CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION

Similar documents
Convergence of Singular Integral Operators in Weighted Lebesgue Spaces

On The Hermite- Hadamard-Fejér Type Integral Inequality for Convex Function

FURTHER GENERALIZATIONS. QI Feng. The value of the integral of f(x) over [a; b] can be estimated in a variety ofways. b a. 2(M m)

Application on Inner Product Space with. Fixed Point Theorem in Probabilistic

Contraction Mapping Principle Approach to Differential Equations

PART V. Wavelets & Multiresolution Analysis

Hermite-Hadamard-Fejér type inequalities for convex functions via fractional integrals

ON THE OSTROWSKI-GRÜSS TYPE INEQUALITY FOR TWICE DIFFERENTIABLE FUNCTIONS

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE BOUNDARY-VALUE PROBLEM

Research Article New General Integral Inequalities for Lipschitzian Functions via Hadamard Fractional Integrals

Hermite-Hadamard and Simpson Type Inequalities for Differentiable Quasi-Geometrically Convex Functions

On the Fourier Transform for Heat Equation

INTEGRALS. Exercise 1. Let f : [a, b] R be bounded, and let P and Q be partitions of [a, b]. Prove that if P Q then U(P ) U(Q) and L(P ) L(Q).

ON THE STABILITY OF DELAY POPULATION DYNAMICS RELATED WITH ALLEE EFFECTS. O. A. Gumus and H. Kose

GENERALIZATION OF SOME INEQUALITIES VIA RIEMANN-LIOUVILLE FRACTIONAL CALCULUS

1. Introduction. 1 b b

ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX

Research Article Generalized Fractional Integral Inequalities for Continuous Random Variables

Solutions to Problems from Chapter 2

SOME PROPERTIES OF GENERALIZED STRONGLY HARMONIC CONVEX FUNCTIONS MUHAMMAD ASLAM NOOR, KHALIDA INAYAT NOOR, SABAH IFTIKHAR AND FARHAT SAFDAR

Green s Functions and Comparison Theorems for Differential Equations on Measure Chains

New Inequalities in Fractional Integrals

An Extension of Hermite Polynomials

Some Inequalities variations on a common theme Lecture I, UL 2007

Yan Sun * 1 Introduction

A LIMIT-POINT CRITERION FOR A SECOND-ORDER LINEAR DIFFERENTIAL OPERATOR IAN KNOWLES

Positive and negative solutions of a boundary value problem for a

On Volterra Integral Equations of the First Kind with a Bulge Function by Using Laplace Transform

Temperature Rise of the Earth

A Time Truncated Improved Group Sampling Plans for Rayleigh and Log - Logistic Distributions

Lecture #6: Continuous-Time Signals

Analytic solution of linear fractional differential equation with Jumarie derivative in term of Mittag-Leffler function

On the Integro-Differential Equation with a Bulge Function by Using Laplace Transform

Research Article Existence and Uniqueness of Periodic Solution for Nonlinear Second-Order Ordinary Differential Equations

REAL ANALYSIS I HOMEWORK 3. Chapter 1

Spectral Galerkin Method for Optimal Control Problems Governed by Integral and Integro- Differential Equations

3. Renewal Limit Theorems

5.1-The Initial-Value Problems For Ordinary Differential Equations

On a Class of Two Dimensional Twisted q-tangent Numbers and Polynomials

NEW FRACTIONAL DERIVATIVES WITH NON-LOCAL AND NON-SINGULAR KERNEL Theory and Application to Heat Transfer Model

Development of a New Scheme for the Solution of Initial Value Problems in Ordinary Differential Equations

C 0 Approximation on the Spatially Homogeneous Boltzmann Equation for Maxwellian Molecules*

Existence Of Solutions For Nonlinear Fractional Differential Equation With Integral Boundary Conditions

SUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL

On the Pseudo-Spectral Method of Solving Linear Ordinary Differential Equations

Fractional Laplace Transform and Fractional Calculus

Journal of Mathematical Analysis and Applications. Two normality criteria and the converse of the Bloch principle

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR

On Hadamard and Fejér-Hadamard inequalities for Caputo k-fractional derivatives

On the Stability of the n-dimensional Quadratic and Additive Functional Equation in Random Normed Spaces via Fixed Point Method

An Integral Two Space-Variables Condition for Parabolic Equations

Procedia Computer Science

An Iterative Method for Solving Two Special Cases of Nonlinear PDEs

Fractional Calculus. Connor Wiegand. 6 th June 2017

ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX.

