The roots of The Third Jackson q-bessel Function
|
|
- Ariel Carroll
- 5 years ago
- Views:
Transcription
1 The roots of The Third Jacson q-bessel Function L. D. Abreu Departamento de Matemática Universidade de Coimbra Coimbra, Portugal J. Bustoz Department of Mathematics, Arizona State University Tempe, Arizona J. L. Cardoso Departamento de Matemática, Universidade de Tras-os-Montes e Alto Douro, Vila Real, Portugal May 8, Abstract We derive analytic bounds on the roots of the third Jacson Function. This bounds prove a conjecture of M. E. H. Ismail concerning the asymptotic behaviour of the roots. 1 Introduction. There are three nown q-analogs of classical Bessel functions [5,6] that are due to Jacson [7]. Following the notation of M. Ismail [5,6] these are designated by J υ () (z; q), = 1,, 3. The parameter q is taen to satisfy < q < 1. The third Jacson q-bessel function J v (3) (z; q) is defined as 1
2 [ J v (3) (z; q) := (qv+1 ; q) z v 1Φ 1 ] q v+1 ; q, qz This function is also nown as the Hahn-Exton q-bessel function [9,1 ]. The notation 1 Φ 1 in equation (1.1) is the standard in use for q-hypergeometric series [4]. J ν (3) (z; q) satisfies a linear q-difference equation and it is nown that J v (3) (z; q) has an infinite number of simple real zeros [9]. In this paper we will give lower and upper bounds for these zeros. The roots of these functions are of interest for several reasons. Firstly, it is intrinsically interesting to determine information about the roots of a function such as (1.1), which is an entire function of order zero. Also, the roots of J υ () (z; q) and J υ (3) (z; q) figure prominently in expansions in terms of q-fourier series [,3]. Lastly, if we denote the roots of J υ (3) (z; q) by j n,υ (3) then the mass points of the orthogonality measure for a q-analog of Lommel polynomials are located at the ponts 1/j n,υ. (3) Furthermore, although the functions defined in (1) are of a simpler character than the remaining Jacson q-bessel functions, it is hoped that the results given here for J υ (3) (z; q) may be extended in the future to J υ () (z; q), = 1,. The Roots of J υ (3) (z; q). We will prove two lemmas stating the existence of an odd number of roots in a certain interval and then we will prove that J v (3) (z; q) has only one root in each such interval. First we will apply the following transformation to (1): [ ] [ ] (c; q) 1 Φ 1 c ; q, z = (z; q) 1 Φ 1 z ; q, c This produces J v (3) (z; q) = (qz ; q) z v 1Φ 1 This last relation in series form gives υ (z; q) = zv [ ] qz ; q, q v+1 ( 1) (qz ; q) q (+v+1) (qz ; q) (q; q) = (1)
3 = zv = ( 1) (q+1 z ; q) (q; q) q (+v+1) () This representation will be critical in the proof of the next two lemmas. [ ] Lemma 1 If q v+1 < (1 q) then sgn J v (3) (q m ; q) = ( 1) m, m = 1,,... Proof: Set z = q m in (.1) to obtain q mv v (q m ; q) = ( 1) (q m++1 ; q) (q; q) = q (+v+1). Now observing that (q m++1 ; q) = if < m, the series on the right side of this last equality can be written as where ( 1) (q m++1 ; q) q (+v+1). (q; q) =m Setting j = m in this last series yields: (q; q) m J q mυ υ (3) (q m ; q) = ( 1) m ( 1) j A j j= A j = (qj+1 ; q) (q; q) j+m q (j+m)(j+m+v+1). Now we prove that A j+1 < A j.a calculation shows that A j+1 < A j is equivalent to q m+j+v+1 < (1 q m+j+1 )(1 q j+1 ). But the left hand side of this inequality is decreasing in m and j, while the right hand side of the inequality is increasing in m and j. So we only need to verify the case j = m =, that is q v+1 < (1 q), but this is the hypothesis of the Lemma. Clearly, since A j+1 < A j, then sgn( 1) m j= ( 1) j A j = ( 1) m. Lemma 1 states that there exist an odd number of roots in the interval (q m + 1, q m ). The next lemma will refine this statement. 3
