTgCu(Rn)Cv(Rn)supxRn{0}v(x)u(x)1010g(t)nj=1tαjjnj=1dtj. (2.59)

    Now assume that the operator ˆTg:Cu(Rn)Cv(Rn) is bounded. Let

    ˆf0(x)=1u(x). (2.60)

    Then

    ˆf0u=1. (2.61)

    By using (2.54), (2.60) and (2.61), as well as some standard calculations it follows that

    ˆTgCu(Rn)Cv(Rn)ˆTg(ˆf0)v=supxRn{0}v(x)|1010g(t)u(xt)nj=1dtj|=supxRn{0}v(x)u(x)1010g(t)nj=1tαjjnj=1dtj, (2.62)

    from which (2.55) follows.

    If the operator ˆTg:Cu(Rn)Cv(Rn) is bounded then from (2.59) and (2.62) we get (2.56), finishing the proof of the theorem.

    The following theorem is proved similar to Theorem 6, so we omit the proof.

    Theorem 7. Let gC[0,1), g(t)0, tR, u,vW(Rn), such that

    u(tx)=tαu(x), (2.63)

    for some α>0 and every t[0,1) and xRn, and

    ˆLg(f)(x)=10f(tx)g(t)dt. (2.64)

    Then the operator ˆLg:Cu(Rn)Cv(Rn) is bounded if and only if

    supxRn{0}v(x)u(x)10g(t)tα<+. (2.65)

    Moreover, if the operator ˆLg:Cu(Rn)Cv(Rn) is bounded then

    ˆLgCuCv=supxRn{0}v(x)u(x)10g(t)tα.

    Example 1. Let

    u(x)=xp and v(x)=xq,

    where 1min{p,q}max{p,q}<+ and for r1

    xr=(nj=1|xj|r)1/r.

    Since all the norms on a finite-dimensional linear space are equivalent (here the linear space is Rn), we have that there are positive constants C1 and C2 such that

    C1xqxpC2xq.

    Hence, we have

    supxRn{0}v(x)u(x)1C1<+.

    Note also that in this case we have

    u(tx)=tu(x).

    Hence, to guaranty the boundedness of the operator ˆLg:Cu(Rn)Cv(Rn) in this case, the corresponding condition in (2.65) holds if the function g satisfies the condition

    10g(t)tdt<+.

    Let ˆLpw(Rn)=ˆLpw be a linear subspace of Lpw containing constant functions, and such that the integral means

    Mpp(f,r)=S|f(rζ)|pdσ(ζ)

    are non-increasing for each fˆLpw.

    Example 2. An example of such a space consists of all harmonic functions on Rn [18,31], for which the integral means are nondecreasing functions (see, e.g., [17]; for one-dimensional case see [26]).

    Theorem 8. Let μ be a nonnegative Borel measure on the interval [0,1], wW(Rn) be a radial function such that

    Rnw(x)dV(x)=1, (2.66)

    and

    Lμ(f)(x)=10f(tx)dμ(t). (2.67)

    Then the operator Lμ:ˆLpw(Rn)ˆLpw(Rn) is bounded if and only if

    10dμ(t)<+. (2.68)

    Moreover, if the operator Lμ:ˆLpw(Rn)ˆLpw(Rn) is bounded then

    LμˆLpw(Rn)ˆLpw(Rn)=10dμ(t). (2.69)

    Proof. First assume that (2.68) holds. By using Minkowski's integral inequality (see, e.g., [16,30]), polar coordinates (see, e.g., [18] or [26,p.150]), the assumption that w is radial, i.e., w(rζ)=w(r), x=rζRn, and the monotonicity of the integral means, we have

    Lμ(f)ˆLpw=(Rn|10f(tx)dμ(t)|pw(x)dV(x))1/p10(Rn|f(tx)|pw(x)dV(x))1/pdμ(t)=10(+0S|f(trζ)|pdσ(ζ)w(r)rn1dr)1/pdμ(t)10(+0S|f(rζ)|pdσ(ζ)w(r)rn1dr)1/pdμ(t)=fˆLpw10dμ(t),

    from which it follows that

    LμˆLpwˆLpw10dμ(t). (2.70)

    Now, assume that the operator Lμ:ˆLpw(Rn)ˆLpw(Rn) is bounded. Note that from (2.66) we have

    1ˆLpw=1.

    On the other hand, by the definition of the space ˆLpw, we have ˆf0(x)1ˆLpw. From this and since

    Lμ(ˆf0)ˆLpw=10dμ(t)

    we get

    10dμ(t)LμˆLpwˆLpw. (2.71)

    If the operator Lμ:ˆLpw(Rn)ˆLpw(Rn) is bounded, then from (2.70) and (2.71) we get (2.69).

    Remark 4. The operator in (2.67) is a Hardy integral-type operator [15].

    Here we calculate the norms of several concrete operators between weighted-type spaces of continuous functions on several domains, as well as the norm of an integral-type operator on some subspaces of the weighted Lebesgue spaces. Several methods, ideas and tricks, which could be used in some other settings, are presented.

    The paper was made during the investigation supported by the Ministry of Education, Science and Technological Development of Serbia, contract no. 451-03-68/2022-14/200029.

    The author declares that he has no competing interest.



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