Some identities of Laguerre polynomials arising from differential equations

Similar documents
Extended central factorial polynomials of the second kind

On the New q-extension of Frobenius-Euler Numbers and Polynomials Arising from Umbral Calculus

Differential equations associated with higher-order Bernoulli numbers of the second kind

arxiv: v1 [math.nt] 17 Jul 2015

Fourier series of sums of products of ordered Bell and poly-bernoulli functions

arxiv: v1 [math.nt] 12 Feb 2019

The graded generalized Fibonacci sequence and Binet formula

Dual Integral Equations and Singular Integral. Equations for Helmholtz Equation

Theory of Generalized k-difference Operator and Its Application in Number Theory

arxiv: v1 [math.nt] 13 Jan 2009

Homotopy Perturbation Method for Solving Partial Differential Equations of Fractional Order

Research Article New Iterative Method: An Application for Solving Fractional Physical Differential Equations

Solution of Wave Equation by the Method of Separation of Variables Using the Foss Tools Maxima

Improving the Reliability of a Series-Parallel System Using Modified Weibull Distribution

Some Applications on Generalized Hypergeometric and Confluent Hypergeometric Functions

Fourier Series. 10 (D3.9) Find the Cesàro sum of the series. 11 (D3.9) Let a and b be real numbers. Under what conditions does a series of the form

Formulas for Angular-Momentum Barrier Factors Version II

Discrete Bernoulli s Formula and its Applications Arising from Generalized Difference Operator

Research Article Numerical Range of Two Operators in Semi-Inner Product Spaces

On Integrals Involving Universal Associated Legendre Polynomials and Powers of the Factor (1 x 2 ) and Their Byproducts

Gaussian Curvature in a p-orbital, Hydrogen-like Atoms

14 Separation of Variables Method

Numerical solution of one dimensional contaminant transport equation with variable coefficient (temporal) by using Haar wavelet

Laplace - Fibonacci transform by the solution of second order generalized difference equation

DYNAMIC RESPONSE OF CIRCULAR FOOTINGS ON SATURATED POROELASTIC HALFSPACE

Strauss PDEs 2e: Section Exercise 2 Page 1 of 12. For problem (1), complete the calculation of the series in case j(t) = 0 and h(t) = e t.

4 Separation of Variables

Some Properties Related to the Generalized q-genocchi Numbers and Polynomials with Weak Weight α

221B Lecture Notes Notes on Spherical Bessel Functions

Generalized Bell polynomials and the combinatorics of Poisson central moments

Integrating Factor Methods as Exponential Integrators

Umbral calculus and Sheffer sequences of polynomials. Taekyun Kim, 1, a) Dae San Kim, 2, b) Toufik Mansour, 3, c) Seog-Hoon Rim, 4, d) and

Mathematical Scheme Comparing of. the Three-Level Economical Systems

HYDROGEN ATOM SELECTION RULES TRANSITION RATES

On the Number of Limit Cycles for Discontinuous Generalized Liénard Polynomial Differential Systems

EXISTENCE OF SOLUTIONS FOR ONE-DIMENSIONAL WAVE EQUATIONS WITH NONLOCAL CONDITIONS

Research Article On the Lower Bound for the Number of Real Roots of a Random Algebraic Equation

The functional variable method for solving the fractional Korteweg de Vries equations and the coupled Korteweg de Vries equations

TRANSFORMATION OF REAL SPHERICAL HARMONICS UNDER ROTATIONS

Legendre Polynomials - Lecture 8

Jackson 4.10 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Complete monotonicity of a function involving the p-psi function and alternative proofs

LECTURE 10. The world of pendula

Sums of finite products of Chebyshev polynomials of the third and fourth kinds

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries

STABILITY OF A PARAMETRICALLY EXCITED DAMPED INVERTED PENDULUM 1. INTRODUCTION

High Accuracy Split-Step Finite Difference Method for Schrödinger-KdV Equations

arxiv: v4 [math.nt] 20 Jan 2015

Research Article Building Infinitely Many Solutions for Some Model of Sublinear Multipoint Boundary Value Problems

$, (2.1) n="# #. (2.2)

2-loop additive mass renormalization with clover fermions and Symanzik improved gluons

Minimizing Total Weighted Completion Time on Uniform Machines with Unbounded Batch

