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 c∈R, 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,y∈Rn, 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 S⊂Rn. A function w:Ω→R 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 w∈W(Ω). The weighted-type space Cw(Ω) consists of all f∈C(Ω) such that
‖f‖w:=supt∈Ωw(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 p≥1 and w∈W(Rn), be the weighted Lp space consisting of all measurable functions f such that
‖f‖Lpw:=(∫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:X→Y be a linear operator. We say that the operator is bounded if there is M≥0, such that
‖Lx‖Y≤M‖x‖X, |
for every x∈X ([6,26,27,44,45]).
Norm of the operator is defined by
‖L‖X→Y=supx∈BX‖Lx‖Y, |
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),t∈Ω, | (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,w2∈W(Ω). Then the operator Mu:Cw1(Ω)→Cw1w2(Ω) is bounded if and only if
u∈Cw2(Ω). | (2.1) |
Moreover, if (2.1) holds then
‖Mu‖Cw1(Ω)→Cw1w2(Ω)=‖u‖w2. | (2.2) |
Proof. First, assume that condition (2.1) holds, that is, that
‖u‖w2<+∞. | (2.3) |
Then, we have
‖Mu(f)‖w1w2=supt∈Ωw1(t)w2(t)|u(t)f(t)|≤supt∈Ωw2(t)|u(t)|supt∈Ωw1(t)|f(t)|=‖u‖w2‖f‖w1 |
from which by taking the supremum over the ball BCw1(Ω) we get
‖Mu‖Cw1(Ω)→Cw1w2(Ω)≤‖u‖w2. | (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/w1‖w1=supt∈Ωw1(t)⋅1w1(t)=1. | (2.5) |
Further, we have
‖Mu(1/w1)‖w1w2=supt∈Ωw1(t)w2(t)|u(t)1w1(t)|=‖u‖w2. | (2.6) |
From (2.5), (2.6) and the boundedness of the operator Mu:Cw1(Ω)→Cw1w2(Ω) it follows that
‖u‖w2≤‖Mu‖Cw1(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,β∈C(R+).
By using the Euler multiplier e∫t0β(ζ)dζ from (2.8) we have
(y(t)e∫t0β(ζ)dζ)′=f(t)e∫t0β(ζ)dζ. |
By integrating the last relation and using condition (2.9), after some calculation, we obtain
y(t)=∫t0e∫stβ(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),t∈R+, |
and acts from C(R+) into the subspace of C1(R+) consisting of all g∈C1(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=supt∈R+w2(t)|∫t0e∫stβ(ζ)dζf(s)ds|≤‖f‖w1supt∈R+w2(t)∫t0e∫stβ(ζ)dζdsw1(s), |
from which it follows that
‖L‖Cw1(R+)→Cw2(R+)≤supt∈R+w2(t)∫t0e∫stβ(ζ)dζdsw1(s). | (2.11) |
From (2.5) and since
‖L(1/w1)‖w2=supt∈R+w2(t)∫t0e∫stβ(ζ)dζdsw1(s), |
we have
‖L‖Cw1(R+)→Cw2(R+)≥supt∈R+w2(t)∫t0e∫stβ(ζ)dζdsw1(s). | (2.12) |
From (2.11) and (2.12) we obtain
‖L‖Cw1(R+)→Cw2(R+)=supt∈R+w2(t)∫t0e∫stβ(ζ)dζdsw1(s). | (2.13) |
From the analysis that we have just conduced it follows that the following result holds.
Theorem 2. Let w1,w2∈W(R+), β∈C(R+) and
L(f)(t)=∫t0e∫stβ(ζ)dζf(s)ds. | (2.14) |
Then the operator L:Cw1(R+)→Cw2(R+) is bounded if and only if
M:=supt∈R+w2(t)∫t0e∫stβ(ζ)dζdsw1(s)<+∞. | (2.15) |
Moreover, if the operator is bounded then
‖L‖Cw1(R+)→Cw2(R+)=M. |
Let
‖f‖δ:=supt∈R+eδt|f(t)|, |
where δ∈R+, and let
Cδ(R+)={f∈C(R+):‖f‖δ<+∞}. |
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, α≥0, w2(t)=eγt, β(t)=β, and β>α≥γ. Then the operator L:Cα(R+)→Cγ(R+) is bounded and the following statements hold.
