MATH 543: FUCHSIAN DIFFERENTIAL EQUATIONS HYPERGEOMETRIC FUNCTION

Similar documents
Additional material: Linear Differential Equations

Series solutions of second order linear differential equations

Quadratic Transformations of Hypergeometric Function and Series with Harmonic Numbers

Lecture 19: Ordinary Differential Equations: Special Functions

Barnes integral representation

ODE Homework Series Solutions Near an Ordinary Point, Part I 1. Seek power series solution of the equation. n(n 1)a n x n 2 = n=0

Ch 5.4: Regular Singular Points

PRELIMINARIES FOR HYPERGEOMETRIC EQUATION. We will only consider differential equations with regular singularities in this lectures.

Elliptic functions. MATH 681: Lecture Notes. Part I. 1 Evaluating ds cos s. 18 June 2014

Considering our result for the sum and product of analytic functions, this means that for (a 0, a 1,..., a N ) C N+1, the polynomial.

Introductions to ExpIntegralEi

ENCYCLOPEDIA OF MATHEMATICS AND ITS APPLICATIONS. Special Functions GEORGE E. ANDREWS RICHARD ASKEY RANJAN ROY CAMBRIDGE UNIVERSITY PRESS

e Hypergeometric Fun ion and the Papperitz Equation

The Expansion of the Confluent Hypergeometric Function on the Positive Real Axis

Nina Virchenko. Abstract

How to Solve Linear Differential Equations

MATH COMPLEX ANALYSIS. Contents

Math Assignment 11

S. Ghorai 1. Lecture XV Bessel s equation, Bessel s function. e t t p 1 dt, p > 0. (1)

On the Weyl symbol of the resolvent of the harmonic oscillator

From trigonometry to elliptic functions

On character sums and complex functions over nite elds

The random continued fractions of Dyson and their extensions. La Sapientia, January 25th, G. Letac, Université Paul Sabatier, Toulouse.

Fredholm determinant with the confluent hypergeometric kernel

arxiv: v2 [math.ca] 2 Sep 2017

LIMIT CYCLES COMING FROM THE PERTURBATION OF 2-DIMENSIONAL CENTERS OF VECTOR FIELDS IN R 3

Section 5.2 Series Solution Near Ordinary Point

Fractional integral and generalized Stieltjes transforms for hypergeometric functions as transmutation operators

The ABC of hyper recursions

Bessel s Equation. MATH 365 Ordinary Differential Equations. J. Robert Buchanan. Fall Department of Mathematics

Contents. I Basic Methods 13

Part IB. Further Analysis. Year

Some Analytical and Numerical Consequences of Sturm Theorems

Notes on character sums and complex functions over nite elds

2. The Schrödinger equation for one-particle problems. 5. Atoms and the periodic table of chemical elements

Qualification Exam: Mathematical Methods

Laplace s Equation in Cylindrical Coordinates and Bessel s Equation (I)

INTEGRATION WORKSHOP 2003 COMPLEX ANALYSIS EXERCISES

A Note on the Differential Equations with Distributional Coefficients

Mathematics 104 Fall Term 2006 Solutions to Final Exam. sin(ln t) dt = e x sin(x) dx.

In numerical analysis quadrature refers to the computation of definite integrals.

Chapter 5.3: Series solution near an ordinary point

Complex Variables. Cathal Ormond

Bessel Functions Michael Taylor. Lecture Notes for Math 524

Notes on differential equations and hypergeometric functions (NOT for publication) F.Beukers

x x2 2 + x3 3 x4 3. Use the divided-difference method to find a polynomial of least degree that fits the values shown: (b)

Degree Master of Science in Mathematical Modelling and Scientific Computing Mathematical Methods I Thursday, 12th January 2012, 9:30 a.m.- 11:30 a.m.

arxiv: v3 [math.ca] 26 Jul 2013

Linear Differential Equations and Group Theory from Riemann to Poincare

SOME UNIFIED AND GENERALIZED KUMMER S FIRST SUMMATION THEOREMS WITH APPLICATIONS IN LAPLACE TRANSFORM TECHNIQUE

Moments of Ramanujan s Generalized Elliptic Integrals and Extensions of Catalan s Constant

FRACTIONAL HYPERGEOMETRIC ZETA FUNCTIONS

Introduction to Spherical Harmonics

Integration in General Relativity

Math 185 Homework Exercises II

A. MT-03, P Solve: (i) = 0. (ii) A. MT-03, P. 17, Solve : (i) + 4 = 0. (ii) A. MT-03, P. 16, Solve : (i)

Generalized Beta Function Defined by Wright Function

PHYS 404 Lecture 1: Legendre Functions

arxiv:math/ v1 [math.ca] 21 Mar 2006

Conformal maps. Lent 2019 COMPLEX METHODS G. Taylor. A star means optional and not necessarily harder.