4 Lemma Let q v+1 < (1 q) and define α (v) m (q) = log(1 q m+v 1 q m ). Then [ ] log q sgn (q m + α (v) m (q) ; q) = ( 1) m 1, m = 1,,... v Proof: First observe that the function α (v) m (q) is well defined, because if q v+1 < (1 q) then q v+1 < (1 q) and so, for positive integer m, q m+v < (1 q m ) 1 qm+v >. Being defined, it is clear that is positive, because 1 q m 1 qm+v < 1 holds for any q (, 1). 1 q m Observe also that α (v) m (q) < 1 log(1 qm+v ) > log q q m+v < 1 q m (1 q)(1 q m ), which is true if q v+1 < (1 q). So, we have < α (v) m (q) < 1. Now, set z = q m + α (v) m (q) in (). The substitution gives q mv + vα(v) m (q) v (q m + α (v) m (q) ; q) = m = =m 1 ( 1) (q m+α (v) ( 1) (q m+α (v) m (q)++1 ;q) (q;q) m (q)++1 ;q) (q;q) q (+v+1) + q (+v+1). Denote the first sum above by S 1 and the second by S. If m, then < α (v) m (q) < 1 implies that sgn(q m+α(v) m (q)++1 ; q) = ( 1) m 1. Thus sgn S 1 = ( 1) m 1, m = 1,,... In S set j = m + 1 to obtain where S = ( 1) m 1 j= ( 1) j A j, (v) A j = (qα m (q)+j ; q) q (j+m 1)(j+m+v). (q; q) j+m 1 A calculation shows that A j+1 < A j reduces to q j+m+v < (1 q α(v) m (q)+j ) (1 q m+j ), which holds because q m+v = (1 q α(v) m (q) )(1 q m ) and because the left side of the last inequality is decreasing in j and the right hand side is increasing in j. The infinite series is thus positive and therefore 4
5 sgns = ( 1) m 1 = sgns 1 From Lemma 1 and Lemma we now that J v (3) (z; q) has an odd number of roots in the interval (q m +α(v) m (q), q m ). The next theorem proves that there is exactly one root in each such interval and that there are no other roots. Theorem 3 If q v+1 < (1 q) and if w (υ) (3) (q) are the positive roots of J v (z; q),ordered increasing in, then w (v) (q) = q +ɛ(ν), with < ɛ (υ) < α (v) (q), = 1,,... Proof: From the preceding lemmas we now that v the form w (v) = q +ɛ, with < ɛ < α (v) (q). To simplify the notation we will set F (z) = (q;q) (z; q). (q ν+1 ;q) z ν v (z; q) has roots of We will prove that the only positive roots of F (z) inside the dis z < q m are the w (υ) (q), = 1,,...m. Suppose there are other roots ±λ, = 1,,..., P m ; λ >. By Jensens Theorem [1] we can write: 1 π log F (q m e iθ ) dθ π m P m = = log q m w + m log q m + ɛ + = m + m log q log q log q m λ P m log q m λ m ɛ + P m log q m λ (3) On the other hand, by the definition of the q-bessel function, we have: F (q m e iθ ) = ( 1) q (+1) m e iθ (q v+1 ; q) (q; q) = q m +m =( 1) m e imθ (q v+1 ; q) m (q; q) m 5 ( 1) q (+1) e iθ. (q m+v+1 ; q) (q m+1 ; q) = m
6 Then we have So that, lim log F (q m e iθ ) = m + m log q log(q v+1 ; q) m log(q; q) m + log ( 1) q (+1) e iθ (q m+v+1 ; q) (q m+1 ; q). 1 π π Now observe that lim = m = m log F (q m e iθ ) m + m dθ = lim + lim 1 π π log = m ( 1) q (+1) e iθ = (q m+v+1 ; q) (q m+1 ; q) log q log(q v+1 ; q) log ( 1) q (+1) e iθ (q m+v+1 ; q) (q m+1 ; q) dθ. = ( 1) q (+1) e iθ [4] The limit above is uniform in θ. By the Jacobi Triple Product Identity = ( q 1 e iθ ) (q 1 ) = (q; qe iθ ; e iθ ; q). Using the uniform convergence to interchange the limit and the integral: lim = 1 π 1 π π π log ( 1) q (+1) e iθ (q m+v+1 ; q) (q m+1 ; q) dθ = m log (q; qe iθ ; e iθ ; q) dθ π = log + 1 π 1 = log + π = log j= log (qe iθ ; q) 1 dθ + π π π log (1 q j+1 e iθ ) dθ + 6 log (e iθ ; q) dθ j= 1 π log (1 q j e iθ ) dθ π
7 The integrals in the next to the last equality above vanish because of the mean value theorem for harmonic functions. We have thus concluded that lim 1 π log F (q m e iθ ) m + m dθ = lim log q log(q v+1 ; q). π From (3) we can write: Pm lim ( log q m λ ) lim ( log q m ɛ ) = log(q v+1 ; q) (4) But, as can be seen by the Taylor expansion of α v (q), ɛ = O(q ) and this implies ɛ <. Also P m log q m λ > log q m λ 1 as m. So the identity (4) can only hold if the first sum is empty, and the only roots are thus ± w (υ) (q), = 1,,... Remar 1. It follows from (4) that = ɛ = log(qν+1 ;q) log q. Remar. Observe that for fixed j, we can always choose m sufficiently large so that q m+j+v+1 < (1 q m+j+1 )(1 q j+1 ) and q j+m+v < (1 q αv m(q)+j )(1 q m+j ). Thus w m q m+ 1 when m without the restriction q υ+1 < (1 q). In [5] Ismail conjectured that 1) lim q m w m (υ) (q) = 1 w (υ) m+1 (q ) w (υ) m (q ) ) lim = 1. q The asymptotic relation above establishes these conjectures. 7