(a) If α=γ, then
‖L‖Cα(R+)→Cα(R+)=1β−α. | (2.16) |
(b) If α>γ, then
‖L‖Cα(R+)→Cγ(R+)=((α−γ)α−γ(β−γ)β−γ)1β−α. | (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,
‖L‖Cα(R+)→Cγ(R+)=supt∈R+eγt∫t0eβ(s−t)e−αsds. | (2.18) |
(a) Since α=γ from (2.18) we have
‖L‖Cα(R+)→Cα(R+)=supt∈R+e(α−β)t∫t0e(β−α)sds=supt∈R+1−e−(β−α)tβ−α=1β−α. |
(b) In this case from (2.18) we have
‖L‖Cα(R+)→Cγ(R+)=supt∈R+e(γ−β)t∫t0e(β−α)sds=supt∈R+e(γ−α)t−e(γ−β)tβ−α. | (2.19) |
Let g(t):=e(γ−α)t−e(γ−β)t, then we have g(0)=0, limt→+∞g(t)=0 (since γ<α<β), and g(t)=e(γ−β)t(e(β−α)t−1)≥0, t∈R+. Since
g′(t)=(γ−α)e(γ−α)t−(γ−β)e(γ−β)t |
we have that g′(t)=0 if and only if
et=(α−γβ−γ)1α−β. |
Hence,
supt∈R+(e(γ−α)t−e(γ−β)t)=(α−γβ−γ)γ−αα−β−(α−γβ−γ)γ−βα−β=β−αβ−γ(α−γβ−γ)α−γβ−α |
from which together with (2.19) and some calculation, formula (2.17) follows.
Let
L(f)(t)=h(t)∫t10⋯∫tn0g(s)f(s)ds1⋯dsn, | (2.20) |
where t=(t1,…,tn), s=(s1,…,sn), sj,tj∈R+, j=¯1,n, and g,h∈C(Rn+).
The following theorem is an extension of Theorem 2.
Theorem 3. Let v,w,h,g∈W(Rn+) and operator L be given in (2.20). Then the operator L:Cw(Rn+)→Cv(Rn+) is bounded if and only if
˜M:=supt∈Rn+v(t)h(t)∫t10⋯∫tn0g(s)w(s)ds1⋯dsn<+∞, | (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=supt∈Rn+v(t)h(t)|∫t10⋯∫tn0g(s)f(s)ds1⋯dsn|≤‖f‖wsupt∈Rn+v(t)h(t)|∫t10⋯∫tn0g(s)w(s)ds1⋯dsn| |
from which along with (2.21) the boundedness of the operator L:Cw(Rn+)→Cv(Rn+) follows. Moreover, we have
‖L‖Cw(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 ‖f0‖w=1, we have
‖L‖Cw(Rn+)→Cv(Rn+)≥‖L(f0)‖v=supt∈Rn+v(t)h(t)|∫t10⋯∫tn0g(s)w(s)ds1⋯dsn|, | (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
‖L‖Cw(Rn+)→Cv(Rn+)=˜M, |
completing the proof.
The following corollary is an extension of Corollary 1.
