[ ) so that the function obtained (denoted, as before, by

Σχετικά έγγραφα
Fourier Transform. Fourier Transform

Oscillatory integrals

THE PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY, Series A, OF THE ROMANIAN ACADEMY Volume 15, Number 2/2014, pp

( ) ( t) ( 0) ( ) dw w. = = β. Then the solution of (1.1) is easily found to. wt = t+ t. We generalize this to the following nonlinear differential

Example Sheet 3 Solutions

Nonlinear Analysis: Modelling and Control, 2013, Vol. 18, No. 4,

Necessary and sufficient conditions for oscillation of first order nonlinear neutral differential equations

Uniform Convergence of Fourier Series Michael Taylor

Linear singular perturbations of hyperbolic-parabolic type

Math221: HW# 1 solutions

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

C.S. 430 Assignment 6, Sample Solutions

On Strong Product of Two Fuzzy Graphs

Matrices and Determinants

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD

Lecture 12 Modulation and Sampling

Statistical Inference I Locally most powerful tests

( ) ( ) ( ) Fourier series. ; m is an integer. r(t) is periodic (T>0), r(t+t) = r(t), t Fundamental period T 0 = smallest T. Fundamental frequency ω

r t te 2t i t Find the derivative of the vector function. 19. r t e t cos t i e t sin t j ln t k Evaluate the integral.

Solutions 3. February 2, Apply composite Simpson s rule with m = 1, 2, 4 panels to approximate the integrals:

ST5224: Advanced Statistical Theory II

Appendix. The solution begins with Eq. (2.15) from the text, which we repeat here for 1, (A.1)

2 Composition. Invertible Mappings

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

Managing Production-Inventory Systems with Scarce Resources

Oscillation Criteria for Nonlinear Damped Dynamic Equations on Time Scales

Homework 3 Solutions

University of Washington Department of Chemistry Chemistry 553 Spring Quarter 2010 Homework Assignment 3 Due 04/26/10

Second Order Partial Differential Equations

Anti-aliasing Prefilter (6B) Young Won Lim 6/8/12

Section 8.3 Trigonometric Equations

6.1. Dirac Equation. Hamiltonian. Dirac Eq.

Inverse trigonometric functions & General Solution of Trigonometric Equations

Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X.

Tridiagonal matrices. Gérard MEURANT. October, 2008

Trigonometry 1.TRIGONOMETRIC RATIOS

L F'(-c, 0) F(c, 0) M' D' x + d = 0 x - d = 0

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

Second Order RLC Filters

Σχολή Εφαρμοσμένων Μαθηματικών και Φυσικών Επιστημών. Εθνικό Μετσόβιο Πολυτεχνείο. Thales Workshop, 1-3 July 2015.

CHAPTER (2) Electric Charges, Electric Charge Densities and Electric Field Intensity

The choice of an optimal LCSCR contract involves the choice of an x L. such that the supplier chooses the LCS option when x xl

Reminders: linear functions

Oscillation criteria for two-dimensional system of non-linear ordinary differential equations

3 Frequency Domain Representation of Continuous Signals and Systems

Review-2 and Practice problems. sin 2 (x) cos 2 (x)(sin(x)dx) (1 cos 2 (x)) cos 2 (x)(sin(x)dx) let u = cos(x), du = sin(x)dx. = (1 u 2 )u 2 ( du)

2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)

Problem Set 3: Solutions

Positive solutions for a multi-point eigenvalue. problem involving the one dimensional

AMS 212B Perturbation Methods Lecture 14 Copyright by Hongyun Wang, UCSC. Example: Eigenvalue problem with a turning point inside the interval

DiracDelta. Notations. Primary definition. Specific values. General characteristics. Traditional name. Traditional notation

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

The one-dimensional periodic Schrödinger equation

EE512: Error Control Coding

F19MC2 Solutions 9 Complex Analysis

Approximation of distance between locations on earth given by latitude and longitude

Concrete Mathematics Exercises from 30 September 2016

ORDINAL ARITHMETIC JULIAN J. SCHLÖDER

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Coefficient Inequalities for a New Subclass of K-uniformly Convex Functions

Strain gauge and rosettes

SOLUTIONS TO PROBLEMS IN LIE ALGEBRAS IN PARTICLE PHYSICS BY HOWARD GEORGI STEPHEN HANCOCK

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is

Every set of first-order formulas is equivalent to an independent set

= e 6t. = t 1 = t. 5 t 8L 1[ 1 = 3L 1 [ 1. L 1 [ π. = 3 π. = L 1 3s = L. = 3L 1 s t. = 3 cos(5t) sin(5t).

