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DOI 10.1007/s13370-017-0509-5

Fourier-Bessel Dini Lipschitz functions in the space L 2 α, n

S. El Ouadih

1

· R. Daher

1

Received: 26 June 2015 / Accepted: 6 June 2017

© African Mathematical Union and Springer-Verlag GmbH Deutschland 2017

Abstract In this paper, using a generalized translation operator, we obtain an analog of Younis’s Theorem 5.2 in Younis (Int J Math Math Sci 9:301–312, 1986) for the generalized Fourier-Bessel transform for functions satisfying the Fourier-Bessel Dini Lipschitz condition in the space L

2α,n

.

Keywords Singular differential operator · Generalized Fourier-Bessel transform · Generalized translation operator

Mathematics Subject Classification Primary 46L55 · Secondary 44B20

1 Introduction and preliminaries

Integral transforms and their inverses the Bessel transform are widely used to solve various problems in calculus, mechanics, mathematical physics, and computational mathematics (see [3,7]).

In this article, we obtain an analog of Younis’s Theorem 5.2 in [5] on description of the image under the generalized Fourier-Bessel transform of a class of functions satisfying the Dini Lipschitz condition in weighted function spaces on [ 0 , ∞[ . We now give the exact statement of this theorem.

Suppose that f (x ) is a function in the L

2

(R) space (all functions below are complex- valued), .

L2(R)

is the norm of L

2

(R), and δ is an arbitrary number in the interval (0, 1).

B

S. El Ouadih

[email protected] R. Daher

[email protected]

1 Department of Mathematics, Faculty of Sciences Aïn Chock, University Hassan II, Casablanca, Morocco

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Theorem 1.1 [12, Theorem 85] Let fL

2

(R) . Then the following conditions are equiva- lents:

(i) f ( x + h )f ( x )

L2(R)

= O ( h

δ

) , as h → 0, 0 < δ < 1, (ii)

|λ|≥r

| f (λ)|

2

= O(r

−2δ

) as r → ∞, where f stands for the Fourier transform of f .

This theorem has been generalized in the case of noncompact rank 1 Riemannian symmet- ric spaces [10], and was extented in [11] for the generalized Fourier transform in the space L

2

(R

n

) using a spherical mean operator. The Titchmarsh’s Theorem has been generalized recently for a class of functions satisfying the Lipschitz condition for the Fourier-Bessel transform in [8,9].

On the other hand, Younis Theorem 5.2 [5] characterized the set of functions in L

2

(R) satisfying the Dini Lipschitz condition by means of an asymptotic estimate growth of the norm of their Fourier transforms, namely we have:

Theorem 1.2 [5] Let fL

2

(R) . Then the following are equivalents:

(a) f ( x + h )f ( x ) = O

hη (log1h)γ

, as h → 0 , 0 < η < 1 , γ ≥ 0, (b)

|λ|≥r

| f (λ)|

2

= O

r

−2η

(log r)

, as r → ∞, where f stands for the Fourier transform of f .

In this paper, we consider a second-order singular differential operator B on the half line which generalizes the Bessel operator B

α

. We obtain an analog of Theorem 1.2 for the generalized Fourier-Bessel transform associated to B in L

2α,n

. For this purpose, we use a generalized translation operator.

We briefly overview the theory of generalized Fourier-Bessel transform and related har- monic analysis (see [1,6])

Consider the second-order singular differential operator on the half line B f (x ) = d

2

f ( x )

d x

2

+ ( 2 α + 1 ) x

d f ( x )

d x − 4n + n ) x

2

f (x),

where α >

−12

and n = 0 , 1 , 2 , .... For n = 0, we obtain the classical Bessel operator B

α

f ( x ) = d

2

f ( x )

d x

2

+ ( 2 α + 1 ) x

d f ( x ) d x . Let M be the map defined by

M f (x ) = x

2n

f (x), n = 0, 1, ....

Let L

α,np

, 1 ≤ p < ∞ , be the class of measurable functions f on [ 0 , ∞[ for which f

p,α,n

= M

−1

f

p,α+2n

< ∞,

where

f

p,α

=

0

| f ( x )|

p

x

2α+1

d x

1/p

.

If p = 2, then we have L

2α,n

= L

2

([0, ∞[, x

2α+1

).