Corollary 2. Let v,w∈W(Rn+), j=¯1,n, βj∈C(R+), j=¯1,n, and
L(f)(t)=∫t10⋯∫tn0e∑nj=1∫sjtjβj(ζj)dζjf(s)ds1⋯dsn. | (2.24) |
Then the operator L:Cw(Rn+)→Cv(Rn+) is bounded if and only if
ˆM:=supt∈Rn+v(t)∫t10⋯∫tn0e∑nj=1∫sjtjβj(ζj)dζjds1⋯dsnw(s)<+∞. | (2.25) |
Moreover, if the operator is bounded then
‖L‖Cw(Rn+)→Cv(Rn+)=ˆM. |
The following integral-type operator is a special case of operator (2.24)
˜L(f)(t)=∫t10⋯∫tn0e∑nj=1βj(sj−tj)f(s)ds1⋯dsn. | (2.26) |
Let C→δ, δj≥0, j=¯1,n, be the class of all f∈C(Rn+) such that
‖f‖→δ=supt∈Rn+e∑nj=1δjtj|f(t)|=supt∈Rn+e⟨t,→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>αj≥γj, j=¯1,n. Then the operator ˜L:C→α(Rn+)→C→γ(Rn+) is bounded and
‖˜L‖C→α(Rn+)→C→γ(Rn+)=∏αj≠γj((αj−γj)αj−γj(βj−γj)βj−γj)1βj−αj∏αj=γj(1βj−αj). | (2.28) |
Proof. By using (2.26), (2.27), Corollary 1 and Corollary 2, we have
‖˜L‖C→α(Rn+)→C→γ(Rn+)=supt∈Rn+e∑nj=1γjtj|∫t10⋯∫tn0e∑nj=1βj(sj−tj)ds1⋯dsn∏nj=1eαjsj|=n∏j=1suptj∈R+e(γj−βj)tj∫tj0e(βj−αj)sjdsj=∏αj≠γj((αj−γj)αj−γj(βj−γj)βj−γj)1βj−αj∏αj=γj(1βj−αj), |
as desired.
Remark 2. The norm in formula (2.28) is achieved for the function
f→α(t):=e−⟨t,→α⟩. |
Indeed, we have f→α∈C(Rn+),
‖f→α‖→α=1, | (2.29) |
and
‖˜L(f→α)‖=n∏j=1suptj∈R+e(γj−βj)tj∫tj0e(βj−αj)sjdsj=∏αj≠γj((αj−γj)αj−γj(βj−γj)βj−γj)1βj−αj∏αj=γj(1βj−αj), | (2.30) |
From (2.28)–(2.30) the claim follows.
Let g∈C([0,1)n) and
Tg(f)(x)=n∏j=1xj∫10⋯∫10f(t1x1,…,tnxn)g(t1x1,…,tnxn)n∏j=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)=n∏j=1xj∫10⋯∫10f(t⋅x)g(t⋅x)n∏j=1dtj. |
By Q→γ we denote the space of all f∈C([0,1)n) such that
‖f‖Q→γ=supx∈[0,1)nn∏j=1(1−xj)γj|f(x)|<+∞, |
where →γ=(γ1,…,γn) is such that γj>0, j=¯1,n. The quantity ‖⋅‖Q→γ is a norm on the space.
In the theorem which follows we estimate norm of the operator Tg:Q→α→Q→α+→β−→1, under some conditions posed on the vectors →α and →β, and calculate it for a concrete function g.