HUI-HSIUNG KUO, ANUWAT SAE-TANG, AND BENEDYKT SZOZDA

Non-oscillation of perturbed half-linear differential equations with sums of periodic coefficients

A Simple Method to Solve Quartic Equations. Key words: Polynomials, Quartics, Equations of the Fourth Degree INTRODUCTION

On some Properties of Conjugate Fourier-Stieltjes Series

Mathematics 805 Final Examination Answers

Correspondence should be addressed to Nguyen Buong,

LAPLACE TRANSFORMS. 1. Basic transforms

A new model for solving fuzzy linear fractional programming problem with ranking function

arxiv:math/ v1 [math.nt] 3 Nov 2005

2k 1. . And when n is odd number, ) The conclusion is when n is even number, an. ( 1) ( 2 1) ( k 0,1,2 L )

On Likelihood Ratio and Stochastic Order. for Skew-symmetric Distributions. with a Common Kernel

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE

Necessary and Sufficient Conditions for Asynchronous Exponential Growth in Age Structured Cell Populations with Quiescence

Fractional operators with exponential kernels and a Lyapunov type inequality

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

Sumudu Decomposition Method for Solving Fractional Delay Differential Equations

e t dt e t dt = lim e t dt T (1 e T ) = 1

Generalization of Some Inequalities for the Ratio of Gamma Functions

THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX

Research Article The General Solution of Differential Equations with Caputo-Hadamard Fractional Derivatives and Noninstantaneous Impulses

Think of the Relationship Between Time and Space Again

How to prove the Riemann Hypothesis

Integral Transform. Definitions. Function Space. Linear Mapping. Integral Transform

Intuitionistic Fuzzy 2-norm

Citation Abstract and Applied Analysis, 2013, v. 2013, article no

Asymptotic instability of nonlinear differential equations

On Two Integrability Methods of Improper Integrals

SOLUTION FOR A SYSTEM OF FRACTIONAL HEAT EQUATIONS OF NANOFLUID ALONG A WEDGE

in Engineering Prof. Dr. Michael Havbro Faber ETH Zurich, Switzerland Swiss Federal Institute of Technology

LAPLACE TRANSFORM OVERCOMING PRINCIPLE DRAWBACKS IN APPLICATION OF THE VARIATIONAL ITERATION METHOD TO FRACTIONAL HEAT EQUATIONS

..,..,.,

Robust Finite-Time H Filtering for Itô Stochastic Systems

Asymptotic relationship between trajectories of nominal and uncertain nonlinear systems on time scales

On a Volterra equation of the second kind with incompressible kernel

Weyl sequences: Asymptotic distributions of the partition lengths

Scientific Research of the Institute of Mathematics and Computer Science DIFFERENT VARIANTS OF THE BOUNDARY ELEMENT METHOD FOR PARABOLIC EQUATIONS

Faα-Irresolute Mappings

A Note on Fractional Electrodynamics. Abstract

September 20 Homework Solutions

A NOTE ON S(t) AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION

Bifurcation Analysis of a Stage-Structured Prey-Predator System with Discrete and Continuous Delays

Lecture 10: The Poincaré Inequality in Euclidean space

Transcription:

Avilble online hp://scik.org Eng. Mh. Le. 15, 15:4 ISSN: 49-9337 CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION PANDEY, C. P. 1, RAKESH MOHAN AND BHAIRAW NATH TRIPATHI 3 1 Deprmen o Mhemics, Ajy Kumr Grg Engineering College, Ghzibd 19, Indi Deprmen o Mhemics, Dehrdun Insiue o Technology, Dehrdun 489, Indi 3 Deprmen o Mhemics, Urkhnd Technicl Universiy, Dehrdun 487, Indi Copyrigh 15 Pndey, Mohn nd Triphi. This is n open ccess ricle disribued under he Creive Commons Aribuion License, which permis unresriced use, disribuion, nd reproducion in ny medium, provided he originl work is properly cied. Absrc. Clderon-ype reproducing ormul or Dunkl convoluion is esblished using he heory o Dunkl rnsorm. Keywords: wvele rnsorm; Dunkl convoluion; Dunkl rnsorm. 1 Mhemics Subjec Clssiicion: 4C4, 44A35, 65T6, 65R1. 1. Inroducion Clderon ormul [8] involving convoluion reled o he Fourier rnsorm is useul in obining reconsrucion ormul or wvele rnsorm besides mny oher pplicions in decomposiion o cerin uncion spces. I is expressed s ollows: * Corresponding uhor d ( ) ( )( ), (1.1) x x n n where : C nd ( x) ( x / ),. For condiions o vlidiy o ideniy (1.1), we my reer o [8]. On he rel line, he Dunkl operor re dierenil-dierence operor inroduced by Dunkl [1] nd re denoed by, where is rel prmeer 1/.These operor ssocied wih he relecion group on. The Dunkl kernel E is used o deine he Dunkl rnsorm which ws inroduced by Dunkl in []. Rosler in [3] show h he Dunkl kernels veriy produc ormul. This llows o deine he Dunkl rnslion. As resul, we hve he Dunkl convoluion. Received December 11, 14 1

PANDEY, MOHAN AND TRIPATHI Dunkl Operor hs unique soluion E x, clled Dunkl kernel nd given by x E x j i x j i x 1 1, x R, (1.) where j is he normlized Bessel uncion o he irs kind nd order. Le 1/ be ixed number nd be he weighed Lebesgue mesure on R, given by 1 1 1 : 1 d x x dx. (1.3) We deine L p, (, ), 1 p, which s he spces o hose rel mesurble uncion on(, ) or 1 p p x d x i p 1, p, (1.4) R nd ess sup ( x) i p =. xr The Dunkl kernel gives rise o n inegrl rnsorm, clled Dunkl rnsorm on R, which ws inroduced nd sudied in [7]. The Dunkl rnsorm F o uncion L1, ( R), is given by F E ix x d x ; R (1.5) An inversion ormul or his rnsorm is given by R F 1 x E ix d (1.6) An Prsevl ormul or his rnsorm is given by R x g x dx g (1.7) To deine Dunkl convoluion, we deine where W x, y, z E ( x) E ( y) E ( z) d ( ) (1.8) x, y, z x y z xy 1 x, y, z z, x, y z, y, x x, y, z, i x, y R \ oherwise

CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION 3 nd is he Bessel kernel. Clerly W x, y, z is symmeric in x, y, z. Apply inversion ormul (1.6) o (1.8), we ge E ( z) W x, y, z d ( z) E ( x) E ( y). (1.9) Now seing, we obin W x, y, z d ( z) 1. (1.1) 1 1 1 Le p, q, r [1, ) nd 1. Then Dunkl convoluion o Lp, ( R) nd g Lq, ( R) r p q is deined by [7] ( g)( x) z g y W ( x, y, z) d y d z (1.11) RR 1 1 1 p nd 1 r p q Le, q, r 1, * g x sisies he ollowing norm inequliy, L R nd g L R p, q,. Then convoluion * g 4 g (1.1) (i) r, p, q, Moreover or ll L R nd g L R 1, (ii) * g g,, we hve (1.13). Clderon s ormul In his secion, we obin Clderon s reproducing ideniy using he properies o Dunkl rnsorm nd Dunkl convoluions. Theorem.1 Le nd 1, [, ) be such h ollowing dmissibiliy condiion holds: L d ( ) ( ) 1 (.1) or ll [, ). Then he ollowing Clderon s reproducing ideniy holds: 1 d ( x) * * ( x), L ( R). (.) Proo: Tking Dunkl rnsorm o he righ hnd side o (.), we ge

