Gen. Math. Notes, Vol. 14, No. 1, January 2013, pp.1-5 c ISSN 2219-7184; Copyright ICSRS Publication, 2013 www.i-csrs.org Available free online at http://www.geman.in On Estimates for the Fourier Transform in the Space Lp(R) M. El Hamma1 and R. Daher2 1,2 Faculty of Sciences Aı̈n Chock, University of Hassan II, Casablanca, Morocco 1 E-mail: m elhamma@yahoo.fr 2 E-mail: ra daher@yahoo.fr (Received: 1-8-12 / Accepted: 18-11-12) Abstract Using a Steklov’s function, we obtain two estimates are proved in certain classes of functions characterized by a generalized continuity modulus. Keywords: Fourier transform; Steklov function; generalized continuity modulus. 1 Introduction and Preliminaries It is well known that Fourier transforms are widely used in mathematical physics. Certain applications of this transform are described in a number of fundamental monographs (e.g., see [2, 3, 6, 7]). In this paper, we prove two estimates in certain classes of functions characterized by a generalized continuity modulus and connected with the Fourier transform in the space Lp (R), 1 < p ≤ 2, analogs of the statements proved in [1]. Assume that Lp (R), (1 < p ≤ 2), is the space of p-power integrable functions f : R −→ C with the norm kf kp = Z |f (x)|p dx 1/p . R It is well known that the Fourier transform of a function f ∈ L1 (R) is defined by 2 M. El Hamma et al. 1 Z fb(x) = √ f (t)e−ixt dt. 2π R The inverse Fourier transform is defined by 1 Z b f (t) = √ f (x)eixt dx. 2π R We have the Hausdroff-Young inequality kfbkq ≤ Ckf kp , (1) where p1 + 1q = 1 and C is a positive constant. In Lp (R), consider Steklov’s function 1 Z x+h f (t)dt, h > 0. 2h x−h We define the differences of first and higher orders as follows: Fh f (x) = ∆h f (x) = Fh f (x) − f (x) = (Fh − I)f (x), ∆kh f (x) = ∆h (∆hk−1 f (x)) = (Fh − I)k f (x) = k X (−1)k−i (ki )Fih f (x), i=0 where F0h f (x) = f (x), Fih f (x) = Fh (Fi−1 h f (x)), i = 1, 2, .., k; k = 1, 2, ... and p I is the unit operator in the space L (R). The quantity Ωk (f ; δ) = sup k∆kh f (x)kp 0<h≤δ is called the generalized continuity modulus of k th order of the function f ∈ Lp (R). r,k Denote by Wp,φ (R) the class of functions f ∈ Lp (R) having the generalized derivatives f 0 (x), f 00 (x), ..., f (r) (x) in the sence of Levi (see [4, 5]) in Lp (R) such that Ωk (f (r) , δ) = O(φ(δ k )), where φ(t) is a continuous steadily increasing function on [0, +∞) and φ(0) = 0. In [1], we have 3 On Estimates for the Fourier Transform... 