Finite Field Problems: Solutions

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in

Bessel functions. ν + 1 ; 1 = 0 for k = 0, 1, 2,..., n 1. Γ( n + k + 1) = ( 1) n J n (z). Γ(n + k + 1) k!

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates

Fourier transform of continuous-time signals

Integrals in cylindrical, spherical coordinates (Sect. 15.7)

Lecture 5: Numerical Integration

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2

Solutions_3. 1 Exercise Exercise January 26, 2017

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.

Bounding Nonsplitting Enumeration Degrees

Other Test Constructions: Likelihood Ratio & Bayes Tests

Vidyamandir Classes. Solutions to Revision Test Series - 2/ ACEG / IITJEE (Mathematics) = 2 centre = r. a

Lecture 26: Circular domains

4.6 Autoregressive Moving Average Model ARMA(1,1)

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

INTEGRAL INEQUALITY REGARDING r-convex AND

Errata (Includes critical corrections only for the 1 st & 2 nd reprint)

J. of Math. (PRC) u(t k ) = I k (u(t k )), k = 1, 2,, (1.6) , [3, 4] (1.1), (1.2), (1.3), [6 8]

Fractional Colorings and Zykov Products of graphs

Riemann Hypothesis: a GGC representation

Almost all short intervals containing prime numbers

( )( ) La Salle College Form Six Mock Examination 2013 Mathematics Compulsory Part Paper 2 Solution

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =

CRASH COURSE IN PRECALCULUS

The Euler Equations! λ 1. λ 2. λ 3. ρ ρu. E = e + u 2 /2. E + p ρ. = de /dt. = dh / dt; h = h( T ); c p. / c v. ; γ = c p. p = ( γ 1)ρe. c v.

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3

A Note on Intuitionistic Fuzzy. Equivalence Relation

Arithmetical applications of lagrangian interpolation. Tanguy Rivoal. Institut Fourier CNRS and Université de Grenoble 1

Transcript:

Ukrinin Mhemicl Journl, Vol. 56, No. 9, 4 APPROXIMATION OF FUNTIONS DEFINED ON THE REAL AXIS BY OPERATORS GENERATED BY -METHODS OF SUMMATION OF THEIR FOURIER INTEGRALS Yu. I. Khrkeych nd T. V. Zhyhllo UD 57.5 We obin sympoic equliies for upper bounds of he deiions of operors genered by - mehods (defined by collecion Λ ( of funcions coninuous on ; { } [ nd depending on rel prmeer on clsses of (, β -differenible funcions defined on he rel xis.. Auxiliry Asserions nd Semen of he Problem For mny yers, Sepnes nd his followers he inesiged he pproximion properies of he clsses L β nd ˆLβ defined by he propery h he generlized ( β-deriies, of heir elemens belong o cerin se. For numerous resuls concerning hese problems, see [ 9]. According o [3] (hp. IX, he clsses ˆLβ re defined s follows: Le L p, p, be he se of π-periodic funcions ϕ( wih finie norm ϕ p, where ϕ p π / p p ϕ d ( for p [ ; nd ϕ ϕ M ess sup ϕ(, so h L M. The spces ˆLp, p, re inroduced s he ses of (no necessrily periodic funcions ϕ( defined on he enire rel xis R nd hing finie norm ϕ ˆp, where ϕ pˆ + π / p p sup ϕ( R d for p [, nd ϕ ˆ ess sup ϕ(. I is obious h, for ll p, he inclusion Lp L ˆ p is lwys rue. Le denoe he se of funcions ( conex downwrd for ll nd such h lim (. [ so h he funcion obined (denoed, s before, by We exend eery funcion o he segmen, ( is coninuous for ll, (, nd is deriie ( ( + hs smll riion on he segmen [,. Denoe he se of hese funcions by. The subse of funcions for which Volyn Uniersiy, Lus k. Trnsled from Ukrins kyi Memychnyi Zhurnl, Vol. 56, No. 9, pp. 67 8, Sepember, 4. Originl ricle submied Noember, 3. 4 5995/4/569 59 5 Springer Science+Business Medi, Inc. 59

