• Tidak ada hasil yang ditemukan

1 Introduction - Eurasian mathematical journal

N/A
N/A
Protected

Academic year: 2024

Membagikan "1 Introduction - Eurasian mathematical journal"

Copied!
9
0
0

Teks penuh

(1)

Volume 6, Number 1 (2015), 76 – 84

BOCHKAREV INEQUALITY FOR THE FOURIER TRANSFORM OF FUNCTIONS IN THE LORENTZ SPACES L2,r(R)

G.K. Mussabayeva, N.T. Tleukhanova Communicated by N.A. Bokayev Key words: Lorentz spaces, Fourier transform.

AMS Mathematics Subject Classification: 42B10.

Abstract. In this article we prove an analogue of Hardy -Littlewood- Stein inequality for the Fourier transform in Lorentz space L2,r(R).

1 Introduction

Let f(x) be a scalar-valued µ measurable function which is finite almost everywhere, we introduce the distribution function m(σ, f) defined by

m(σ, f) = µ({x:|f(x)|> σ}) and f its non-increasing rearrangement of the function f.

f(t) = inf{σ :m(σ, f)6t}. (1.1) In [1], the Lorentz space Lp,q is defined that f ∈Lp,q,16p6∞,if and only if

kfkLp,q =

 Z

R

t1pf(t)q dt t

1 q

<∞

when 16q <∞,

kfkLp,∞ = sup

t

t1pf(t) when q =∞.

Well-known classical theorem Hausdorff-Young [11], whereby iff(x)is a 1- periodic function and satisfying

1

Z

0

|f(x)|pdx <∞, 1< p 62, then following relation holds

+∞

X

n=−∞

|cn|p0

!p10

6

1

Z

0

|f(x)|pdx

1 p

, (1.2)

(2)

where

cn=

1

Z

0

f(x)e−2πinxdx, n ∈Z

are the Fourier coefficients of f(x) and p0 = p−1p .

An analogue of theorem Hausdorff-Young for the Fourier transform was proved by Titchmarsh [9],[10] and the inequality of Titchmarsh for Fourier integrals

Z

−∞

fb(ξ)

p0

1 p0

6

Z

−∞

|f(x)|pdx

1 p

, (1.3)

where

fb(ξ) =

Z

−∞

f(x)e−2πixξdx

is Fourier transform of f(x).

The Hardy-Littlewood inequalities for the Lorentz spaces Lp,q(R) was proved by Stein [3]-[8]:

Let1< p <2, 16q 6∞and p0 = p−1p , then

X

k=1

kp10ckq 1 k

!1q

6CkfkLp,q[0,1], (1.4)

where ck is a non-increasing rearrangement of the Fourier coefficients.

kfbkLp0,q(R) 6CkfkLp,q(R), (1.5) Unlike inequalities (1.2) and (1.3), relations (1.4) and (1.5) don’t cover the case ofp= 2.

S.V.Bochkarev in [2] for the Fourier transform on the torus has shown that the Hardy -Littlewood- Stein inequality is not the case.

Theorem A. Let {ϕn}n=1 be an orthonormal system of complex-valued functions on [0,1], such that

nk6M, n= 1,2, ....

let f ∈L2,r[0,1], 2< r6∞. Then the inequality

sup

n∈N

1

|n|12(log(n+ 1))121r

n

X

m=1

am 6CkfkL2,r[0,1] (1.6) holds, where an are the Fourier coefficients of the system {ϕn}n=1.

(3)

2 Main result

The aim of this paper is to obtain an analogue of Bochkarev theorem for the Fourier transform. The main result of this paper is the following.

Theorem 2.1. Let <N = {A =

N

S

i=1

Ai, where Ai are segments in R}. Then for any function f ∈L2,r(R) and 2< r <∞ we have the inequality

sup

N>8

sup

A⊂<N

1

|A|12 log2(1 +N)121r Z

A

fˆ(ξ)dξ

623kfkL2,r. (2.1)

To prove Theorem 2.1, we establish the following lemmas.

Lemma 2.1. Let 43 < q < 2 < r < 4 and f ∈ Lq,r(R). Then for any measurable set A of finite measure of <N, the inequality

1

|A|1q Z

A

f(ξ)dξˆ

62 q

2−q

q10(r−2r )

kfkLq,r(R) (2.2)

holds.