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For α

−12

, we introduce the Bessel normalized function of the first kind j

α

defined by j

α

( z ) = + 1 )

n=0

(− 1 )

n

z

2

2n

n !( n + α + 1 ) , z ∈ C, (1)

where ( x ) is the gamma-function (see [4]). The function y = j

α

( x ) satisfies the differential equation

B

α

y + y = 0,

with the condition initial y(0) = 0 and y

(0) = 0. The function j

α

(x ) is infinitely differen- tiable, even, and, moreover entire analytic.

From (1) we see that

z

lim

→0

j

α

( z ) − 1

z

2

= 0 , (2)

by consequence, there exists c > 0 and η > 0 satisfying

|z| ≤ η ⇒ | j

α

(z) − 1| ≥ c|z|

2

. (3) From [2], we have

| j

α

(x )| ≤ 1, (4)

1 − j

α

( x ) = O ( x

2

), 0 ≤ x ≤ 1 . (5) For λ ∈ C , and x ∈ R , put

ϕ

λ

( x ) = x

2n

j

α+2n

x ). (6)

From [1,6] recall the following properties.

Proposition 1.3

(c) ϕ

λ

satisfies the differential equation

B ϕ

λ

= −λ

2

ϕ

λ

. (d) For all λ ∈ C, and x ∈ R

λ

(x )| ≤ x

2n

e

|I mλ||x|

.

The generalized Fourier-Bessel transform we call the integral transform (see [1]) F

B

f (λ) =

0

f (x

λ

(x )x

2α+1

d x, λ ≥ 0, fL

1α,n

.

Let fL

1α,n

such that F

B

( f )L

1α+2n

= L

1

([ 0 , ∞[, x

2α+4n+1

d x ) . Then the inverse generalized Fourier-Bessel transform is given by the formula (see [1])

f (x ) =

0

F

B

f (λ)ϕ

λ

(x)dμ

α+2n

(λ), where

d μ

α+2n

(λ) = a

α+2n

λ

2α+4n+1

dλ, a

α

= 1

4

α

((α + 1))

2

.

From [1,6], we have

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Proposition 1.4

(e) For every fL

1α,n

L

2α,n

we have the Plancherel formula

+∞

0

| f (x )|

2

x

2α+1

d x =

+∞

0

| F

B

f (λ)|

2

α+2n

(λ).

(f) The generalized Fourier-Bessel transform F

B

extends uniquely to an isometric isomor- phism from L

2α,n

onto L

2

([ 0 , +∞[, μ

α+2n

) .

Define the generalized translation operator T

h

, h ≥ 0 by the relation T

h

f ( x ) = ( x h )

2n

τ

α+2nh

( M

−1

f )( x ), x ≥ 0 , where τ

αh

are the Bessel translation operators of order α defined by

τ

αh

f ( x ) = c

α

π

0

f ( x

2

+ h

2

− 2x hcost ) si n

tdt , where

c

α

=

π

0

si n

tdt

1

= + 1 )

(π)

α +

12

. For fL

2α,n

, we have (see [1])

F

B

( T

h

f )(λ) = ϕ

λ

( h ) F

B

( f )(λ), (7)

F

B

( B f )(λ) = −λ

2

F

B

( f )(λ). (8)

2 Fourier-Bessel Dini Lipschitz condition

Definition 2.1 Let fL

2α,n

, and let

T

h

f (x)h

2n

f (x)

2,α,n

C h

η+2n

log

1h

γ

, γ ≥ 0, i.e.,

T

h

f (x )h

2n

f (x )

2,α,n

= O

h

η+2n

log

1h

γ

,

for all x in R

+

and for all sufficiently small h, C being a positive constant . Then we say that f satisfies a Fourier-Bessel Dini Lipschitz of order η, or f belongs to Lip(η, γ ).

Definition 2.2 If however

T

h

f ( x )h

2n

f ( x )

2,α,n hη+2n

log1h

γ

→ 0 , as h → 0 , γ ≥ 0 ,

i.e.,

T

h

f (x)h

2n

f (x)

2,α,n

= o

h

η+2n

log

h1

γ

,

then f is said to be belong to the little Fourier-Bessel Dini Lipschitz class lip(η, γ ).

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Remark It follows immediately from these definitions that lip(η, γ )Lip(η, γ ).

Theorem 2.3 Let η > 1. If f ∈ Lip(η, γ ), then flip(1, γ ).

Proof For x ∈ R

+

and h small, fLip(η, γ ) we have T

h

f (x)h

2n

f (x)

2,α,n

C h

η+2n

log

h1

γ

.