5 YU. I. KHARKEVYH AND T. V. ZHYHALLO ( d < is denoed by F. We se ˆ ( ˆ ( ( cos π β + d, where F nd β is cerin fixed number. If F, hen, s shown in [4], for ny β R he rnsformion ˆ ( is summble on he enire xis: ˆ ( d <. Le ˆLβ denoe he se of funcions f( x Lˆ h, for lmos ll x R, cn be represened in he form f( x A ( x ˆ + ϕ + ( d, ( where A is cerin consn, ϕ( Lˆ, nd he inegrl is undersood s he limi of inegrls oer symmericlly expnding inerls. If f( Lˆ β nd, in ddiion,, where is cerin subse of coninuous funcions from ˆL, hen we ssume h f( Lˆ β. The subses of coninuous funcions from ˆLβ ˆLβ ( re denoed by Ĉ β ( Ĉ β. If coincides wih he se of funcions ϕ( sisfying he condiion ess sup ϕ (, hen he clss Ĉ β is denoed by ˆ β,. If f Lˆβ nd f β, hen we sy h f L ˆ ˆ β,. In [3] (hp. IX, i ws shown h if ϕ( is π-periodic summble funcion, hen he ses ˆLβ, ˆ L β,, nd ˆ β, rnsform ino he clsses L β, L β,, nd β,, respeciely. In he periodic cse where relion ( holds, we he ϕ( f β ( lmos eerywhere. In his connecion, ny funcion equilen o he funcion ϕ( in relion ( is clled, s in he periodic cse [see, e.g., [] (hp. I nd [4] (hp. III], he ( β-deriie, of f ( nd is denoed by f β (. As menioned boe, he clsses ˆLβ were inroduced by Sepnes. He lso considered he problem of he pproximion of funcions from he clsses ˆLβ by using he so-clled Fourier operors, which, in he periodic cse, re Fourier sums of order [ ] ; in he generl cse, hey re enire funcions of exponenil ype (see [4, 5]. In hese works, Sepnes obined represenion on he clsses ˆLβ for he deiions of he operors U( f, x,, which re inegrl nlogs of he polynomil operors genered by ringulr - mehods of summion of Fourier series. These resuls were pplied in [6 9] o he problem of pproximion of funcions from he clsses ˆLβ by he operors of Zygmund, Seklo, de l Vllée-Poussin, ec.

APPROXIMATION OF FUNTIONS DEFINED ON THE REAL AXIS BY OPERATORS GENERATED BY -METHODS 5 U The im of he presen pper is o sudy he deiions (on he clsses ˆ L β, nd ˆ β, of he operors ( f, x, genered by -mehods (defined by collecion Λ ( { } of funcions coninuous on [, nd depending on rel prmeer of summion of Fourier inegrls. In he periodic cse, for ( r, r >, he mos complee resuls in his direcion were obined in []; for funcions decresing o zero, he mos complee resuls were obined in []. Le Λ { } be collecion of funcions coninuous for ll nd depending on rel prmeer. We ssocie eery funcion f L wih he expression ˆβ U ( Λ U( f, x, Λ A + f x + + β d d π ( ( cos. ( Furher, we ssume h he funcions ( nd re such h he rnsformions $ π ( cos + d re summble on he enire number xis. Then, using relions ( nd (, for eery funcion f( ˆ β we obin f( x U ( f, x, Λ + f x r + β ( cos dd, (3 π where, for, r (, (4 nd, on he segmen, he funcion r is rbirrily defined so h i is coninuous for ll, equl o zero he origin, nd such h is Fourier rnsform is summble on he enire number xis. In he presen pper, we inesige he quniies rˆ ( r cos + d π ( β, f ˆ β, ˆ, U ( Λ sup f( x U ( f, x, Λ, (5

