TWO DIMENSIONAL MELLIN TRANSFORM IN QUANTUM CALCULUS∗
1 Introduction
It is well known that the integral transforms are very important in the areas of science and Engineering,and they attracted the attention of many researchers(see[1–5]).Two of the most frequently used formulas in the area of integral transforms are the classical Mellin transform and the corresponding formal inversion formula;they were successfully applied in the theory of differential equations,plain harmonic problems in special domains,elasticity mechanics,special functions,summing series,and calculating integrals.
In 1854–1933,Hjalmar Mellin defined the Mellin transform of a suitable function f over(0,∞)as
In 2006,A.Fitouhi et al[5]studied the q-analogue of the Mellin transform and its inversion given,respectively,by
and
where Rq,+:={qn,n∈Z}.
As a generalization of the Mellin transform,the two-dimensional Mellin transform is defined by[2,13]
the inversion formula for the two-dimensional Mellin transform is given by the following relation
The q-Jackson integrals from 0 to a and from 0 to∞are defined by[9]
In[8],using two parameters of deformation q1and q2,Haran et al gave the definition of an analogue of the two-dimensional Mellin transform by
The aim of this article is devoted first to study the analogue of the Mellin transform Mq1,q2(f)(1.5)and second to discuss its properties and to give its inversion formula which is an analogue of(1.4).Furthermore,we define the convolution product.And finally as applications,we prove an analogue of the Titchmarsch theorem.
This article is organized as follows:In Section 2,we present some preliminary results and notations that will be useful in the sequel.In Section 3,we introduce the˜q-analogue of the two-dimensional Mellin transform,give some properties,and prove the inversion formula of the ˜q-two dimensional Mellin transform.In Section 4,we study the convolution product and give some relations of the˜q-analogue of the two-dimensional Mellin transform.In Section 5,we give some applications.Finally,in Section 6,we establish Paley-Wiener theorems for the modified-two-dimentional Mellin transform.
2 Basic Definitions
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The q-derivatives Dqf and of a function f are given by[10]:
We also denote
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For q∈(0,1)and a∈C,the q-shifted factorials are defined by
(Dqf)(0)=f′(0)andprovided f′(0)exists.
If f is differentiable,then(Dqf)(x)andtend to f′(x)as q tends to 1.For n ∈ N,we note
The q-derivative of a product
The two-dimensional Mellin convolution product of the functions f and g is defined by
provided the sums converge absolutely.
A q-analogue of the integration by parts formula is given by
Use the q-Jackson integrals from 0 to∞to define the double integrals for q1,q2∈(0,1)by
provided the sums converge absolutely.
The q-analogues of the exponential function are defined by(see[6,15])
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and the q-exponential functions are q-analogues of the classical one and satisfy the relations
and
Jackson defined the q-analogue of the classical gamma function by(see[17–25])
It is well known that it satisfies
The function Γqhas the following q-integral representations
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In[15],Sole A.De and Kac V.G.gave a q-integral representation of Γqbased on the exponential function and gave a q-integral representation of q-Beta function as follows:
For∀s,t> 0,we have
and
where
Moreover,ifwe obtain
Where log(x)means loge(x).
3 The-Two Dimensional Mellin Transform
Definition 3.1Letand f be a function defined on Rq1,+×Rq2,+.Then,the-two dimensional Mellin transform of f is defined by
Remark 3.2It is easy to see that for a suitable function f,M˜q(f)(s,t)tends to M(f)(s,t)when tend to(1,1).
We define the set Hfby
Proposition 3.3If f is a function defined on Rq1,+×Rq2,+,then M˜q(f)is analytic on Hfand we have the followings:
(1) ∀(s,t)∈C2,M˜q(f)(s,t)=M˜q[ilog(x)f(x,y)](s,t);
(2) ∀(s,t)∈C2,M˜q(f)(s,t)=M˜q[ilog(y)f(x,y)](s,t);
(3) ∀(s,t)∈C2,M˜q(f)(s,t)=M˜q[−log(x)log(y)f(x,y)](s,t).
3.1 Properties
In the following subsection,we give some interesting properties of the˜q-two dimensional Mellin transform,which coincide with the classical ones when tend to(1,1).
(P1)For a∈Rq1,+,b∈Rq2,+and(s,t)∈C2,we have
(P2)For(s,t)∈ C2such that(−s,−t)∈ Hf,we have
(P3)For(s,t)∈ C2such that(−s,t)∈ Hf,we have
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(P4)For a,b∈R and(s,t)∈C2such that(s+a,t+b)∈Hf,we have
(P5)For(s,t)∈C2such that(s−1,t)∈Hf,we have
The proof of all previous properties are easily established by using the definition of the ˜q-two dimensional Mellin transform and the properties of the q-Jackson integrals mentioned before.
(P7)For(s,t)∈C2such that(s−1,t−1)∈Hf,we have
By induction,it is obtained that:for n,m∈N∗and(s,t)∈C2such that(s−n,t−m)∈Hf,
Using classical arguments,one can easily prove the following result.
(P9)For(s,t)∈C2such that(s,t−1)∈ Hf,we have
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(P10)For(s,t)∈C2such that(s+1,t)∈Hf,we have
(P11)For(s,t)∈C2such that(s,t+1)∈Hf,we have
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(P12)For τ>0,ρ >0 and(s,t)∈C2such that∈Hf,we have
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(P13)Let(µk)kand(νk)kbe two sequences of Rq1,+ × Rq2,+,let(λk)kbe a sequence of C,and let f be a suitable function,then we have
provided the sums converge.