4 PANDEY, MOHAN AND TRIPATHI d F * * ( x) = Now, by puing Hence he resul ollows. 垐 d ( ) ( ) ( ) = 垐 d ( ) ( ) ( ) (.3) = 垐 ( ) ( ) ( ) d = ( ) ( ) ( ) d ( ) ( ) d (.4) 1. Theorem. Suppose 1, [, ) is rel vlued nd sisies For 1,, L d ( ) 1. (.5) L [, ) L [, ), suppose h Then, s &., d, ( x) * * ( x) (.6) Proo: Tking Dunkl rnsorm o boh sides o (.6) nd using Fubini s heorem, we ge By [4], we hve, ( ) ( ) ( ) * * * d, 1,,. 1,, (.7) (.8) Now using bove inequliy nd Minkowski s inequliy [6, pge 41], we ge

CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION 5 d d x * * ( ), x Hence by Prsevl ormul, we ge Since lim * * ( x) d x d d * * ( x) (.9), 1,, d log 1,,. lim,,,, lim ( ) 1 d ( ) d x. (.1) ( ) 1 d ( ) ( ), hereore by he domined convergence heorem, he resul ollows. The reproducing ideniy (.) holds in he poin wise sense under dieren se o nice condiions. Theorem.3 Suppose, L1, [, ). Le L1, [, ) be rel vlued nd sisies Then Proo: Le d ( ) 1, R. (.11) By [4, pge 311], we hve d lim * * ( x) ( x). (.1) d, ( x) * * ( x). (.13)

6 PANDEY, MOHAN AND TRIPATHI * * * 1, 1, 1, 1, 1, (.14) Now Thereore, 1, L(, ) d, d x * * ( ) 1, x * * ( x) d x d d * * ( x) (.15) 1, 1, 1, d log 1, 1,.. Also using Fubini s, we ge heorem nd king Dunkl rnsorm o (.13), we ge ( ) ( ) ( * * )( ) d, E x x d d E ( x )( * * )( x) d x (.16) ( ) ( ) d ( ) ( ) [ ( )] Thereore, by (.11),, ( ) ( ). d I ollows h, 1, [, ).By inversion, we hve L. Puing ( x) ( x) E ( x )[ ( ) ( )] d, x [, ) (.17),, h, ( : x) E ( x ) ( ), ( )

CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION 7 we ge Now using (.11) in (.18), we ge ( ) E ( ) 1 x [ ( )] d (.18) ( x), ( x) ( ) ( ), ( ) E x d (.19),, h ( : x) d. lim h ( : x), R. (.) Since h, ( : x) ( ), he Lebsegue domined convergence heorem yields lim ( x), ( x), x. (.1) Conlic o Ineress The uhors declre h here is no conlic o ineress. REFERENCES [1] C.F.Dunkl, Dierenil-dierence operors ssocied wih relecions groups, Trns. Amer. Mh. Soc. 311(1989), 167-183. [] C.F.Dunkl, Hnkel rnsorms ssocied o inie relecion groups, Amer. Mh. Soc. 138 (199), 13-138. [3] M.Rosler, Bessel-ype signed hypergroups on, in Probbily mesures on groups nd reled srucure, XI (Oberwolch, 1994), H.Heyer nd A.Mukherje, Eds., 9-34, World Scieniic, River edge, NJ, USA, 1995. [4] E.Gorlich nd C.Mrke, A convoluion srucure or Lguerre series, Indg.Mh.44 (198), 61-171. [5] F.M.cholewinski nd D.T.Him, The dul Poisson-Lguerre rnsorm, Trns.Am.Mh.Soc.144 (1969), 71-3. [6] H.L.Ellio nd M.Loss, Anlysis, Nros Publishing House, New Delhi, 1997. [7] Vgi S.GULIYEV nd Ygub Y.MAMMADOV, Funcion Spces nd Inegrl Operors or he Dunkl Operors on he Rel Line, Khjr Journl o Mhemics 4 (6), 17-4. [8] M.Frzier, B.Jwerh, nd G.Weiss, Lilewood-Pley heory nd he sudy o uncion spces, CBMS Regionl Conerence Series in Mhemics, Vol.79, Americn Mhemicl Sociey, Rhode Islnd, 1991.