5 YU. I. KHARKEVYH AND T. V. ZHYHALLO ( β, ˆ ˆ f Lˆ β, L ˆ, U ( Λ sup f( x U ( f, x, Λ where U( f, x, Λ re he operors defined by (. Firs, we presen seerl uxiliry definiions nd semens necessry for wh follows., (6 Definiion []. Le funcion τ( be defined on [,, bsoluely coninuous, nd such h τ(. We sy h τ( if he deriie τ ( cn be defined he poins where i does no exis so h, for cerin, he following inegrls exis: / dτ (, dτ (. / Le K nd K i denoe consns h re, generlly speking, differen in differen relions. Lemm []. If τ(, hen τ( τ( + τ( + / dτ ( + dτ ( : H( τ. (7 / Theorem []. Suppose h τ( nd sin τ(. In order h he inegrl A( τ τ( cos + d d π (8 be conergen, i is necessry nd sufficien h he inegrls τ( sin d, τ( τ( + d be conergen. In his cse, he following esime is rue: 4 d A( τ ξsin τ (, j [ τ ( τ ( + ] KH( τ π, (9 where ξ( AB, is he funcion defined s follows []: ξ( AB, π A, B A, A A rcsin + B A, B > A, B (

APPROXIMATION OF FUNTIONS DEFINED ON THE REAL AXIS BY OPERATORS GENERATED BY -METHODS 53 j, < <,,. ( Le. Following [, pp. 59, 6], we se ( η( :, µ ( : η(, { : < µ (, K }, { } c : < K < µ (, K. If nd, moreoer, or for, hen, following [4, p. ], we wrie or, respeciely. Theorem [, p. 6]. A funcion belongs o if nd only if he quniy α( (, ( : ( +, ( sisfies he condiion α( K >. Theorem 3 [, p. 75]. In order h funcion belong o, i is necessry nd sufficien h here exis consn K such h, for ll, he following inequliy is rue: ( ( c K, where c is n rbirry consn h sisfies he condiion c >. ( β,. Asympoic Relions for ˆ, U ( Λ For conenience, performing chnge of ribles, we rewrie relions (3 nd (4 in he form f( x U ( f, x, Λ π τ ( β + f x ( cos + dd, ( ( τ( τ( ( (, (, (3

54 YU. I. KHARKEVYH AND T. V. ZHYHALLO where, s before, he funcion τ ( is rbirrily defined on he segmen,, equl o zero he origin, nd such h is Fourier rnsform so h i is coninuous for ll is summble on he enire number xis. Then he following heorem is rue: Theorem. Suppose h he following condiions re sisfied: (i ( F ; (ii τ( ; τˆ( ( cos π τ + d (4 (iii sin τ ( ; (i he following inegrls conerge: τ sin ( d, ( ( + d. (5 Then he funcion τ( τ ( ( ( (, (, ( ( ( (,, (6 sisfies he following relion: ( β, ˆ, U ( Λ 4 π ξ ( sin τ (, j [ τ ( τ ( + ] d + O( ( H(,, (7 τ where H( τ, ξ( AB,, nd j re defined by (7, (, nd (, respeciely. Proof. Using Theorem, we show h he inegrl A( τ conerges, nd, hence, by irue of Lemm in [8], he following relion holds s : ( β, ˆ, U( Λ ( A ( τ. (8

APPROXIMATION OF FUNTIONS DEFINED ON THE REAL AXIS BY OPERATORS GENERATED BY -METHODS 55 One of he condiions of Theorem is he conergence of he inegrl τ( τ( + d, (9 wheres one of he condiions of Theorem is he conergence of he inegrl ( ( + d. ( Le us show h if, hen τ( τ( + d ( ( ( + ( d+ H( τ O(, ( where O( is quniy uniformly bounded in. Therefore, he conergence of inegrl ( yields he conergence of inegrl (9. Using relion (6, we ge τ τ ( ( + ( ( (, (, ( ( ( (,, ( ( ( (, ( +, ( ( + ( ( +,. ( ( (3 Firs, we consider he cse > nd represen relion (9 s sum of wo inegrls: τ( τ( + d τ( τ( + d + τ( τ( + d. (4 Le us esime he firs erm on he righ-hnd side of (4. To his end, we dd nd subrc he quniy ( ( ( + ( ( under he modulus sign in he inegrnd. As resul, we obin