Strauss PDEs 2e: Section Exercise 1 Page 1 of 7

NIKOS FRANTZIKINAKIS. N n N where (Φ N) N N is any Følner sequence

The Symmetric and Antipersymmetric Solutions of the Matrix Equation A 1 X 1 B 1 + A 2 X 2 B A l X l B l = C and Its Optimal Approximation

Lecture Note 3: Stationary Iterative Methods

Homework #04 Answers and Hints (MATH4052 Partial Differential Equations)

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l

arxiv: v1 [math.ca] 6 Mar 2017

CS229 Lecture notes. Andrew Ng

The second maximal and minimal Kirchhoff indices of unicyclic graphs 1

A Novel Learning Method for Elman Neural Network Using Local Search

THE PARTITION FUNCTION AND HECKE OPERATORS

Math 124B January 17, 2012

Volume 13, MAIN ARTICLES

Sums of finite products of Legendre and Laguerre polynomials

Research Article Solution of Point Reactor Neutron Kinetics Equations with Temperature Feedback by Singularly Perturbed Method

A Fictitious Time Integration Method for a One-Dimensional Hyperbolic Boundary Value Problem

Separation of Variables and a Spherical Shell with Surface Charge

Approximation and Fast Calculation of Non-local Boundary Conditions for the Time-dependent Schrödinger Equation

David Eigen. MA112 Final Paper. May 10, 2002

BP neural network-based sports performance prediction model applied research

STOCHASTIC Volterra integral equations (SVIEs) is a

Notes: Most of the material presented in this chapter is taken from Jackson, Chap. 2, 3, and 4, and Di Bartolo, Chap. 2. 2π nx i a. ( ) = G n.

EXACT CLOSED FORM FORMULA FOR SELF INDUC- TANCE OF CONDUCTOR OF RECTANGULAR CROSS SECTION

Wavelet Galerkin Solution for Boundary Value Problems

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES

VTU-NPTEL-NMEICT Project

THE NUMERICAL EVALUATION OF THE LEVITATION FORCE IN A HYDROSTATIC BEARING WITH ALTERNATING POLES

Week 6 Lectures, Math 6451, Tanveer

C. Fourier Sine Series Overview

RELATIONSHIP BETWEEN QUATERNION LINEAR CANONICAL AND QUATERNION FOURIER TRANSFORMS

Displacement Solution for a Static Vertical Rigid Movement of an Interior Circular Disc in a Transversely Isotropic Tri-Material Full-Space

Math 124B January 31, 2012

ODE Homework 2. Since M y N x, the equation is not exact. 2. Determine whether the following equation is exact. If it is exact, M y N x 1 x.

Path planning with PH G2 splines in R2

Research of Data Fusion Method of Multi-Sensor Based on Correlation Coefficient of Confidence Distance

General Decay of Solutions in a Viscoelastic Equation with Nonlinear Localized Damping

Fitting affine and orthogonal transformations between two sets of points

New families of special numbers and polynomials arising from applications of p-adic q-integrals

Introduction. Figure 1 W8LC Line Array, box and horn element. Highlighted section modelled.

Construction of Supersaturated Design with Large Number of Factors by the Complementary Design Method

NODIA AND COMPANY. GATE SOLVED PAPER Mathematics Calculus of Variations & Integral Equations. Copyright By NODIA & COMPANY

Summation of p-adic Functional Series in Integer Points

PHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased

1. Measurements and error calculus

Existence, Uniqueness and Finite Difference Solution for the Dirichlet problem of the Schrodinger-Maxwell equations

Another Class of Admissible Perturbations of Special Expressions

Revisit nonlinear differential equations associated with Bernoulli numbers of the second kind

A Brief Introduction to Markov Chains and Hidden Markov Models

Transcription:

Kim et a. Advances in Difference Equations 2016) 2016:159 DOI 10.1186/s13662-016-0896-1 R E S E A R C H Open Access Some identities of Laguerre poynomias arising from differentia equations Taekyun Kim 1,2,DaeSanKim 3, Kyung-Won Hwang 4* andjongjinseo 5 * Correspondence: khwang@dau.ac.kr 4 Department of Mathematics, Dong-A University, Busan, 49315, Repubic of Korea Fu ist of author information is avaiabe at the end of the artice Abstract In this paper, we derive a famiy of ordinary differentia equations from the generating function of the Laguerre poynomias. Then these differentia equations are used in order to obtain some properties and new identities for those poynomias. MSC: 05A19; 33C45; 11B37; 35G35 Keywords: Laguerre poynomias; differentia equations 1 Introduction The Laguerre poynomias, L n x)n 0), are defined by the generating function e 1 t xt 1 t L n x)t n see [1, 2]). 1) n0 Indeed, the Laguerre poynomia L n x) is a soution of the second order inear differentia equation xy +1 x)y + ny 0 see[2 5]). 2) From 1), we can get the foowing equation: L n x)t n n0 xt e 1 t 1 t m0 1) m x m t m 1 t) m 1 m! 1) m x m t m ) m + t m! m0 0 n 1) m ) ) n m x m t n. 3) m! n0 m0 Thus by 3), we get immediatey the foowing equation: L n x) n m0 1) m ) n m x m m! n 0) see [2, 6 8] ). 4) 2016 Kim et a. This artice is distributed under the terms of the Creative Commons Attribution 4.0 Internationa License http://creativecommons.org/icenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the origina authors) and the source, provide a ink to the Creative Commons icense, and indicate if changes were made.