Theorem 4. Let →α,→β∈Rn+ be such that αj+βj>1, j=¯1,n, and
‖g‖Q→β<+∞. | (2.32) |
Then the operator Tg:Q→α→Q→α+→β−→1 is bounded and
‖Tg‖Q→α→Q→α+→β−→1≤‖g‖Q→β∏nj=1(αj+βj−1). | (2.33) |
If additionally
g(x)=n∏j=11(1−xj)βj | (2.34) |
then
‖Tg‖Q→α→Q→α+→β−→1=1∏nj=1(αj+βj−1). | (2.35) |
Proof. Suppose that relation (2.32) holds. Let f be an arbitrary function in Q→α and x be an arbitrary point in the cube [0,1)n. Then by using the definition of the spaces Q→α and Q→β, some known inequalities, as well as some calculations it follows that
|Tgf(x)|≤n∏j=1xj∫10⋯∫10|f(t⋅x)g(t⋅x)|n∏j=1dtj≤n∏j=1xj∫10⋯∫10|f(t⋅x)|∏nj=1(1−tjxj)αj∏nj=1(1−tjxj)αj+βj|g(t⋅x)|n∏j=1(1−tjxj)βjdtj≤‖f‖Q→α‖g‖Q→βn∏j=1xj∫10⋯∫10dt1⋯dtn∏nj=1(1−tjxj)αj+βj=‖f‖Q→α‖g‖Q→βn∏j=1∫10xjdtj(1−tjxj)αj+βj=‖f‖Q→α‖g‖Q→β∏nj=1(αj+βj−1)n∏j=11−(1−xj)αj+βj−1(1−xj)αj+βj−1, |
from which it follows that
n∏j=1(1−xj)αj+βj−1|Tgf(x)|≤‖f‖Q→α‖g‖Q→βn∏j=11−(1−xj)αj+βj−1αj+βj−1, | (2.36) |
for every x∈[0,1)n and f∈Q→α.
By taking the supremum in (2.36) over the set [0,1)n, it follows that the following inequality holds
‖Tg(f)‖Q→α+→β−→1≤‖g‖Q→β∏nj=1(αj+βj−1)‖f‖Q→α, | (2.37) |
for every f∈Q→α.
By taking the supremum in (2.37) over the unit ball BQ→β the boundedness of the operator Tg:Q→α→Q→α+→β−→1 follows.
Moreover, from inequality (2.37) we obtain the following estimate for the norm of the operator
‖Tg‖Q→α→Q→α+→β−→1≤‖g‖Q→β∏nj=1(αj+βj−1). | (2.38) |
Now, assume that the operator Tg:Q→α→Q→α+→β−→1 is bounded and that function g is defined as in (2.34).
Let
f0(x)=1∏nj=1(1−xj)αj, | (2.39) |
then
‖f0‖Q→α=1. | (2.40) |
By using (2.34), (2.39) and (2.40), as well as some standard calculations it follows that
‖Tg‖Q→α→Q→α+→β−→1≥‖Tg(f0)‖Q→α+→β−→1=supx∈[0,1)nn∏j=1xj(1−xj)αj+βj−1|∫10⋯∫10g(t⋅x)∏nj=1(1−tjxj)αjn∏j=1dtj|=supx∈[0,1)nn∏j=1(1−xj)αj+βj−1∫10xjdtj(1−tjxj)αj+βj=supx∈[0,1)nn∏j=11−(1−xj)αj+βj−1αj+βj−1=n∏j=11αj+βj−1. | (2.41) |
From (2.38), (2.41), and since in this case ‖g‖Q→β=1, we have
‖Tg‖Q→α→Q→α+→β−→1=1∏nj=1(αj+βj−1), |
finishing the proof of the theorem.
Generally speaking operator (2.31) can be considered on functions defined on any set of the form
n∏j=1[0,cj)orn∏j=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,w∈W(I), g∈Cv(I), where the set I has one of the forms in (2.42). If
supx∈Iu(x)∫x10⋯∫xn0ds1⋯dsnw(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/v‖Cw(I)→Cu(I)=supx∈Iu(x)∫x10⋯∫xn0ds1⋯dsnw(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)|=|n∏j=1xj∫10⋯∫10f(t⋅x)g(t⋅x)n∏j=1dtj|=|n∏j=1xj∫10⋯∫10w(t⋅x)f(t⋅x)v(t⋅x)g(t⋅x)w(t⋅x)v(t⋅x)n∏j=1dtj|≤n∏j=1xj∫10⋯∫10‖f‖w‖g‖vw(t⋅x)v(t⋅x)n∏j=1dtj=∫x10⋯∫xn0‖f‖w‖g‖vw(s)v(s)n∏j=1dsj, | (2.46) |
for every x∈I and f∈Cw(I).