56 YU. I. KHARKEVYH AND T. V. ZHYHALLO τ( τ( + d ( ( ( + ( d + O ( τ ( ( + + ( ( ( + τ ( d. (5 Since relions ( nd (3 re rue, for, we ge ( ( τ( ( ( nd ( ( + τ( +. ( ( + Then ( τ( τ( + + ( ( + ( ( d ( τ ( ( ( d + ( τ ( + ( ( + d. (6 Since τ (, ccording o Lemm we ge ( τ ( ( ( d + ( τ ( + ( ( + d H( τ O ( ( ( ( ( d + ( ( + ( ( ( + d. (7

APPROXIMATION OF FUNTIONS DEFINED ON THE REAL AXIS BY OPERATORS GENERATED BY -METHODS 57 Le us show h, s, I, : I, : ( ( ( ( ( ( ( + ( ( ( + d O(, (8 d O(, (9 where he quniy O( is uniformly bounded in. Indeed, he funcion ( / ( ( for ll δ,, < δ <, nd, furhermore, by irue of Theorem, we he is bounded ( / ( ( ( lim ( K. Therefore, I, O( s. Pssing o he esimion of he inegrl I,, we noe h I, < ( ( ( ( + d. Performing he chnge of ribles u ( +, we ge I, < ( ( ( u du < u ( ( ( u du. u Using Lemm.5 from [3] nd Theorem 3 for he righ-hnd side of he ls inequliy, we obin I, < K( K( K3. ( ( Thus, equliies (8 nd (9 re rue. ombining relions (5 (9, we ge τ( τ( + d ( ( ( + ( d+ H( τ O(. (3 Le us esime he second erm on he righ-hnd side of (4. I is obious h

58 YU. I. KHARKEVYH AND T. V. ZHYHALLO τ( τ( + d ( ( ( + ( d + O ( τ( τ( + + ( ( ( + ( d. (3 Using relions ( nd (3, for, we ge ( ( τ( ( (3 nd Hence, by irue of Lemm, we obin ( ( + τ( +. ( ( + ( τ( τ( + + ( ( + ( ( d ( τ ( τ ( + ( ( ( + ( d H( τ O ( ( ( ( + ( d + ( ( ( + d. (33 We esime he righ-hnd side of (33 s follows: ( ( ( d - ln O(. (34 ( (

APPROXIMATION OF FUNTIONS DEFINED ON THE REAL AXIS BY OPERATORS GENERATED BY -METHODS 59 By nlogy wih he proof of relion (9, we ge ( ( + ( ( ( + d ( ( u ( u du ( ( u ( u du ( ( O(. (35 Using relions (3 (35, we obin τ( τ( + d ( ( ( + ( d + H( τ O(. (36 ombining relions (36 nd (3, we rrie equliy (. By nlogy wih he proof of relion (, for > <. For <, relion (3 is rue nd Then ( ( + τ ( +. ( one cn show h equliy ( is lso lid for τ( τ( + d ( ( ( ( + d. The conergence of inegrl ( yields he conergence of inegrl (9. Thus, for, ll condiions of Theorem re sisfied. Then, subsiuing relion (9 ino equliy (8, we ge (7. Theorem is proed. Noe h n nlogous heorem ws proed in [] in he periodic cse where ( [] for he clsses β,,. orollry. Suppose h he condiions of Theorem re sisfied. If r, r >, nd in τ ( τ ( + sin τ (, [, ], >, (37 hen

5 YU. I. KHARKEVYH AND T. V. ZHYHALLO ˆ ( β,, U( Λ π τ ( ( sin d + O ( sin π τ( d ( ( + + O( ( d + O( ( H( τ,. (38 If sin τ ( < τ ( τ ( +, [, ], >. (39 hen ˆ ( β,, U( Λ 4 π ( ( + ( d + O( π j ( ( + d + O τ ( sin ( d O( ( H( τ,. (4 Proof. Relion (38 follows direcly from equliy (7 nd he definiion of he funcion ξ( AB., To proe relion (4, noe h, by irue of (39 nd (4, he following equliies re rue: ξ sin τ [ τ τ + ] (, j ( ( d sin τ ( sin ( rcsin τ τ ( τ ( + + ( τ( τ( + sin τ ( d sin τ ( sin τ ( τ( τ( + ( d + O sin τ ( d,. (4