8 w (υ) Remar 3. Lemmas 1 and and Theorem 3 state that the roots (q) satisfy the inequalities q m +α(υ) m (q) < w (υ) m (q) < q m. These bounds are quite accurate. This is evident if we estimate the length of the interval containing the roots. A somewhat tedious calculation with Taylor series shows that q m q m +α(υ) m (q) = q m +υ O(1). Clearly, for fixed q satisfying the conditions of the theorem, the bounds become increasingly accurate as either m or υ increases. References [1] L. V. Ahlfors, Complex Analysis, McGraw Hill (1979). [] J. Bustoz and J.L.Cardoso, Basic Analog of Fourier Series on a q-linear grid, Journal of Approximation Theory, 11(1), [3] J. Bustoz and S.K.Suslov, Basic Analog of Fourier Series on a q- Quadratic Grid, Methods and Applications of Analysis, 5 (1998), [4] G. Gasper and M. Rahman, Basic Hypergeometric Series, Encyclopedia of Mathematics and its Applications, Vol. 35, Cambridge (1999). [5] M. E. H. Ismail, Some Properties of Jacsons Third q-bessel Function, to appear. [6] M. E. H. Ismail, The Zeros of Basic Bessel Functions, the Functions J υ+ax (x), and Associated Orthogonal Polynomials, Journal of Mathematical Analysis and Applications, 86 (198), [7] F.H. Jacson, On Generalized Functions of Legendre and Bessel, Transactions of the Royal Society of Edinburgh, 41(194), 1-8. [8] H. T. Koelin, Some Basic Lommel Polynomials, Journal of Approximation Theory, 96(1999),
9 [9] H. T. Koelin and R. F. Swarttouw, On the zeros of the Hahn-Exton q-bessel Function and Associated q-lommel Polynomials, Journal of Mathematical Analysis and Applications, 186(1994), [1] R. Swarttouw, The Hahn-Exton q-bessel Function, thesis, Technische Universiteit Delft,
OWN ZEROS LUIS DANIEL ABREU
Pré-Publicações do Departamento de Matemática Universidade de Coimbra Preprint Number 4 3 FUNCTIONS q-orthogonal WITH RESPECT TO THEIR OWN ZEROS LUIS DANIEL ABREU Abstract: In [4], G. H. Hardy proved that,
More informationSpectral analysis of two doubly infinite Jacobi operators
Spectral analysis of two doubly infinite Jacobi operators František Štampach jointly with Mourad E. H. Ismail Stockholm University Spectral Theory and Applications conference in memory of Boris Pavlov
More informationA q-linear ANALOGUE OF THE PLANE WAVE EXPANSION
A q-linear ANALOGUE OF THE PLANE WAVE EXPANSION LUÍS DANIEL ABREU, ÓSCAR CIAURRI, AND JUAN LUIS VARONA Abstract. We obtain a q-linear analogue of Gegenbauer s expansion of the plane wave. It is expanded
More informationPositivity of Turán determinants for orthogonal polynomials
Positivity of Turán determinants for orthogonal polynomials Ryszard Szwarc Abstract The orthogonal polynomials p n satisfy Turán s inequality if p 2 n (x) p n 1 (x)p n+1 (x) 0 for n 1 and for all x in
More informationBessel s and legendre s equations
Chapter 12 Bessel s and legendre s equations 12.1 Introduction Many linear differential equations having variable coefficients cannot be solved by usual methods and we need to employ series solution method
More informationSpecial Functions of Mathematical Physics
Arnold F. Nikiforov Vasilii B. Uvarov Special Functions of Mathematical Physics A Unified Introduction with Applications Translated from the Russian by Ralph P. Boas 1988 Birkhäuser Basel Boston Table
More information0.1 Valuations on a number field
The Dictionary Between Nevanlinna Theory and Diophantine approximation 0. Valuations on a number field Definition Let F be a field. By an absolute value on F, we mean a real-valued function on F satisfying
More informationLUIS DANIEL ABREU. The Gegenbauer expansion of the two variable complex exponential in terms of the ultraspherical polynomials
Pré-Publicações do Departamento de Matemática Universidade de Coimbra Preprint Number 05 7 THE REPRODUCING KERNEL STRUCTURE ASSOCIATED TO FOURIER TYPE SYSTEMS AND THEIR QUANTUM ANALOGUES LUIS DANIEL ABREU
More information= i 0. a i q i. (1 aq i ).