Then

log 1 h

γ

T

h

f ( x )h

2n

f ( x )

2,α,n

C h

η+2n

. Therefore

log

h1

γ

h

1+2n

T

h

f (x )h

2n

f (x )

2,α,n

C h

η−1

, which tends to zero with h → 0. Thus

log

1h

γ

h

1+2n

T

h

f ( x )h

2n

f ( x )

2,α,n

→ 0 , h → 0 .

Then flip ( 1 , γ ) .

Theorem 2.4 If η < ν , then Lip (η, 0 )Lip (ν, 0 ) and lip (η, 0 )lip (ν, 0 ).

Proof We have 0 ≤ h ≤ 1 and η < ν , then h

ν

h

η

.

Then the proof of this theorem.

3 New results on Fourier-Bessel Dini Lipschitz class Lemma 3.1 For fL

2α,n

, we have

h

4n

0

| j

α+2n

h ) − 1 |

2

| F

B

f (λ)|

2

d μ

α+2n

(λ)

1

2

= T

h

f ( x )h

2n

f ( x )

2,α,n

. where m = 0, 1, 2...

Proof We use the formulas (6) and (7) we conclude that

F

B

( T

h

f )(λ) = h

2n

j

α+2n

h ) F

B

f (λ).

Then

F

B

((T

h

h

2n

I ) f )(λ) = h

2n

( j

α+2n

(λh) − 1) F

B

f (λ).

By Proposition 1.4, we have the result.

Theorem 3.2 Let η > 2. If f belong to the Fourier-Bessel Dini Lipschitz class, i.e., fLip (η, γ ), η > 2 , γ ≥ 0 .

Then f is equal to the null function in R

+

.

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Proof Assume that fLip (η, γ ) . Then

T

h

f (x )h

2n

f (x )

2,α,n

C h

η+2n

log

1h

γ

, γ ≥ 0.

From Lemma 3.1, we have h

4n

0

| j

α+2n

h ) − 1 |

2

| F

B

f (λ)|

2

d μ

α+2n

(λ)C

2

h

2η+4n

log

1h

2γ

. Therefore

0

| j

α+2n

(λh) − 1|

2

| F

B

f (λ)|

2

α+2n

(λ)C

2

h

log

1h

.

Then

0

| j

α+2n

h ) − 1 |

2

| F

B

f (λ)|

2

d μ

α+2n

(λ)

h

4

C

2

h

2η−4

log

1h

, Since η > 2 we have

h

lim

→0

h

2η−4

log

1h

= 0 . Then

h

lim

→0

0

| 1 − j

α

h )|

λ

2

h

2

2

λ

4

| F

B

f (λ)|

2

d μ

α+2n

(λ) = 0 . and also from the formula (2) and Fatou Theorem, we obtain

0

λ

4

| F

B

f (λ)|

2

d μ

α+2n

(λ) = 0 .

Thus λ

2

F

B

f (λ) = 0 for all λ ∈ R

+

, then f is the null function.

Analog of the Theorem 3.2, we obtain this theorem.

Theorem 3.3 Let fL

2α,n

. If f belong to lip(2, 0). i.e.,

T

h

f (x )h

2n

f (x)

2,α,n

= O(h

2

), as h → 0.

Then f is equal to null function in R

+

.

Now, we give another the main result of this paper analog of Theorem 1.2.

Theorem 3.4 Let fL

2α,n

. Then the following conditions are equivalents (i) fLip(η, γ ) , 0 < η < 1, γ ≥ 0,

(ii)

r

| F

B

f (λ)|

2

α+2n

(λ) = O

r

−2η

(log r)

, as r → ∞.

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Proof ( i )( ii ) . Suppose that fLip (η, γ ) . Then T

h

f (x )h

2n

f (x )

2,α,n

= O

h

η+2n

log

1h

γ

, h → 0.

From Lemma 3.1, we have T

h

f ( x )h

2n

f ( x )

22,α,n

= h

4n

0

| j

α+2n

h ) − 1 |

2

| F

B

f (λ)|

2

d μ

α+2n

(λ).

By formula (3), we get

η

h η 2h

| j

α+2n

(λh) − 1|

2

| F

B

f (λ)|

2

α+2n

(λ)c

2

η

4

2

4

η

h η 2h

| F

B

f (λ)|

2

d μ

α+2n

(λ).

There exists then a positive constant C such that

η

h η 2h

| F

B

f (λ)|

2

α+2n

(λ)C

η

h η 2h

| j

α+2n

(λh) − 1|

2

| F

B

f (λ)|

2

α+2n

(λ)

C

h

4n

T

h

f (x )h

2n

f (x)

22,α,n

= O

h

2η

log

1h

2γ

.