APPROXIMATION OF FUNTIONS DEFINED ON THE REAL AXIS BY OPERATORS GENERATED BY -METHODS 5 Since relion (39 is rue, we conclude h sin τ ( ( τ ( τ ( + [, ] if [, ]. Using relion (4 nd he expnsion of he funcion, [, ], in power series, we obin ξ sin τ [ τ τ + ] (, j ( ( d d τ ( sin τ ( + Osin d,. (4 Subsiuing (4 ino (7 nd using relion (, we ge (4. orollry is proed. orollry. Le Λ{ nk, }, where n, k,, nd n, for ll n, be recngulr numericl mrix h ssocies eery funcion f ˆβ wih series (. Suppose h he mrix Λ is such h series ( is he Fourier series of cerin coninuous funcion denoed by Un( f, x, Λ. Also ssume h k he mrix Λ is deermined by sequence of funcions n ( u, u <, such h nk, n n nd n, for ll n. The sympoic equliies for he quniies ( ˆ β,, U n ( Λ sup f( x U (,, n f x Λ ˆ f β, cn be obined by seing n, n N, in relions (7, (38, nd (4, proided h ll condiions of Theorem re sisfied. We ge ( ˆ β,, U n ( Λ 4 π ξ ( n d sin τ n (, j u τ n ( τ n ( [ + ] + O ( ( H ( τn,, where he funcions τ n (, n,,, re defined by he equliies τ n ( ( ( ( (, n n, ( n ( ( (, n n. If

5 YU. I. KHARKEVYH AND T. V. ZHYHALLO hen τ ( τ ( + sin τ ( n n n, [, ], >, ( ˆ β,, U n ( Λ π τ ( ( n sin n nπ τ d + O ( n sin n( d + O n n( ( n( + ( d + O( ( n H( τ n,. If sin τ n( < τ n( τ n( +, [, ], >, hen ( ˆ β,, U n ( Λ 4 π ( ( ( n n n + d + O( n nπ j n( n( + d ( β, Λ ˆ 3. Asympoic Relions for L ˆ, U ( τ + O ( n sin n( d + O( ( n H( τ n, n. In his secion, we sudy he behior of upper bounds of (6. Firs, we gie seerl definiions nd uxiliry resuls. Assume h f L ˆβ, F, nd he funcion τ ( is defined by (3 nd such h is Fourier rnsform τˆ ( ˆ ( (4 is summble on R. Then, lmos eery poin x R, we he τ f( x U ( f, x, ( f x + ( cos + β d d π τ Λ. (43 Noe h he funcion τ ( cn be chosen so h i is coninuous for nd is Fourier rnsform τˆ ( is summble on R. Using relion (43, we esblish he following semen:

APPROXIMATION OF FUNTIONS DEFINED ON THE REAL AXIS BY OPERATORS GENERATED BY -METHODS 53 Lemm. Suppose h F, he funcion τ ( is defined by (3 nd coninuous for ll, nd inegrl (8 conerges. Then he following relion holds s : ( + β, ˆ ˆ f Lˆ β, L ˆ ; U ( Λ sup f( x U ( f, x, Λ ( A( τγ ( (, (44 where γ ( nd Proof. Tking ino ccoun h γ ( O τ( cos + d d. (45 π f x + d τˆ ( ˆ π sup f x + + ˆ ( ddx τ f ˆ ˆ τ ( d R π nd using equliies (6 nd (43, we ge ( sup f( x U( f, x, β, ˆ L ˆ, U ( Λ ˆ f Lβ, On he oher hnd, by irue of Proposiion. in [3, p. 69], we he Λ ˆ ( τˆ ( d ( A ( τ. (46 Lˆ L β (, π Lβ β Lβ he se of π-periodic funcions wih men lue zero on ( π,. Therefore, Lˆ,,. Hence,, where L (, π is sup f x ˆ + ( d τ f Lˆ β, ˆ sup f x ˆ + ( d τ f L β,. (47 Moreoer, i is shown in [, p. 4] h sup ( f ˆ x + ( d ( A( + ( ( τ τγ, (48 f L β, where γ ( nd relion (45 is rue. Using (46 (48, we obin relion (44. The lemm is proed. In he periodic cse, n nlogous lemm ws proed in [] for he clsses L β,.