SIEVED PARTITIO FUCTIOS AD Q-BIOMIAL COEFFICIETS Fran Garvan* and Dennis Stanton** Abstract. The q-binomial coefficient is a polynomial in q. Given an integer t and a residue class r modulo t, a sieved
More informationSeries of Error Terms for Rational Approximations of Irrational Numbers
2 3 47 6 23 Journal of Integer Sequences, Vol. 4 20, Article..4 Series of Error Terms for Rational Approximations of Irrational Numbers Carsten Elsner Fachhochschule für die Wirtschaft Hannover Freundallee
More informationOn an Eigenvalue Problem Involving Legendre Functions by Nicholas J. Rose North Carolina State University
On an Eigenvalue Problem Involving Legendre Functions by Nicholas J. Rose North Carolina State University njrose@math.ncsu.edu 1. INTRODUCTION. The classical eigenvalue problem for the Legendre Polynomials
More informationENCYCLOPEDIA OF MATHEMATICS AND ITS APPLICATIONS. Special Functions GEORGE E. ANDREWS RICHARD ASKEY RANJAN ROY CAMBRIDGE UNIVERSITY PRESS
ENCYCLOPEDIA OF MATHEMATICS AND ITS APPLICATIONS Special Functions GEORGE E. ANDREWS RICHARD ASKEY RANJAN ROY CAMBRIDGE UNIVERSITY PRESS Preface page xiii 1 The Gamma and Beta Functions 1 1.1 The Gamma
More informationMath Homework 2
Math 73 Homework Due: September 8, 6 Suppose that f is holomorphic in a region Ω, ie an open connected set Prove that in any of the following cases (a) R(f) is constant; (b) I(f) is constant; (c) f is
More informationA Riemann Lebesgue Lemma for Jacobi expansions
A Riemann Lebesgue Lemma for Jacobi expansions George Gasper 1 and Walter Trebels Dedicated to P. L. Butzer on the occasion of his 65-th birthday (To appear in Contemporary Mathematics) Abstract. A Lemma
More informationBounds on Turán determinants
Bounds on Turán determinants Christian Berg Ryszard Szwarc August 6, 008 Abstract Let µ denote a symmetric probability measure on [ 1, 1] and let (p n ) be the corresponding orthogonal polynomials normalized
More informationwhich implies that we can take solutions which are simultaneous eigen functions of
Module 1 : Quantum Mechanics Chapter 6 : Quantum mechanics in 3-D Quantum mechanics in 3-D For most physical systems, the dynamics is in 3-D. The solutions to the general 3-d problem are quite complicated,
More informationCOMPLEX ANALYSIS Spring 2014
COMPLEX ANALYSIS Spring 24 Homework 4 Solutions Exercise Do and hand in exercise, Chapter 3, p. 4. Solution. The exercise states: Show that if a
More informationPólya s Random Walk Theorem arxiv: v2 [math.pr] 18 Apr 2013
Pólya s Random Wal Theorem arxiv:131.3916v2 [math.pr] 18 Apr 213 Jonathan ova Abstract This note presents a proof of Pólya s random wal theorem using classical methods from special function theory and
More informationHankel Operators plus Orthogonal Polynomials. Yield Combinatorial Identities
Hanel Operators plus Orthogonal Polynomials Yield Combinatorial Identities E. A. Herman, Grinnell College Abstract: A Hanel operator H [h i+j ] can be factored as H MM, where M maps a space of L functions
More informationAsymptotics of Integrals of. Hermite Polynomials
Applied Mathematical Sciences, Vol. 4, 010, no. 61, 04-056 Asymptotics of Integrals of Hermite Polynomials R. B. Paris Division of Complex Systems University of Abertay Dundee Dundee DD1 1HG, UK R.Paris@abertay.ac.uk
More informationBASIC HYPERGEOMETRIC SERIES
ENCYCLOPEDIA OF MATHEMATICS AND ITS APPLICATIONS BASIC HYPERGEOMETRIC SERIES Second Edition GEORGE GASPER Northwestern University, Evanston, Illinois, USA MIZAN RAHMAN Carleton University, Ottawa, Canada
More informationInfinite Continued Fractions
Infinite Continued Fractions 8-5-200 The value of an infinite continued fraction [a 0 ; a, a 2, ] is lim c k, where c k is the k-th convergent k If [a 0 ; a, a 2, ] is an infinite continued fraction with
More informationOn rational approximation of algebraic functions. Julius Borcea. Rikard Bøgvad & Boris Shapiro
On rational approximation of algebraic functions http://arxiv.org/abs/math.ca/0409353 Julius Borcea joint work with Rikard Bøgvad & Boris Shapiro 1. Padé approximation: short overview 2. A scheme of rational
More informationJournal of Combinatorial Theory, Series A
Journal of Combinatorial Theory, Series A 118 (2011) 240 247 Contents lists available at ScienceDirect Journal of Combinatorial Theory, Series A wwwelseviercom/locate/jcta Bailey s well-poised 6 ψ 6 -series