1 Z sin(ht) b ixt √ Fh f (x) = f (t)e dt, 2π R ht then 1 Z sin(ht) Fh f (x) − f (x) = √ − 1)fb(t)eixt dt ( ht 2π R By Hausdroff-Young inequality (1), we obtain !1/q sin(ht) | − 1|q |fb(t)|q dt ht R Z ≤ CkFh f (x) − f (x)kp . r,k Hence, for any function f ∈ Wp,φ (R), we have !1/q sin(ht) qk b q t |1 − | |f (t)| dt ht R Z 2 qr ≤ Ck∆kh f (r) (x)kp . (2) Main Result In this section, we estimate the integral Z |fb(x)|q dx |x|≥N in certain classes of functions in Lp (R). Theorem 2.1 It holds that ! Z sup q |fb(t)| dt = O N |t|≥N r,k f ∈Wp,φ (R) 2 φ (( )k ) , N −qr q where r = 0, 1, ...; k = 1, 2, ....; and φ(t) is any nonnegative function defined on the interval [0, ∞). r,k Proof. Let f ∈ Wp,φ (R). By the Hölder inequality, we have Z |fb(t)|q dt − |t|≥N = Z |t|≥N (1 − |t|≥N ≤ Z Z |t|≥N Z sin(ht) b q sin(ht) b q |f (t)| dt = (1 − )|f (t)| dt ht ht |t|≥N sin(ht) b q− 1 b 1 )|f (t)| k |f (t)| k dt ht ! qk−1 qk q |fb(t)| dt ! sin(ht) qk b q |1 − | |f (t)| dt ht |t|≥N Z 1 qk 4 M. El Hamma et al. ! qk−1 qk Z = q |fb(t)| dt |t|≥N ≤ N Z ! −qr t |t|≥N ! qk−1 qk q b |f (t)| dt Z −r/k |t|≥N sin(ht) qk b q qr | |f (t)| t dt |1 − ht 1 qk ! sin(ht) qk b q | |f (t)| dt t |1 − ht |t|≥N Z 1 qk qr From formula (2), we conclude that Z tqr |1 − |t|≥N sin(ht) qr b q | |f (t)| dt ≤ C q k∆kh f (r) (x)kqp . ht Therefore Z |fb(t)|q dt ≤ |t|≥N ! qk−1 Z qk sin(ht) b q |f (t)| dt+C q N −r/k |fb(t)|q dt k∆kh f (r) (x)k1/k p . ht |t|≥N Z |t|≥N Note that Z |t|≥N sin(ht) b q Z sin(ht) b q 1 Z | |fb(t)|q dt |f (t)| dt ≤ ||f (t)| dt ≤ ht ht N h |t|≥N |t|≥N Then ! qk−1 Z Z qk 1 q q −r/k q |fb(t)| dt ≤ |fb(t)| dt+C N |fb(t)| dt k∆kh f (r) (x)k1/k p . N h |t|≥N |t|≥N |t|≥N Z q Setting h = 2 h we obtain ! qk−1 Z qk 1Z q q −r/k q b b |f (t)| dt ≤ C N |f (t)| dt k∆kh f (r) (x)k1/k p . 2 |t|≥N |t|≥N Since k∆kh f (r) (x)kp = O[φ( 2 k ) ]. N Consequently Z |t|≥N which completes the proof. |fb(t)|q dt = O[N −qr φq (( 2 k ) )] N On Estimates for the Fourier Transform... 5 r,k Corollary 2.2 Let φ(t) = tα , α > 0, and let f ∈ Wp,t α (R). Then Z |fb(t)|q dt = O(N −qr−qkα ) |t|≥N r,k Proof. Let f ∈ Wp,φ (R) and φ(t) = tα , α > 0. Then by Theorem 2.1 we have Z |fb(t)|q dt = O(N −qr N −qkα ) |t|≥N = O(N −qr−qkα ) which completes the proof. References [1] V.A. Abilov, F.V. Abilova and M.K. Kerimov, Some remarks concerning the Fourier transform in the space L2 (R), Zh. Vychisl. Mat. Mat. Fiz., 48(2008), 939-945,(Comput. Math. Math. Phys., 48, 885-891). [2] S. Bochner, Lectures on Fourier Integrals; With an Author’s Supplement on Monotonic Functions, Stieltjes Integrals and Harmonic Analysis, Princeton University Press, Princeton, (1959), Fizmatlit, Moscow, (1962). [3] M.M. Dzhrbashyan, Integral Transformation of Functions in Complex Domain, Nauka, Moscow, (1966), (In Russian). [4] B. Levi, Sul rincipio di dirichlet, Rend. Circolo Mat. di Palermo., 22(1906), 293-359. [5] S.M. Nikol’skii, Approximation of Functions of Several Variables and Embedding Theorems, Nauka, Moscow, (1969), (In Russian). [6] A.G. Sveshnikov, A.N. Bogolyubov and V.V. Kravtsov, Lecture in Mathematical Physics, Nauka, Moscow, (2004), (In Rssian). [7] E.C. Titchmarsh, Eigenfunction Expansions Associated with SecondOrder Differential Equations, Claredon, Oxford, (1962), Kom-Kniga, Moscow, (2005).