Integrability, Nonintegrability and the Poly-Painlevé Test

Computing the real zeros of hypergeometric functions

Math 334 A1 Homework 3 (Due Nov. 5 5pm)

MATH5685 Assignment 3

Weierstrass and Hadamard products

Properties of orthogonal polynomials

Riemann integral and volume are generalized to unbounded functions and sets. is an admissible set, and its volume is a Riemann integral, 1l E,

Transformation formulas for the generalized hypergeometric function with integral parameter differences

Series Solutions of ODEs. Special Functions

Special Functions of Mathematical Physics

Background and Definitions...2. Legendre s Equation, Functions and Polynomials...4 Legendre s Associated Equation and Functions...

such as the ratio test. However, even without knowing the formula for a n and y 4

Chapter 2 Continuous Distributions

Closed-form Second Solution to the Confluent Hypergeometric Difference Equation in the Degenerate Case

Note on the Schwarz Triangle functions

Math221: HW# 7 solutions

Electromagnetism HW 1 math review

A finite element solution for the fractional equation

On the singularities of non-linear ODEs

Infinite Series. 1 Introduction. 2 General discussion on convergence

SPECIAL FUNCTIONS OF MATHEMATICS FOR ENGINEERS

Laplace s Résultat Remarquable[4] and its Ramifications

Review for Exam 2. Review for Exam 2.

Two special equations: Bessel s and Legendre s equations. p Fourier-Bessel and Fourier-Legendre series. p

Inner Product Spaces An inner product on a complex linear space X is a function x y from X X C such that. (1) (2) (3) x x > 0 for x 0.

ON GENERALIZED LAGUERRE POLYNOMIALS WITH REAL AND COMPLEX PARAMETER.

ARITHMETIC WITH HYPERGEOMETRIC SERIES

arxiv:math/ v1 [math.ca] 15 Jul 2004

CHAPTER 3 ELEMENTARY FUNCTIONS 28. THE EXPONENTIAL FUNCTION. Definition: The exponential function: The exponential function e z by writing

arxiv: v2 [math.ca] 19 Oct 2012

Continued Fractions for Special Functions: Handbook and Software

A Catalogue of Sturm-Liouville differential equations

Irregular continued fractions

Math Homework 2

arxiv: v1 [math-ph] 14 Apr 2015

Non-Liouvillian solutions for second order linear ODEs

A FEW REMARKS ON THE SUPREMUM OF STABLE PROCESSES P. PATIE

INTEGRAL TRANSFORMS and THEIR APPLICATIONS

Weak Solution of the Singular Cauchy Problem of Euler-Poisson-Darboux Equation for n =4

Solutions to Homework 2

Transcription:

SET 7 MATH 543: FUCHSIAN DIFFERENTIAL EQUATIONS HYERGEOMETRIC FUNCTION References: DK and Sadri Hassan. Historical Notes: lease read the book Linear Differential Equations and the Group Theory by Jeremy J. Gray, Birkhouser, 000 for the contributions of Euler, faff, Gauss, Riemann, Kummer, Jacobi and others on the symboll and on the Hypergeometric equation and hyoergeometric function. Definition. Linear ordinary differential equations having only regular singular points are called Fuchsian Differential Equations (FDE). FDE with two regular singular points Definition. (Regular singular point at ). If the transformed DE by z = has regular singular point at t = 0 then the original DE has a regular t singular point (in the extended complex plane) at z =. roposition. Second order FDE having only two singular points is equivalent to a DE with constant coefficients, hence solvable in terms of the elementary functions sin z,cos z and polynomial in z. FDE with three regular singular points: The Riemann equation and Riemann Symbol. Riemann has put a second order linear FDE with three regular singular points z = z, z = z and z = z 3 into the form u + ( + α + α + β + β + + γ + ) γ z z z z z z 3 (z z )(z z 3 )ββ z z + (z 3 z )(z 3 z )γ γ z z 3 ) + ( (z z )(z z 3 )α α z z + u (z z )(z z )(z z 3 ) = 0, ()