More informationAnalytic Theory of Polynomials
Analytic Theory of Polynomials Q. I. Rahman Universite de Montreal and G. Schmeisser Universitat Erlangen -Niirnberg CLARENDON PRESS-OXFORD 2002 1 Introduction 1 1.1 The fundamental theorem of algebra
More informationCOMBINATORICS OF RAMANUJAN-SLATER TYPE IDENTITIES. James McLaughlin Department of Mathematics, West Chester University, West Chester, PA 19383, USA
COMBINATORICS OF RAMANUJAN-SLATER TYPE IDENTITIES James McLaughlin Department of Mathematics, West Chester University, West Chester, PA 9383, USA jmclaughl@wcupa.edu Andrew V. Sills Department of Mathematical
More informationEQ: What are limits, and how do we find them? Finite limits as x ± Horizontal Asymptote. Example Horizontal Asymptote
Finite limits as x ± The symbol for infinity ( ) does not represent a real number. We use to describe the behavior of a function when the values in its domain or range outgrow all finite bounds. For example,
More informationAn integral formula for L 2 -eigenfunctions of a fourth order Bessel-type differential operator
An integral formula for L -eigenfunctions of a fourth order Bessel-type differential operator Toshiyuki Kobayashi Graduate School of Mathematical Sciences The University of Tokyo 3-8-1 Komaba, Meguro,
More informationMOMENTS OF HYPERGEOMETRIC HURWITZ ZETA FUNCTIONS
MOMENTS OF HYPERGEOMETRIC HURWITZ ZETA FUNCTIONS ABDUL HASSEN AND HIEU D. NGUYEN Abstract. This paper investigates a generalization the classical Hurwitz zeta function. It is shown that many of the properties
More informationON LINEAR COMBINATIONS OF
Física Teórica, Julio Abad, 1 7 (2008) ON LINEAR COMBINATIONS OF ORTHOGONAL POLYNOMIALS Manuel Alfaro, Ana Peña and María Luisa Rezola Departamento de Matemáticas and IUMA, Facultad de Ciencias, Universidad
More informationThe infrared properties of the energy spectrum in freely decaying isotropic turbulence
The infrared properties of the energy spectrum in freely decaying isotropic turbulence W.D. McComb and M.F. Linkmann SUPA, School of Physics and Astronomy, University of Edinburgh, UK arxiv:148.1287v1
More informationOn the number of dominating Fourier coefficients of two newforms
On the number of dominating Fourier coefficients of two newforms Liubomir Chiriac Abstract Let f = n 1 λ f (n)n (k 1 1)/2 q n and g = n 1 λg(n)n(k 2 1)/2 q n be two newforms with real Fourier coeffcients.
More informationarxiv: v3 [math.ca] 14 Oct 2015
Symmetry, Integrability and Geometry: Methods and Applications Certain Integrals Arising from Ramanujan s Noteboos SIGMA 11 215), 83, 11 pages Bruce C. BERNDT and Armin STRAUB arxiv:159.886v3 [math.ca]
More informationCERTAIN INTEGRALS ARISING FROM RAMANUJAN S NOTEBOOKS
CERTAIN INTEGRALS ARISING FROM RAMANUJAN S NOTEBOOKS BRUCE C. BERNDT AND ARMIN STRAUB Abstract. In his third noteboo, Ramanujan claims that log x dx + π 2 x 2 dx. + 1 In a following cryptic line, which
More informationDispersion for the Schrodinger Equation on discrete trees
Dispersion for the Schrodinger Equation on discrete trees April 11 2012 Preliminaries Let Γ = (V, E) be a graph, denoting V the set of vertices and E the set of edges, assumed to be segments which are
More informationUNIFORM BOUNDS FOR BESSEL FUNCTIONS
Journal of Applied Analysis Vol. 1, No. 1 (006), pp. 83 91 UNIFORM BOUNDS FOR BESSEL FUNCTIONS I. KRASIKOV Received October 8, 001 and, in revised form, July 6, 004 Abstract. For ν > 1/ and x real we shall
More informationMOCK THETA FUNCTIONS AND THETA FUNCTIONS. Bhaskar Srivastava
NEW ZEALAND JOURNAL OF MATHEMATICS Volume 36 (2007), 287 294 MOCK THETA FUNCTIONS AND THETA FUNCTIONS Bhaskar Srivastava (Received August 2004). Introduction In his last letter to Hardy, Ramanujan gave
More informationA Right Inverse Of The Askey-Wilson Operator arxiv:math/ v1 [math.ca] 5 Oct 1993 B. Malcolm Brown and Mourad E. H. Ismail
A Right Inverse Of The Askey-Wilson Operator arxiv:math/9310219v1 [math.ca] 5 Oct 1993 B. Malcolm Brown and Mourad E. H. Ismail Abstract We establish an integral representation of a right inverse of the
More informationHarmonic sets and the harmonic prime number theorem
Harmonic sets and the harmonic prime number theorem Version: 9th September 2004 Kevin A. Broughan and Rory J. Casey University of Waikato, Hamilton, New Zealand E-mail: kab@waikato.ac.nz We restrict primes