Kim eta. Advances in Difference Equations 2016) 2016:159 Page 2 of 9 Aternativey, the Laguerre poynomias are aso defined by the recurrence reation as foows: L 0 x)1, L 1 x)1 x, n +1)L n+1 x)2n +1 x)l n x) nl n 1 x) n 1). 5) The Rodrigues formua for the Laguerre poynomias is given by L n x) 1 dn ex e x x n) n 0). 6) n! dx n The first few of L n x)n 0) are L 0 x)1, L 1 x)1 x, L 2 x) 1 2 x 2 4x +2 ), L 3 x) 6 1 x 3 +9x 2 18x +6 ), L 4 x) 1 x 4 16x 3 +72x 2 96x +24 ). 24 The Laguerre poynomias arise from quantum mechanics in the radia part of the soution of the Schrödinger equation for a one-eectron action. They aso describe the static Wigner functions of osciator system in the quantum mechanics of phase space. They further enter in the quantum mechanics of the Morse potentia and of the 3D isotropic harmonic osciator see [4, 5, 9]). A contour integra that is commony taken as the definition of the Laguerre poynomia is given by L n x) 1 e xt 1 t 2πi C 1 t t n 1 dt see [4, 5, 10, 11] ), 7) where the contour encoses the origin but not the point z 1. FDEs fractiona differentia equations) have wide appications in such diverse areas as fuid mechanics, pasma physics, dynamica processes and finance, etc. Most FDEs do not have exact soutions and hence numerica approximation techniques must be used. Spectra methods are widey used to numericay sove various types of integra and differentia equations due to their high accuracy and empoy orthogona systems as basis functions. It is remarkabe that a new famiy of generaized Laguerre poynomias are introduced in appying spectra methods for numerica treatments of FDEs in unbounded domains. They can aso be used in soving some differentia equations see [12 17]). Aso, it shoud be mentioned that the modified generaized Laguerre operationa matrix of fractiona integration is appied in order to sove inear muti-order FDEs which are important in mathematica physics see [12 17]). Many authors have studied the Laguerre poynomias in mathematica physics, combinatorics and specia functions see [1 30]). For the appications of specia functions and poynomias, one may referred to the papers see [18, 19, 28]).

Kim eta. Advances in Difference Equations 2016) 2016:159 Page 3 of 9 In [22], Kim studied noninear differentia equations arising from Frobenius-Euer poynomias and gave some interesting identities. In this paper, we derive a famiy of ordinary differentia equations from the generating function of the Laguerre poynomias. Then these differentia equations are used in order to obtain some properties and new identities for those poynomias. 2 Laguerre poynomias arising from inear differentia equations Let F Ft, x) 1 1 t e xt 1 t. 8) From 8), we note that F 1) dft, x) dt Thus, by 3), we get 1 t) 1 x1 t) 2) F. 9) and F 2) df1) dt 21 t) 2 4x1 t) 3 + x 2 1 t) 4) F 10) F 3) df2) dt So we are ed to put F N) 2N 61 t) 3 18x1 t) 4 +9x 2 1 t) 5 x 3 1 t) 6) F. 11) a i N N, x)1 t) i )F, 12) where N 0,1,2,... From 12), we can get equation 13): F N+1) 2N 2N + 2N 2N 2N+1 +1 a i N N, x)i1 t) i 1 )F + a i N N, x)i1 t) i 1 )F 2N a i N N, x)1 t) i ) a i N N, x)1 t) i ) 1 t) 1 x1 t) 2) F i +1)a i N N, x)1 t) i 1 x ia i N 1 N, x)1 t) i x 2N+2 +2 2N F 1) a i N N, x)1 t) i 2 )F a i N 2 N, x)1 t) i )F. 13)