Proof.

Z

A

f(ξ)dξˆ

6 Z

A

Z

−∞

f(t)e−iξtdtdξ

6|A|kfkL1

and from the Plancherel’s theorem, we have

Z

A

fˆ(ξ)dξ

6|A|12kfkL2.

Let τ ∈(0,+∞). Define

f1(x) =

f(x), if |f(x)|6f(τ), 0, otherwise,

f0(x) =f(x)−f1(x).

Then, for any0< τ <∞, we have

Z

A

f(ξ)dξˆ

6 Z

A

0(ξ)dξ

+ Z

A

1(ξ)dξ

6|A|

τ

Z

0

f(s)ds+|A|12

Z

τ

(f(s))2ds

1 2

.

(4)

Using Holder’s inequality, we obtain

Z

A

fˆ(ξ)dξ

6

|A|

τ

Z

0

t1qf(t) r dt

t

1

r

τ

Z

0

tr

0 q0dt

t

1 r0

+|A|12

Z

τ

t1qf(t)r dt t

1

r

Z

τ

t1−2qr−2r dt t

r−2 2r

6kfkLq,r |A|τ1−1q

1−1 q

1r−1

+|A|12τ121q

r(2−q) q(r−2)

1r12! .

Now let τ = q(r−2)

r(2−q)

r−2r

q q−1

2(1−r)r

/|A| and using the 43 < q < 2 < r < 4, we can estimate

Z

A

f(ξ)dξˆ

62|A|1q q

2−q

q10(r−2r )

kfkLq,r.

The method of the proof in this paper is based on a study of the constants in inequalities of the form (2.2), namely their dependence on the relevant parameters.

Lemma 2.2. Let 2< p < 4, p0 = p−1p , 2< r <∞, f ∈Lp,r and A=

N

S

i=1

Ai, where Ai are segments in R. Then we have

1

|A|1pNp101p Z

A

f(ξ)dξˆ

6CkfkLp,r,

where

C = 4√ 2

r(p−2) p(r−2)

1p(2−rr )

. Proof. Let f ∈C0.

Z

A

fˆ(ξ)dξ

= Z

A

Z

−∞

f(t)e−iξtdtdξ

6

N

X

i=1

Z

Ai

Z

−∞

f(t)e−iξtdtdξ

6

N

X

i=1

Z

−∞

|f(t)|

Z

Ai

e−iξt

dt=

N

X

i=1

Z

−∞

|f(t)|

bi

Z

ai

e−iξt

dt=

N

X

i=1

Z

−∞

|f(t)|

2 sin(bi−a2 i)t t

dt

6

N

X

i=1

Z

−∞

|f(t)|min

(bi−ai),2 t

dt62

N

X

i=1

Z

−∞

|f(t)|min

|Ai|,1 t

dt. (2.3)

(5)

From the Plancherel’s theorem we get Z

A

fˆ(ξ)dξ

6|A|12kfkL2. (2.4)

Consider the function f1(x) =

f(x), |f(x)|6f(τ), x∈R\

τ2,τ2 0, otherwise,

f0(x) =f(x)−f1(x).

Then using the (2.3) and (2.4) we get

Z

A

f(ξ)dξˆ

6 Z

A

0(ξ)dξ

+ Z

A

1(ξ)dξ

6|A|12kf0kL2 + 2

N

X

i=1

Z

−∞

|f1(x)|min

|Ai|, 1

|x|

dx

=B(I1+I2) We have

I1 =

Z

−∞

|f0(x)|2dx

1 2

=

τ 2

Z

τ

2

|f(x)|2dx+ Z

τ 26|x|<∞

|f0(x)|2dx

1 2

62

τ

Z

0

|f(t)|2dt

1 2

I2 = 2

N

X

i=1

Z

−∞

|f1(x)|min

|Ai|, 1

|x|

= 2

N

X

i=1

Z

τ 26|x|<∞

|f1(x)|min

|Ai|, 1

|x|

62N

τ

Z

0

f1(t) 1 t+τdt=

= 2N

Z

0

f(t+τ) dt

t+τ 62N

Z

τ

f(t)dt t . Therefore,

Z

A

fˆ(ξ)dξ

62|A|12

τ

Z

0

(f(t))2dt

1 2

+ 2N

Z

τ

f(t)dt t .