Multiplying (2.46) by u(x), then taking the supremum over the set I we have
supx∈Iu(x)|Tgf(x)|≤‖f‖w‖g‖vsupx∈Iu(x)∫x10⋯∫xn0ds1⋯dsnw(s)v(s) |
from which it follows that
‖Tg‖Cw(I)→Cu(I)≤‖g‖vsupx∈Iu(x)∫x10⋯∫xn0ds1⋯dsnw(s)v(s). | (2.47) |
Using the assumption g∈Cv(I), (2.43) and (2.47) the boundedness of Tg:Cw(I)→Cu(I) follows.
If (2.44) holds, then
‖g‖v=1. | (2.48) |
Now, note that for ˜f0(x)=1w(x) we have
‖˜f0‖w=1. | (2.49) |
Further, we have
‖T1/v(˜f0)‖u=supx∈Iu(x)|T1/v(˜f0)(x)|=supx∈Iu(x)|n∏j=1xj∫10⋯∫10˜f0(t⋅x)g(t⋅x)n∏j=1dtj|=supx∈Iu(x)|n∏j=1xj∫10⋯∫10dt1⋯dtnw(t⋅x)v(t⋅x)|=supx∈Iu(x)∫x10⋯∫xn0ds1…dsnw(s)v(s). | (2.50) |
From (2.49) and (2.50) we obtain
supx∈Iu(x)∫x10⋯∫xn0ds1…dsnw(s)v(s)≤‖T1/v‖Cw(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)=e⟨x,→α⟩ and v(x)=e⟨x,→β⟩, |
we have
|Tgf(x)|=|n∏j=1xj∫10⋯∫10f(t⋅x)g(t⋅x)n∏j=1dtj|=|n∏j=1xj∫10⋯∫10e⟨t⋅x,→α⟩f(t⋅x)e⟨t⋅x,→β⟩g(t⋅x)e⟨t⋅x,→α⟩e⟨t⋅x,→β⟩n∏j=1dtj|≤n∏j=1xj∫10⋯∫10‖f‖→α‖g‖→βe⟨t⋅x,→α+→β⟩n∏j=1dtj=‖f‖→α‖g‖→βn∏j=1∫xj0e−(αj+βj)sjdsj=‖f‖→α‖g‖→βn∏j=11−e−(αj+βj)xjαj+βj, | (2.52) |
from which by taking the supremum in (2.52) over the set Rn+ it follows that
‖Tgf‖∞≤‖f‖→α‖g‖→β. |
Here, as usual
‖h‖∞=supx∈Rn+|h(x)|, |
the standard supremum norm.
Let g∈C([0,1)n) and
ˆTg(f)(x)=∫10⋯∫10f(t1x1,…,tnxn)g(t1,…,tn)n∏j=1dtj, | (2.53) |
where x∈Rn. From now on, for the operator in (2.53) we use the notation
ˆTg(f)(x)=∫10⋯∫10f(t⋅x)g(t)n∏j=1dtj. |
Let u∈W(Rn) and
‖f‖u=supx∈Rnu(x)|f(x)|. |
The following theorem holds.
Theorem 6. Let g∈C([0,1)n), g(x)≥0, x∈Rn, u,v∈W(Rn), such that
u(t⋅x)=n∏j=1tαjju(x), | (2.54) |
for some αj∈R+, j=¯1,n.