More informationPHYS 404 Lecture 1: Legendre Functions
PHYS 404 Lecture 1: Legendre Functions Dr. Vasileios Lempesis PHYS 404 - LECTURE 1 DR. V. LEMPESIS 1 Legendre Functions physical justification Legendre functions or Legendre polynomials are the solutions
More informationElectromagnetism HW 1 math review
Electromagnetism HW math review Problems -5 due Mon 7th Sep, 6- due Mon 4th Sep Exercise. The Levi-Civita symbol, ɛ ijk, also known as the completely antisymmetric rank-3 tensor, has the following properties:
More informationVectors in Function Spaces
Jim Lambers MAT 66 Spring Semester 15-16 Lecture 18 Notes These notes correspond to Section 6.3 in the text. Vectors in Function Spaces We begin with some necessary terminology. A vector space V, also
More informationHigher monotonicity properties of q gamma and q-psi functions
Advances in Dynamical Systems and Applications ISSN 973-5321, Volume x, Number x, pp. 1 13 (2xx) http://campus.mst.edu/adsa Higher monotonicity properties of q gamma and q-psi functions Mourad E. H. Ismail
More informationa non-standard generating function for continuous dual q-hahn polynomials una función generatriz no estándar para polinomios q-hahn duales continuos
Revista de Matemática: Teoría y Aplicaciones 2011 181 : 111 120 cimpa ucr issn: 1409-2433 a non-standard generating function for continuous dual -hahn polynomials una función generatriz no estándar para
More informationIntroduction to Series and Sequences Math 121 Calculus II Spring 2015
Introduction to Series and Sequences Math Calculus II Spring 05 The goal. The main purpose of our study of series and sequences is to understand power series. A power series is like a polynomial of infinite
More informationContents. I Basic Methods 13
Preface xiii 1 Introduction 1 I Basic Methods 13 2 Convergent and Divergent Series 15 2.1 Introduction... 15 2.1.1 Power series: First steps... 15 2.1.2 Further practical aspects... 17 2.2 Differential
More informationre r = n. e 2r + O(e 3r ), P 1 = r2 + 3r + 1 2r(r + 1) 2 1 P 2 = 2r(r + 1)
Notes by Rod Canfield July, 994 file: /bell/bellmoser.tex update(s: August, 995 The Moser-Wyman expansion of the Bell numbers. Let B n be the n-th Bell number, and r be the solution of the equation Then
More informationInner 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.
Inner Product Spaces An inner product on a complex linear space X is a function x y from X X C such that (1) () () (4) x 1 + x y = x 1 y + x y y x = x y x αy = α x y x x > 0 for x 0 Consequently, (5) (6)
More informationarxiv: v2 [math.ca] 19 Oct 2012
Symmetry, Integrability and Geometry: Methods and Applications Def inite Integrals using Orthogonality and Integral Transforms SIGMA 8 (, 77, pages Howard S. COHL and Hans VOLKMER arxiv:.4v [math.ca] 9
More informationLecture 14 Conformal Mapping. 1 Conformality. 1.1 Preservation of angle. 1.2 Length and area. MATH-GA Complex Variables
Lecture 14 Conformal Mapping MATH-GA 2451.001 Complex Variables 1 Conformality 1.1 Preservation of angle The open mapping theorem tells us that an analytic function such that f (z 0 ) 0 maps a small neighborhood
More informationSubharmonic functions
Subharmonic functions N.A. 07 Upper semicontinuous functions. Let (X, d) be a metric space. A function f : X R { } is upper semicontinuous (u.s.c.) if lim inf f(y) f(x) x X. y x A function g is lower semicontinuous
More informationJUST THE MATHS UNIT NUMBER DIFFERENTIATION APPLICATIONS 5 (Maclaurin s and Taylor s series) A.J.Hobson
JUST THE MATHS UNIT NUMBER.5 DIFFERENTIATION APPLICATIONS 5 (Maclaurin s and Taylor s series) by A.J.Hobson.5. Maclaurin s series.5. Standard series.5.3 Taylor s series.5.4 Exercises.5.5 Answers to exercises
More informationPhase Calculations for Planar Partition Polynomials
Phase Calculations for Planar Partition Polynomials Robert Boyer and Daniel Parry Abstract. In the study of the asymptotic behavior of polynomials from partition theory, the determination of their leading
More informationTewodros Amdeberhan, Dante Manna and Victor H. Moll Department of Mathematics, Tulane University New Orleans, LA 70118
The -adic valuation of Stirling numbers Tewodros Amdeberhan, Dante Manna and Victor H. Moll Department of Mathematics, Tulane University New Orleans, LA 7011 Abstract We analyze properties of the -adic