Kim eta. Advances in Difference Equations 2016) 2016:159 Page 4 of 9 Repacing N by N +1in12), we get F N+1) 2N+2 +1 a i N 1 N +1,x)1 t) i )F. 14) Comparing the coefficients on both sides of 13)and14), we have and a 0 N +1,x)N +1)a 0 N, x), 15) a N+1 N +1,x)a N N, x), 16) a i N 1 N +1,x)ia i N 1 N, x) xa i N 2 N, x) N +2 i 2N + 1). 17) We note that F F 0) a 0 0, x)f. 18) Thus, by 18), we get a 0 0, x)1. 19) From 9)and12), we note that 1 t) 1 x1 t) 2) F F 1) a 0 1, x)1 t) 1 + a 1 1, x)1 t) 2) F. 20) Thus, by comparing the coefficients on both sides of 20), we get a 0 1, x)1, a 1 1, x). 21) From 15), 16), we get and a 0 N +1,x)N +1)a N N, x)n +1)Na N 1 N 1,x) N +1)NN 1) 2a 0 1, x)n + 1)! 22) a N+1 N +1,x) x)a N N, x) x) 2 a N 1 N 1,x) x) N a 1 1, x) x) N+1. 23) We observe that the matrix [a i j, x)] 0 i,j N is given by 1 1! 2! N! 0 x) 0 0 x) 2... 0 0 x) N

Kim eta. Advances in Difference Equations 2016) 2016:159 Page 5 of 9 From 17), we can get the foowing equations: and a 1 N +1,x)a 0 N, x)+n +2)a 1 N, x) { a 0 N, x)+n +2)a 0 N 1,x) } +N +2)N +1)a 1 N 1,x) N 1 N +2) i a 0 N i, x)+n +2)N +1) 3a 1 1, x) N 1 N +2) i a 0 N i, x)+n +2)N +1) 3 x) N N +2) i a 0 N i, x), 24) a 2 N +1,x)a 1 N, x)+n +3)a 2 N, x) { a 1 N, x)+n +3)a 1 N 1,x) } +N +3)N +2)a 2 N 1,x) N 2 N +3) i a 1 N i, x)+n +3)N +2) 5a 2 2, x) N 2 N +3) i a 1 N i, x)+n +3)N +2) 5 x) 2 N 1 N +3) i a 1 N i, x), 25) a 3 N +1,x)a 2 N, x)+n +4)a 3 N, x) { a 2 N, x)+n +4)a 2 N 1,x) } +N +4)N +3)a 3 N 1,x) N 3 N +4) i a 2 N i, x)+n +4)N +3) 7a 3 3, x) N 3 N +4) i a 2 N i, x)+n +4)N +3) 7 x) 3 N 2 N +4) i a 2 N i, x), 26) where x) n xx 1) x n +1)n 1), and x) 0 1. Continuing this process, we have N j+1 a j N +1,x) N + j +1) i a j 1 N i, x), 27)

Kim eta. Advances in Difference Equations 2016) 2016:159 Page 6 of 9 where j 1,2,...,N. Now we give expicit expressions for a j N +1,x), j 1,2,...,N.From 22)and24), we note that N a 1 N +1,x) N +2) i1 a 0 N i 1, x) i 1 0 N N +2) i1 N i 1 )!. 28) i 1 0 By 25)and28), we get N 1 a 2 N +1,x) N +3) i2 a 1 N i 2, x) i 2 0 N 1 N i 2 1 x) 2 i 2 0 N +3) i2 N i 2 +1) i1 N i 2 i 1 1)!. 29) i 1 0 From 26)and29), we get N 2 a 3 N +1,x) N +4) i3 a 2 N i 3, x) i 3 0 x) 3 N 2 i 3 0 N i 3 2 i 2 0 N i 3 i 2 2 i 1 0 N +4) i3 N i 3 +2) i2 N i 3 i 2 ) i1 N i 3 i 2 i 1 2)!. 30) By continuing this process, we get N j+1 a j N +1,x) x) j i j 0 N i j j+1 i j 1 0 N i j i 2 j+1 i 1 0 N + j +1) ij j N i j i k j 2k 1) ) ) i k 1 k2 N i j i 1 j + 1)!. 31) Therefore, we obtain the foowing theorem. Theorem 1 The inear differentia equation 2N F N) a i N N, x)1 t) )F i N N)