where α, α, β, β, γ, γ are constant satisfying the constraint α + α + β + β + γ + γ = The solution of () is denoted as the Riemann -symbol u(z) = The columns in the symbol indicate the location of the regular singular points and the corresponding roots of the indical equation, i.e.,. z = z, r = α and r = α.. z = z, r = β and r = β. 3. z = z 3, r = γ and r = γ. One can reduce the 9 number of parameters in the Riemann equation (or in the Riemann symbol) into three parameters by using the following type of transformation (i) u(z) = (z z ) r (z z ) s (z z 3 ) t v(z), r + s + t = 0 (ii) The Mobius transformation: z = (z z ) (z 3 z ) (z z ) (z 3 z ) we obtain first (from (i) above) and the using (ii) we obtain () 0 a 0 z ( ) z z α ( ) z z3 γ = z z z z (3) ( ) z z α ( ) z z3 γ = z z z z 0 0 a 0 z (4),

where z = (z z )(z 3 z ), a = α + β + γ, (5) (z z )(z 3 z ) b = α + β + γ, c = + α α (6) The symboll in the right hand side of (4) is the hypergeomtric function, F (a, b; c; z ) roblems F (a, b; c; z) = 0 0 a 0 z. rove that the hypergeometric function defined above (7) satisfies the differential equation (hypergeometric DE) (7) z( z) u + [c ( + a + b) z) u ab u = 0 (8). Find (Kummer) transformations leaving the Reiemann equation form invariant. 3. rove that where a n = F = Γ(a + n), b n = Γ(a) 4. rove the following roposition. roposition. n=0 a n b n c n z n n! Γ(b + n), c n = Γ(b) Γ(c + n) Γ(c) z Solutions of the hypergeometric function bout its regular singular points z = 0, z = and z =, provided c, b a, and c a b are not integers, are respectively given by 3

u(z) = A F (a, b; c; z) + B z c F (b c +, a c + ; c; z), (9) u(z) = A z a F (a, a c + ; a b + ; z ) + B z b F (b, b c + ; b a + ; ), (0) z u(z) = A 3 F (a, b; a + b + c; z) + B 3 z c a b F (c b, c a; + c a b; z), () where A i, B i, (i =,, 3) are arbitrary constants. 5. Find the solutions (0) and () about the regular singular points z = and z = by the use of Kummer s transformations mentioned in the r.. 6. rove the following: The Jacobi function (α,β) λ satisfying the Jacobi equation equation ( z )u + [β α (α + β + )z]u + λ(λ + α + β + )u = 0 can be written in terms of the hypergeometric function (α,β) λ = Γ(n + α + ) z F ( λ, λ + α + β; α + ; Γ(n + )Γ(α + ) ) When λ = n a non-negative integer the the solution becomes Jacobi polynomials containing the Legendre, and Tchbechev polynomials. 7. rove that when the regular singular points z = z and z 3 of the Riemann equation are pushed out then the resulting function function is the confluent hypergeometric function Φ(a, c; z) in 8. rove that Φ(a, c, z) = lim b F (a, b; c; z b ) 9. rove that the confluent hypergeometric function satisfies the DE z u + (c z) u a u = 0 () 0. rove that the point z = of the confluent hypergeometric equation () is an irregular singular point. 4

. Find solutions of the confluent hypergeometric equation about all it regular singular points. The form of the equation is of the form u(z) = A Φ(a, c; z) + B z c Φ(a, c, b z) where A and B are arbitrary constants. Find the constants a, c and b. rove that Bessel s function J v (z) satisfying the Bessel equation u + z u + ( ν z )u = 0 is given by 3. rove that d n dz Use induction. J v (z) = Γ(ν + ) (z/)ν Φ(ν + /, ν + ; iz) n F (a, b;, c; z) = Γ(a + n)γ(b + n)γ(c) Γ(a)Γ(b)Γ(c + n) 4. rove the following: (i) F ( a, b; b; z) = ( + z) a, (ii) F (, ; ; z) = ln( + z), z (iii) F (, ; 3; z ) = z sin z, (iv) F (, ; ; z ) = π (v) e z = lim b F ((, b,, z b ) (vi) The error function Erf(z) = π 0 0 F (a + n, b + n; c + n; z) dθ z sin θ, e t dt 5. rove that the Hermite-Weber differential equation u + (ν + 4 z )u = 0 can be converted to the confluent hypergeometric equation by with u(z) = e z 4 v(ξ), ξ = z v(ξ) = Φ( ν/, /; ξ) 5