(6)

Applying H´older’s inequality, we obtain

Z

A

f(ξ)dξˆ

62|A|12

τ

Z

0

(f(t)t1p)rdt t

1

r

τ

Z

0

t1−2pr−2r dt t

r−2 2r

+2N

Z

τ

f(t)tp1 r dt

t

1

r

Z

τ

tr

0 p dt

t

1 r0

6kfkLp,r 2|A|12

r(p−2) p(r−2)

2−r2r

τ121p + 2N pr−1r τ1p

! .

Now let τ = N2

|A|(p−2p )2−rr p2(1−rr ) and using that 2 < p < 4 we have the following estimate:

Z

A

f(ξ)dξˆ

64√

2|A|1/p

p−2 p

1p(2r−1)

Np101pkfkLp,r.

Lemma 2.3. Let A =

N

S

i=1

Ai, where Ai are segments. Then for any 2 < p < 4 and 2< r <∞ the inequality

1

|A|12 Z

A

f(ξ)dξˆ

6CkfkL2,r (2.5)

holds, where

C= 8 p

p−2

1p(1−2r) p+ 2

p 14

N121p. Proof. Let τ >0,

f1(x) =

f(x), |f(x)|6f(τ) 0, otherwise, f0(x) =f(x)−f1(x).

Then, using Lemmas 2.1, 2.2 and 2< r <∞, we obtain

Z

A

fˆ(ξ)dξ

6 Z

A

0(ξ)dξ

+ Z

A

1(ξ)dξ

62kf0kLp0,r

p0 2−p0

1p(r−2r )

|A|p10

+4√

2kf1kLp,r

p−2 p

1p(2−rr )

|A|1pNp10p1

(7)

62

τ

Z

0

tp10f(t)r dt t

1 r

|A|p10 p0

2−p0

1p(r−2r )

+4√ 2

Z

0

t1pf(t+τ)rdt t

1 r

|A|1p

p−2 p

p1(2−rr )

Np101p. Further, we estimate each integral separately

τ

Z

0

tp10f(t)rdt t

1 r

=

τ

Z

0

t1−1pf(t)r dt t

1 r

6

τ

Z

0

t12f(t)rdt t

1 r

sup

06t6τ

t121p 6τ(121p)kfkL2,r.

Z

0

tp1f(t+τ) r dt

t

1 r

6

τ

Z

0

t1p(t+τ)12rdt t

sup

0<s<∞

s12f(s) r

+

Z

τ

(t1pf(t+τ))rdt t

1 r

6

τ

Z

0

t1pτ12rdt t sup

0<s<∞

r 2

s

Z

0

ξr2−1f(ξ)rdξ+

Z

τ

t1pf(t)r dt t

1 r

6

τ(1p12)rp

2kfkrL2,r +τ(1p12)r

Z

τ

t12f(t)r dt t

1 r

6τ(1p12) p+ 2

2 1r

kfkL2,r.

Therefore given the 2< r <∞, we have

Z

A

fˆ(ξ)dξ

62|A|1−1p p

p−2

1p(1−2r)

τ(121p)kfkL2,r

+4√ 2|A|1p

p−2 p

1p(2−rr ) p+ 2

2 12

Np101pτ(1p12)kfkL2,r.

Taking τ(121p) = N

|A|

p101

p p+2

2

12 12

, we have

Z

A

f(ξ)dξˆ

68|A|12N121p p

p−2

1p(1−2r) p+ 2

2 14

kfkL2,r.

(8)

The proof of Theorem 2.1. Let A⊂ <N and |A|=N 68.

In the right part of the constant (2.5) we put p= 3. Then

8 p

p−2

1p(1−2r) p+ 2

2 14

N121p 620.

Therefore, from Lemma 2.3, we get 1

N12 log2(1 +N)121r Z

A

f(ξ)dξˆ

6 1 N12

Z

A

fˆ(ξ)dξ

620kfkL2,r.