Kim eta. Advances in Difference Equations 2016) 2016:159 Page 7 of 9 has a soution F Ft, x)1 t) 1 exp xt 1 t ), where a 0N, x)n!, a N N, x) x) N, N j a j N, x) x) j N i j j i j 0 i j 1 0 N i j i 2 j i 1 0 N + j) ij j N ij i k j 2k 2) )) ) N i i j i 1 j)!. k 1 k2 From 1), we note that xt e 1 t F Ft, x) 1 t L n x)t n. 32) Thus, by 32), we get n0 ) d N F N) Ft, x) dt L n x)n) N t n N L n+n x)n + N) N t n. 33) nn On the other hand, by Theorem 1,wehave F N) 2N 2N 2N a i N N, x)1 t) i )F a i N N, x) a i N N, x) 2N n0 ) i + 1 t 0 n0 0 k0 n0 L k x)t k n ) ) i + 1 L n x) 0 t n N ) ) i + 1 a i N N, x) L n x) t n. 34) Therefore, by comparing the coefficients on both sides of 33) and34), we have the foowing theorem. Theorem 2 For n N {0} and N N, we have 1 L n+n x) n + N) N 2N a i N N, x) N ) i + 1 L n x), 0 where a 0 N, x)n!, a N N, x) x) N, N j a j N, x) x) j N i j j i j 0 i j 1 0 N i j i 2 j i 1 0 N + j) ij j N ij i k j 2k 2) )) ) N i i j i 1 j)!. k 1 k2

Kim eta. Advances in Difference Equations 2016) 2016:159 Page 8 of 9 3 Concusion It has been demonstrated that it is a fascinating idea to use differentia equations associated with the generating function or a sight variant of generating function) of specia poynomias or numbers. Immediate appications of them have been in deriving interesting identities for the specia poynomias or numbers. Aong this ine of research, here we derived a famiy of differentia equations from the generating function of the Laguerre poynomias. Then from these differentia equations we obtained interesting new identities for those poynomias. Competing interests The authors decare that they have no competing interests. Authors contributions A authors contributed equay to this work. A authors read and approved the fina manuscript. Author detais 1 Department of Mathematics, Coege of Science, Tianjin Poytechnic University, Tianjin, 300387, China. 2 Department of Mathematics, Kwangwoon University, Seou, 139-701, Repubic of Korea. 3 Department of Mathematics, Sogang University, Seou, 04107, Repubic of Korea. 4 Department of Mathematics, Dong-A University, Busan, 49315, Repubic of Korea. 5 Department of Appied mathematics, Pukyong Nationa University, Busan, 48513, Repubic of Korea. Acknowedgements This work was supported by the Dong-A university research fund. The first author is appointed as a chair professor at Tianjin Poytechnic University by Tianjin City in China from August 2015 to August 2019. Received: 25 January 2016 Accepted: 12 June 2016 References 1. Kim, T: Identities invoving Laguerre poynomias derived from umbra cacuus. Russ. J. Math. Phys. 211), 36-45 2014) 2. Zi, DG, Cuen, MR: Advanced Engineering Mathematics. Jones & Bartett, Boston 2005) 3. Abramowitz, M, Stegun, IA: Handbook of Mathematica Functions with Formuas, Graphs, and Mathematica Tabes. Nationa Bureau of Standards Appied Mathematics Series, vo. 55. U.S. Government Printing Office, Washington 1964) 4. Arfken, G, Weber, H: Mathematica Methods for Physicists. Academic Press, San Diego 2000) 5. Bhrawy, AH, Aghamdi, MA: The operationa matrix of Caputo fractiona derivatives of modified generaized Laguerre poynomias and its appications. Adv. Differ. Equ. 2013, Artice ID307 2013) 6. Srivastava, HM, Lin, S-D, Liu, S-J, Lu, H-C: Integra representations for the Lagrange poynomias, Shivey s pseudo-laguerre poynomias, and the generaized Besse poynomias. Russ. J. Math. Phys. 191), 121-130 2012) 7. Uspensky, JV: On the deveopment of arbitrary functions in series of Hermite s and Laguerre s poynomias. Ann. Math. 2) 281-4), 593-619 1926/1927) 8. Watson, GN: An integra equation for the square of a Laguerre poynomia. J. Lond. Math. Soc. S1-114),256 1936) 9. Karaseva, IA: Fast cacuation of signa deay in RC-circuits based on Laguerre functions. Russ. J. Numer. Ana. Math. Mode. 263),295-301 2011) 10. Caritz, L: Some generating functions for Laguerre poynomias. Duke Math. J. 35, 825-827 1968) 11. Caritz, L: The product of severa Hermite or Laguerre poynomias. Monatshefte Math. 66, 393-396 1962) 12. Baeanu, D, Bhrawy, AH, Taha, TM: Two efficient generaized Laguerre spectra agorithms for fractiona initia vaue probems. Abstr. App. Ana. 2013,Artice ID 546502 2013) 13. Bhrawy, AH, Abdekawy, MA, Azahrani, AA, Baeanu, D, Azahrani, EO: A Chebyshev-Laguerre-Gauss-Radau coocation scheme for soving a time fractiona sub-diffusion equation on a semi-infinite domain. Proc. Rom. Acad., Ser. A : Math. Phys. Tech. Sci. Inf. Sci. 16, 490-498 2015) 14. Bhrawy, AH, Ahamed, YA, Baeanu, D, A-Zahrani, AA: New spectra techniques for systems of fractiona differentia equations using fractiona-order generaized Laguerre orthogona functions. Fract. Cac. App. Ana. 17, 1137-1157 2014) 15. Bhrawy, AH, Aghamdi, MM, Taha, TM: A new modified generaized Laguerre operationa matrix of fractiona integration for soving fractiona differentia equations on the haf ine. Adv. Differ. Equ. 2012, Artice ID 179 2012) 16. Bhrawy, AH, Hafez, RM, Azahrani, EO, Baeanu, D, Azahrani, AA: Generaized Laguerre-Gauss-Radau scheme for first order hyperboic equations on semi-infinite domains. Rom. J. Phys. 60, 918-934 2015) 17. Bhrawy, AH, Taha, TM, Azahrani, EO, Baeanu, D, Azahrani, AA: New operationa matrices for soving fractiona differentia equations on the haf-ine. PLoS ONE 105),e0126620 2015).doi:10.1371/journa.pone.0126620 18. Chaurasia, VBL, Kumar, D: On the soutions of integra equations of Fredhom type with specia functions. Tamsui Oxf. J. Inf. Math. Sci. 28, 49-61 2012) 19. Chaurasia, VBL, Kumar, D: The integration of certain product invoving specia functions. Scientia, Ser. A, Math. Sci. 19, 7-12 2010) 20. Chen,Y,Griffin,J:Deformedq 1 -Laguerre poynomias, recurrence coefficients, and non-inear difference equations. ActaPhys.Po.A469), 1871-1881 2015) 21. Hegazi, AS, Mansour, M: Generaized q-modified Laguerre functions. Int. J. Theor. Phys. 419),1803-1813 2002)