More informationTHE ZERO-DISTRIBUTION AND THE ASYMPTOTIC BEHAVIOR OF A FOURIER INTEGRAL. Haseo Ki and Young One Kim
THE ZERO-DISTRIBUTION AND THE ASYMPTOTIC BEHAVIOR OF A FOURIER INTEGRAL Haseo Ki Young One Kim Abstract. The zero-distribution of the Fourier integral Q(u)eP (u)+izu du, where P is a polynomial with leading
More informationCOMBINATORICS OF RAMANUJAN-SLATER TYPE IDENTITIES
COMBINATORICS OF RAMANUJAN-SLATER TYPE IDENTITIES James McLaughlin Department of Mathematics, West Chester University, West Chester, PA 9383, USA jmclaughl@wcupa.edu Andrew V. Sills Department of Mathematical
More informationElements with Square Roots in Finite Groups
Elements with Square Roots in Finite Groups M. S. Lucido, M. R. Pournaki * Abstract In this paper, we study the probability that a randomly chosen element in a finite group has a square root, in particular
More informationd 1 µ 2 Θ = 0. (4.1) consider first the case of m = 0 where there is no azimuthal dependence on the angle φ.
4 Legendre Functions In order to investigate the solutions of Legendre s differential equation d ( µ ) dθ ] ] + l(l + ) m dµ dµ µ Θ = 0. (4.) consider first the case of m = 0 where there is no azimuthal
More informationIntroductions to ExpIntegralEi
Introductions to ExpIntegralEi Introduction to the exponential integrals General The exponential-type integrals have a long history. After the early developments of differential calculus, mathematicians
More informationCONVERGENCE OF THE FOURIER SERIES
CONVERGENCE OF THE FOURIER SERIES SHAW HAGIWARA Abstract. The Fourier series is a expression of a periodic, integrable function as a sum of a basis of trigonometric polynomials. In the following, we first
More informationEigenvalues, random walks and Ramanujan graphs
Eigenvalues, random walks and Ramanujan graphs David Ellis 1 The Expander Mixing lemma We have seen that a bounded-degree graph is a good edge-expander if and only if if has large spectral gap If G = (V,
More informationq-series IDENTITIES AND VALUES OF CERTAIN L-FUNCTIONS Appearing in the Duke Mathematical Journal.
q-series IDENTITIES AND VALUES OF CERTAIN L-FUNCTIONS George E. Andrews, Jorge Jiménez-Urroz and Ken Ono Appearing in the Duke Mathematical Journal.. Introduction and Statement of Results. As usual, define
More informationPart III Example Sheet 1 - Solutions YC/Lent 2015 Comments and corrections should be ed to
TIME SERIES Part III Example Sheet 1 - Solutions YC/Lent 2015 Comments and corrections should be emailed to Y.Chen@statslab.cam.ac.uk. 1. Let {X t } be a weakly stationary process with mean zero and let
More informationPOLYNOMIALS WITH COEFFICIENTS FROM A FINITE SET
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 00, Number 0, Pages 000 000 S 0002-9947(XX)0000-0 POLYNOMIALS WITH COEFFICIENTS FROM A FINITE SET PETER BORWEIN, TAMÁS ERDÉLYI, FRIEDRICH LITTMANN
More informationUpper Bounds for Partitions into k-th Powers Elementary Methods
Int. J. Contemp. Math. Sciences, Vol. 4, 2009, no. 9, 433-438 Upper Bounds for Partitions into -th Powers Elementary Methods Rafael Jaimczu División Matemática, Universidad Nacional de Luján Buenos Aires,
More informationComplex Variables...Review Problems (Residue Calculus Comments)...Fall Initial Draft
Complex Variables........Review Problems Residue Calculus Comments)........Fall 22 Initial Draft ) Show that the singular point of fz) is a pole; determine its order m and its residue B: a) e 2z )/z 4,
More informationLegendre s Equation. PHYS Southern Illinois University. October 13, 2016
PHYS 500 - Southern Illinois University October 13, 2016 PHYS 500 - Southern Illinois University Legendre s Equation October 13, 2016 1 / 10 The Laplacian in Spherical Coordinates The Laplacian is given
More informationRecall that any inner product space V has an associated norm defined by
Hilbert Spaces Recall that any inner product space V has an associated norm defined by v = v v. Thus an inner product space can be viewed as a special kind of normed vector space. In particular every inner
More informationTwo special equations: Bessel s and Legendre s equations. p Fourier-Bessel and Fourier-Legendre series. p
LECTURE 1 Table of Contents Two special equations: Bessel s and Legendre s equations. p. 259-268. Fourier-Bessel and Fourier-Legendre series. p. 453-460. Boundary value problems in other coordinate system.