Then the operator ˆTg:Cu(Rn)→Cv(Rn) is bounded if and only if
supx∈Rn∖{→0}v(x)u(x)∫10⋯∫10g(t)∏nj=1tαjjn∏j=1dtj<∞. | (2.55) |
Moreover, if the operator ˆTg:Cu(Rn)→Cv(Rn) is bounded then
‖ˆTg‖Cu(Rn)→Cv(Rn)=supx∈Rn∖{→0}v(x)u(x)∫10⋯∫10g(t)∏nj=1tαjjn∏j=1dtj. | (2.56) |
Proof. Assume that (2.55) holds. Let f∈Cu(Rn). Then by using the definition of the norm in Cu(Rn) and (2.54) we have
|ˆTgf(x)|≤∫10⋯∫10|f(t⋅x)g(t)|n∏j=1dtj≤‖f‖u∫10⋯∫10g(t)u(t⋅x)n∏j=1dtj=‖f‖uu(x)∫10⋯∫10g(t)∏nj=1tαjjn∏j=1dtj, |
from which it follows that
v(x)|ˆTgf(x)|≤‖f‖uv(x)u(x)∫10⋯∫10g(t)∏nj=1tαjjn∏j=1dtj. | (2.57) |
By taking the supremum in (2.57) over the set Rn∖{→0}, it follows that the following inequality holds
‖ˆTg(f)‖v≤‖f‖usupx∈Rn∖{→0}v(x)u(x)∫10⋯∫10g(t)∏nj=1tαjjn∏j=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
‖ˆTg‖Cu(Rn)→Cv(Rn)≤supx∈Rn∖{→0}v(x)u(x)∫10⋯∫10g(t)∏nj=1tαjjn∏j=1dtj. | (2.59) |
Now assume that the operator ˆTg:Cu(Rn)→Cv(Rn) is bounded. Let
ˆf0(x)=1u(x). | (2.60) |
Then
‖ˆf0‖u=1. | (2.61) |
By using (2.54), (2.60) and (2.61), as well as some standard calculations it follows that
‖ˆTg‖Cu(Rn)→Cv(Rn)≥‖ˆTg(ˆf0)‖v=supx∈Rn∖{→0}v(x)|∫10⋯∫10g(t)u(x⋅t)n∏j=1dtj|=supx∈Rn∖{→0}v(x)u(x)∫10⋯∫10g(t)∏nj=1tαjjn∏j=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 g∈C[0,1), g(t)≥0, t∈R, u,v∈W(Rn), such that
u(tx)=tαu(x), | (2.63) |
for some α>0 and every t∈[0,1) and x∈Rn, 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
supx∈Rn∖{→0}v(x)u(x)∫10g(t)tα<+∞. | (2.65) |
Moreover, if the operator ˆLg:Cu(Rn)→Cv(Rn) is bounded then
‖ˆLg‖Cu→Cv=supx∈Rn∖{→0}v(x)u(x)∫10g(t)tα. |
Example 1. Let
u(x)=‖x‖p and v(x)=‖x‖q, |
where 1≤min{p,q}≤max{p,q}<+∞ and for r≥1
‖x‖r=(n∑j=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
C1‖x‖q≤‖x‖p≤C2‖x‖q. |
Hence, we have
supx∈Rn∖{→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 f∈ˆLpw.
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], w∈W(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
‖Lμ‖ˆLpw(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=rζ∈Rn, and the monotonicity of the integral means, we have
‖Lμ(f)‖ˆLpw=(∫Rn|∫10f(tx)dμ(t)|pw(x)dV(x))1/p≤∫10(∫Rn|f(tx)|pw(x)dV(x))1/pdμ(t)=∫10(∫+∞0∫S|f(trζ)|pdσ(ζ)w(r)rn−1dr)1/pdμ(t)≤∫10(∫+∞0∫S|f(rζ)|pdσ(ζ)w(r)rn−1dr)1/pdμ(t)=‖f‖ˆLpw∫10dμ(t), |
from which it follows that
‖Lμ‖ˆLpw→ˆLpw≤∫10dμ(t). | (2.70) |
Now, assume that the operator Lμ:ˆLpw(Rn)→ˆLpw(Rn) is bounded. Note that from (2.66) we have
‖1‖ˆLpw=1. |
On the other hand, by the definition of the space ˆLpw, we have ˆf0(x)≡1∈ˆLpw. From this and since
‖Lμ(ˆf0)‖ˆLpw=∫10dμ(t) |
we get
∫10dμ(t)≤‖Lμ‖ˆLpw→ˆLpw. | (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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