(P6)For(s,t)∈C2such that(s,t−1)∈ Hf,we have
Example 3.4 Let q1=q2=q, s=n,and t=m such that n,m∈N∗and the functionSuppose thatthen by formulas(2.11),(2.7),and(2.13),we have
3.2-Two Dimensional Mellin Inversion Formula
Theorem 3.5 Let f be a function defined on Rq1,+×Rq2,+and let(c1,c2)∈Hf∩R2,then for all(x,y)∈Rq1,+×Rq2,+,we have
Proof By definition,we have
Multiplying the both sides of(3.3)byand integrating with respect to t fromtowe get
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Now,multiplying the both sides of(3.4)bythen integrating the resulting identity with respect to s fromthe result follows.
4-Two Dimensional Mellin’s Convolution Product
Definition 4.1The-two dimensional Mellin convolution of the functions f and g is the function f∗M˜qg defined by
provided the double integral exists.
(P8)For(s,t)∈C2such that(s−1,t)∈Hf,we have
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Proposition 4.2If the-two dimensional Mellin convolution product of f and g exists,then
Proposition 4.3 For a suitable functions f and g,the following relations holds:
For the convenience of the reader,in this section we provide a summary of the mathematical notations and definitions used in this article(see[6,9,10]).
and
Proof (1)From relation(4.3)and the inversion formula,we have,for x=1 and y=1,
(2)LetApplying relation(4.4)for the functions f and h,relation(4.5)follows.
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5 Applications
Application 5.1-double integral equations
Lemma 5.1 Let k and g be a pair functions defined on Rq1,+×Rq2,+such that the set Ik,g=Hk∩{(1−s,1−t),(s,t)∈Hg}is not empty.Put
Then,
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ProofWe have
and we make the change of variable:xu=z and yv=w,then,we obtain
whereThus,from the properties(P4)and formula(4.3),the result follows.
Theorem 5.2 Let k and g be two functions defined on Rq1,+×Rq2,+.For a suitable reals c1and c2,put for all(x,y)∈Rq1,+×Rq2,+,
and suppose that the set IL,g=HL∩{(1−s,1−t),(s,t)∈Hg}is not empty.Then,the following integral equation:
has the solution
Furthermore,if
equation(5.4)has the solution
Proof From formula(5.4),we get
then,
By(3.2),we obtain
Application 5.2 Analogue of the Titchmarsh Theorem.
Theorem 5.3 Let k be a function defined on Rq1,+×Rq2,+such that the set Hkis not empty.If the integral equation
has a suitable solution f,then,for every s,t∈C such that(s,t)and(1−s,1−t)∈Hk,we have
Proof The integral equation(5.8)may be written as a pair of reciprocal formulas:
and
Using Lemma 5.1,we obtain
and
Changing s into 1−s and t into 1−t in one of these equations and multiplying,we deduce that
6Paley-Wiener Thoeremes for the Modified-two Dimentional Mellin Transform
Definition 6.1 Let f be a function defined on Rq1,+×Rq2,+,we define the modified-double Mellin transformof f as
Proposition 6.2Let f be a function defined on Rq1,+×Rq2,+,the modified˜q-double Mellin transformof f is aperiodic function.
Proof Using(2.8),we have
For all n,m∈N,we have
then for a polynomial function P(·,·),we have
We consider
and
The notation is induced by two norm
and
Theorem 6.3Let f be a function defined on J such thatThen,∈L∞(I,dsdt)and
Proof For all(s,t)∈I,we have
then
Theorem 6.4(Plancherel formula) Let f be a function on J such thatThen,M˜q(f)∈L2(I,dsdt)and
Proof Using(4.5)and(P4),we have
Thus,
Theorem 6.5(Hausdorff-Young inequality) Let f be a function defined on J and 1 ≤n≤2(resp.n=1)such thatThen,for m=(resp.m=∞),we have∈Lm(I,dsdt)and
ProofLet T be the linear operator defined by T(f)=From Theorem 6.3,we have,for all
and from Theorem 6.4,we have,for all
then,from the Riesz-Thorin interpolation theorem(see[14]),we have
We begin by the following useful Lemma.
Lemma 6.6 Let p>0,and F and Q be two functions defined on J,such that QnF∈for all n=0,1,2,···,then
Proof The case F=0 is trivial.Suppose now that F/=0 and we define the measureµon J by
then,we haveµ(J)=1 and
On the other hand,we have
and
Then,we obtain
Thus,Lemma 6.6 is proved.
Theorem 6.7 Let f be a function defined on J such that
then
In particular,supp(f)∩J⊂Ω,if and only if
Proof By relation(6.1)and the Plancherel formula,we have
On the other side,Lemma 6.6 gives
Then,the fact that supp(f)∩J⊂Ω shows that
and the result follows.
We can show easily a particular case for
Owing to the Hausdorff-Young inequality,the previous theorem can be generalized by the substitution of the L2norm by an Lpnorm,2≤p≤∞.This is the aim of the following result.
Theorem 6.8 Let 2≤ p≤ ∞ and P be a polynomial function with real coefficients,satisfying
Proof For 2 ≤ p ≤ ∞,we note p′,its conjugate number(that is,+=1).If 2≤ p< ∞,then from the Hausdorff-Young inequality and relation(6.1),we have
So,by Lemma 6.6,we get
Now,if p= ∞,from Theorem 6.3 and by the q-Hölder inequality(see[12]),we obtain
Consequently,
As well,the use of Lemma 6.6 gives
On the other hand,asis aperiodic function,then by partial integration,we get
So,by the q-Hölder inequality(see[12]),we obtain
And,from Theorem 6.7,we obtain
Thus,we changein formula(6.4),then,we obtain
Therefore,
Finally,the result follows from this relation and formulas(6.2)and(6.3).
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