Kim eta. Advances in Difference Equations 2016) 2016:159 Page 9 of 9 22. Kim, T: Identities invoving Frobenius-Euer poynomias arising from non-inear differentia equations. J. Number Theory 13212), 2854-2865 2012) 23. Kim, T, Kim, DS: Extended Laguerre poynomias associated with Hermite, Bernoui, and Euer numbers and poynomias. Abstr. App. Ana. 2012, Artice ID 957350 2012) 24. Kim, T, Rim, S-H, Dogy, DV, Lee, S-H: Some identities on Bernoui and Euer poynomias arising from the orthogonaity of Laguerre poynomias. Adv. Differ. Equ. 2012, Artice ID 201 2012) 25. Koepf, W: Identities for famiies of orthogona poynomias and specia functions. Integra Transforms Spec. Funct. 5, 69-102 1997) 26. Fiipuk, G, Smet, C: On the recurrence coefficients for generaized q-laguerre poynomias. J. Noninear Math. Phys. 20Supp. 1), 48-56 2013) 27. Moano, LAM: An eectrostatic mode for zeros of cassica Laguerre poynomias perturbed by a rationa factor. Math. Sci. 82), Artice ID 120 2014) 28. Singh, J, Kumar, D: On the distribution of mixed sum of independent random variabes one of them associated with Srivastava s poynomias and H-function. J. App. Math. Stat. Inform. 10, 53-62 2014) 29. Spain, B, Smith, MG: Functions of Mathematica Physics. Van Nostrand Reinhod Company, London 1970). Chapter 10 deas with Laguerre poynomias 30. Spencer, VE: Asymptotic expressions for the zeros of generaized Laguerre poynomias and Weber functions. Duke Math. J. 34), 667-675 1937)