We obtain

2r

r

| F

B

f (λ)|

2

d μ

α+2n

(λ)C

r

−2η

(log r)

2γ

, where C

is a positive constant. Now,

r

| F

B

f (λ)|

2

d μ

α+2n

(λ) =

i=0

2i+1r

2ir

| F

B

f (λ)|

2

d μ

α+2n

(λ)

C

r

−2η

(log r)

+ (2r)

−2η

(log 2r)

+ (4r)

−2η

(log 4r)

+ · · ·

C

r

−2η

( log r )

1 + 2

−2η

+ ( 2

−2η

)

2

+ ( 2

−2η

)

3

+ · · ·

K

η

r

−2η

(log r)

, where K

η

= C

(1 − 2

−2η

)

−1

since 2

−2η

< 1.

Consequently

r

| F

B

f (λ)|

2

d μ

α+2n

(λ) = O

r

2η

( log r )

2γ

, as r → ∞.

(ii )(i). Suppose now that

r

| F

B

f (λ)|

2

α+2n

(λ) = O

r

2η

( log r )

2γ

, as r → ∞,

(8)

and write

T

h

f ( x )h

2n

f ( x )

22,α,n

= h

4n

( I

1

+ I

2

), where

I

1

=

1/h

0

| j

α+2n

h ) − 1 |

2

| F

B

f (λ)|

2

d μ

α+2n

(λ), and

I

2

=

1/h

| j

α+2n

h ) − 1 |

2

| F

B

f (λ)|

2

d μ

α+2n

(λ).

Using the inequality (4), we get I

2

≤ 4

1/h

| F

B

f (λ)|

2

d μ

α+2n

(λ) = O

h

log

1h

, as h → 0 . Set

φ(λ) =

λ

| F

B

f (x )|

2

α+2n

(x).

From formula (5) and integration by parts, we have I

1

= −

1/h

0

| j

α+2n

h ) − 1 |

2

(λ) d λ

≤ −h

2

1/h

0

λ

2

φ

(λ)dλ

≤ −φ 1

h

+ 2h

2

1/h

0

λφ(λ)dλ

≤ 2h

2

1/h

0

λ

1−2η

(log λ)

−2γ

C

1

h

log

h1

where C

1

is a positive constant, and this ends the proof.

References

1. Al Subaie, R.F., Mourou, M.A.: The continuous wavelet transform for a Bessel type operator on the half line. Math. Stat.1(4), 196–203 (2013)

2. Abilov, V.A., Abilova, F.V.: Approximation of functions by Fourier-Bessel sums. Izv. Vyssh. Uchebn.

Zaved. Mat.8, 3–9 (2001)

3. Vladimirov, V.S.: Equations of mathematical physics, Marcel Dekker, New York, 1971, Nauka, Moscow (1976)

4. Levitan, B.M.: Expansion in Fourier series and integrals over Bessel functions. Uspekhi Math. Nauk6(2), 102–143 (1951)

5. Younis, M.S.: Fourier transforms of Dini-Lipschitz functions. Int. J. Math. Math. Sci.9(2), 301–312 (1986). doi:10.1155/S0161171286000376

6. Al Subaie, R.F., Mourou, M.A.: Transmutation operators associated with a Bessel type operator on the half line and certain of their applications. Tamsii. oxf. J. Inf. Math. Scien29(3), 329–349 (2013)

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7. Sveshnikov, A.G., Bogolyubov, A.N., Kratsov, V.V.: Lectures on mathematical physics, Nauka, Moscow (2004) (in Russian)

8. Daher, R., El Hamma, M., El Ouadih, S.: An analog of Titchmarsh’s Theorem for the Generalized Fourier- Bessel transform. Lobachevskii J. Math.37(2), 114–119 (2016)

9. El Ouadih, S., Daher, R.: Generalized Fourier-Bessel transform of(η, γ )-Bessel-Lipschitz functions in the spaceLα,pn. MATEMATIKA31(2), 143–148 (2015)

10. Platonov, S.S.: The Fourier transform of functions satisfying the Lipschitz condition on rank 1 symmetric spaces. Sib. Math. J46(6), 1108–1118 (2005)

11. Daher, R., Boujeddaine, M., El Hamma, M.: Generalization of Titchmarsh’s theorem for the Fourier transform in the SpaceL2(Rn), Afr. Mat. doi:10.1007/s13370-015-0368-x

12. Titchmarsh, E.C.: Introduction to the theory of Fourier Integrals. Claredon , oxford, 1948, Komkniga.

Moxow (2005)

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