54 YU. I. KHARKEVYH AND T. V. ZHYHALLO ( nd β, ˆ ompring he lemm proed wih Lemm in [8], we conclude h he quniies L ˆ, U ( Λ ( ˆ β,, U( Λ my differ only by quniy h does no exceed γ ( in order, i.e., he following relion holds s : ( ( + ( Lˆ, U ( Λ ˆ, U ( Λ O ( γ β, ˆ β,. Using he ls equliy, we cn proe n nlog of Theorem for funcions of he clsses ˆ L β,. Theorem. Suppose h he following condiions re sisfied: (i ( F ; (ii τ ( ; τ (iii sin ( ; (i inegrls (5 conerge. Then, for he funcion τ( ( defined by (6, he following sympoic equliy is rue: τ ( β, ˆ L ˆ, U ( Λ 4 π ξ ( sin τ (, j [ τ ( τ ( + ] d π + O ( sin τ ( + j [ τ ( τ ( + ] d + O( ( H(,, where H( τ, ξ( AB,, nd j re defined by (7, (, nd (, respeciely. If, in ddiion, inequliy (37 is rue, hen τ ( L ˆ, β, U ( Λ ˆ ( sin π τ ( d + O ( sin π τ( d + O ( If inequliy (39 is rue, hen ( ( + d + O( ( H( τ,.

APPROXIMATION OF FUNTIONS DEFINED ON THE REAL AXIS BY OPERATORS GENERATED BY -METHODS 55 ( L ˆ, ( β, U Λ ˆ 4 π ( ( + ( d + O( π j ( ( + d + O τ ( sin ( d + O( ( H( τ,. REFERENES F. A. I. Sepnes, lssificion nd Approximion of Periodic Funcions [in Russin], Nuko Dumk, Kie (987.. A. I. Sepnes, Mehods of Approximion Theory [in Russin], Vol., Insiue of Mhemics, Ukrinin Acdemy of Sciences, Kie (. 3. A. I. Sepnes, Mehods of Approximion Theory [in Russin], Vol., Insiue of Mhemics, Ukrinin Acdemy of Sciences, Kie (. 4. A. I. Sepnes, lsses of funcions defined on he rel xis nd heir pproximion by enire funcions. I, Ukr. M. Zh., 4, No., (99. 5. A. I. Sepnes, lsses of funcions defined on he rel xis nd heir pproximion by enire funcions. II, Ukr. M. Zh., 4, No., (99. 6. M. G. Dzimisrishili, Approximion of lsses of oninuous Funcions by Zygmund Operors [in Russin], Preprin No. 89.5, Insiue of Mhemics, Ukrinin Acdemy of Sciences, Kie (989, pp. 3 4. 7. M. G. Dzimisrishili, On he Behior of Upper Bounds of Deiions of Seklo Operors [in Russin], Preprin No. 9.5, Insiue of Mhemics, Ukrinin Acdemy of Sciences, Kie (99, pp. 3 9. 8. V. I. Rukso, Approximion of funcions defined on he rel xis by de l Vllée-Poussin operors, Ukr. M. Zh., 44, No. 5, 68 69 (99. 9. L. A. Repe, Approximion of funcions of he clsses ˆ ϕ, β, by operors of he form U, in: Fourier Series: Theory nd Applicions [in Russin], Insiue of Mhemics, Ukrinin Acdemy of Sciences, Kie (99, pp. 47 54.. L. I. Buso, Liner mehods of summion of Fourier series wih gien recngulr mrices. I, Iz. Vyssh. Uchebn. Zed., 46, No. 3, 5 3 (965.. A. K. Noiko, On pproximion of funcions in he spces nd L, in: Problems of Summion of Fourier Series [in Russin], Preprin No. 85.6, Insiue of Mhemics, Ukrinin Acdemy of Sciences, Kie (985, pp. 4 5.. S. A. Telykoskii, On he norms of rigonomeric polynomils nd pproximion of differenible funcions by liner mens of heir Fourier series. II, Iz. Akd. Nuk SSSR, Ser. M., 7, No., 53 7 (963. 3. A. I. Sepnes, Approximion of funcions wih slowly rying Fourier coefficiens by Fourier sums, in: Approximion of Periodic Funcions by Fourier Sums [in Russin], Preprin No. 84.43, Insiue of Mhemics, Ukrinin Acdemy of Sciences, Kie (984, pp. 3 5.