Now let A⊂ <N so that N >8. Putp= log2 log2N

2N−2, i.e. p−22p = log1

2N, then p66.

Note also thatN121p =Nlog21N 62.

Using Lemma 2.3, we obtain 1

N12 Z

A

fˆ(ξ)dξ

623 log2(1 +N)

1 2 1

log2N

(1−2r)kfkL2,r

623 log2(1 +N)121rkfkL2,r. Taking the top exact bound over all N of N we obtain

sup

N>8

sup

A⊂<N

1

N12 log2(1 +N)121r Z

A

fˆ(ξ)dξ

623kfkL2,r

Theorem is proved.

Acknowledgments

This work was supported by the grant of the Ministry of Education and Science of the Republic of Kazakhstan (project 3311/GF4)

(9)

References

[1] J. Bergh, J. L´ofstr´om,Interpolation Spaces, New York. 1976, 210p.

[2] S.V. Bochkarev,Hausdorff-Young-Riesz theorem in Lorentz spaces and multiplicative inequalities, Proc. Steclov Inst. Math. 219 (1997), 96-107.

[3] A.N. Kopezhanova, E.D. Nursultanov, L.-E. Persson,On inequalities for the Fourier transform of functions from Lorentz spaces, Mathematical notes. 90 (2011), no. 5, 785-788.

[4] E.D. Nursultanov,Net spaces and the Fourier transform, (Russian) Dokl. Akad. Nauk 361 (1998), no 5, 597–599.

[5] E.D Nursultanov, T.U. Aubakirov, Hardy-Littlewood theorem for Fourier series, Mathematical notes. 73 (2003), 340-347.

[6] E.D. Nursultanov,Interpolation properties of some anisotropic spaces and Hardy–Littlewood type inequalities,East J. Approx. 4 (1998), no. 2, 277-290.

[7] E.D. Nursultanov,Application of interpolational methods to the study of properties of functions of several variables, Mathematical Notes. 75 (2004), no.3, 341-351.

[8] M. Stein Elias,Interpolation of linear operators, Trans. Amer. Math. Soc. 83 (1956), 482-492.

[9] E.C. Titchmarsh,A contribution to the theory of Fourier transforms, Proc. London Math. Soc.

23 (1924), no. 2, 279-289.

[10] E.C. Titchmarsh,Introduction to the theory of Fourier integrals, Clarendon Press, Oxford 1937;

Russian transl. Gostekhizdat, Moscow-Leningrad 1948.

[11] A. Zygmund,Trigonometrical series, 2nd ed. Vols. I, II, Cambridge Univ. Press, New York 1959;

Russian transl. Mir, Moscow 1965.

Guliya Mussabayeva

L.N. Gumilyov Eurasian National University 2 Satpayev st,

010010 Astana, Kazakhstan E-mail: [email protected] Nazerke Tleukhanova

L.N. Gumilyov Eurasian National University 2 Satpayev st,

010010 Astana, Kazakhstan E-mail: [email protected]

Received: 03.02.2015

Referensi

Dokumen terkait

In this article we deal with a Schwarz-type boundary value problem for both the inhomogeneous Cauchy-Riemann equation and the generalized Beltrami equation on an unbounded sector with

A review should cover the following topics: - compliance of the paper with the scope of the EMJ; - compliance of the title of the paper to its content; - compliance of the paper to

2 Main result In order to prove that in the category Rel of sets and relations, functions can be described in purely category terms, we will prove that several set-theoretic notions

Moreover, note that leading term of the asymptotics for the weighted differential entropy exceeds that for the classical differential entropy studied in [8].. The difference tends to

The nal part of the review should contain an overall opinion of a reviewer on the paper and a clear recommendation on whether the paper can be published in the Eurasian Mathematical

An iterative scheme containing two asymptotically nonexpansive mappings has been used in this paper to approximate common xed points in a strictly convex Banach space.. This improves

In this paper we obtain a special integral representation of functions with a set of multi-indices and use it to prove embedding theorems for multianisotropic spaces in

We prove an analogue of the Hahn-Banach theorem on the extension of a linear functional with a convex estimate for each abstract convex cone with the cancellation law.. Also we consider