More informationConvergence properties of Kemp s q-binomial distribution. Stefan Gerhold and Martin Zeiner
FoSP Algorithmen & mathematische Modellierung FoSP Forschungsschwerpunkt Algorithmen und mathematische Modellierung Convergence properties of Kemp s -binomial distribution Stefan Gerhold and Martin Zeiner
More informationAN ASYMPTOTICALLY UNBIASED MOMENT ESTIMATOR OF A NEGATIVE EXTREME VALUE INDEX. Departamento de Matemática. Abstract
AN ASYMPTOTICALLY UNBIASED ENT ESTIMATOR OF A NEGATIVE EXTREME VALUE INDEX Frederico Caeiro Departamento de Matemática Faculdade de Ciências e Tecnologia Universidade Nova de Lisboa 2829 516 Caparica,
More informationComplex Analysis Homework 9: Solutions
Complex Analysis Fall 2007 Homework 9: Solutions 3..4 (a) Let z C \ {ni : n Z}. Then /(n 2 + z 2 ) n /n 2 n 2 n n 2 + z 2. According to the it comparison test from calculus, the series n 2 + z 2 converges
More informationCentrum voor Wiskunde en Informatica
Centrum voor Wiskunde en Informatica Modelling, Analysis and Simulation Modelling, Analysis and Simulation Two-point Taylor expansions of analytic functions J.L. Lópe, N.M. Temme REPORT MAS-R0 APRIL 30,
More informationMath 259: Introduction to Analytic Number Theory More about the Gamma function
Math 59: Introduction to Analytic Number Theory More about the Gamma function We collect some more facts about Γs as a function of a complex variable that will figure in our treatment of ζs and Ls, χ.
More informationC.7. Numerical series. Pag. 147 Proof of the converging criteria for series. Theorem 5.29 (Comparison test) Let a k and b k be positive-term series
C.7 Numerical series Pag. 147 Proof of the converging criteria for series Theorem 5.29 (Comparison test) Let and be positive-term series such that 0, for any k 0. i) If the series converges, then also
More informationSuper congruences involving binomial coefficients and new series for famous constants
Tal at the 5th Pacific Rim Conf. on Math. (Stanford Univ., 2010 Super congruences involving binomial coefficients and new series for famous constants Zhi-Wei Sun Nanjing University Nanjing 210093, P. R.
More informationTHE GENERALIZED GOURSAT-DARBOUX PROBLEM FOR A THIRD ORDER OPERATOR. 1. Introduction In this paper we study the generalized Goursat-Darboux problem
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 5, Number, February 997, Pages 47 475 S 000-9939(97)03684-8 THE GENERALIZED GOURSAT-DARBOUX PROBLEM FOR A THIRD ORDER OPERATOR JAIME CARVALHO E SILVA
More informationHigher Monotonicity Properties of q-gamma and q-psi Functions
Advances in Dynamical Systems and Applications ISSN 973-5321, Volume 8, Number 2, pp. 247 259 (213) http://campus.mst.edu/adsa Higher Monotonicity Properties of q-gamma and q-psi Functions Mourad E. H.
More informationProperties of orthogonal polynomials
University of South Africa LMS Research School University of Kent, Canterbury Outline 1 Orthogonal polynomials 2 Properties of classical orthogonal polynomials 3 Quasi-orthogonality and semiclassical orthogonal
More informationLecture 4: Series expansions with Special functions
Lecture 4: Series expansions with Special functions 1. Key points 1. Legedre polynomials (Legendre functions) 2. Hermite polynomials(hermite functions) 3. Laguerre polynomials (Laguerre functions) Other
More informationON THE LINEAR INDEPENDENCE OF THE SET OF DIRICHLET EXPONENTS
ON THE LINEAR INDEPENDENCE OF THE SET OF DIRICHLET EXPONENTS Abstract. Given k 2 let α 1,..., α k be transcendental numbers such that α 1,..., α k 1 are algebraically independent over Q and α k Q(α 1,...,
More informationCongruence Properties of Partition Function
CHAPTER H Congruence Properties of Partition Function Congruence properties of p(n), the number of partitions of n, were first discovered by Ramanujan on examining the table of the first 200 values of
More informationNew Multiple Harmonic Sum Identities
New Multiple Harmonic Sum Identities Helmut Prodinger Department of Mathematics University of Stellenbosch 760 Stellenbosch, South Africa hproding@sun.ac.za Roberto Tauraso Dipartimento di Matematica Università
More informationThe ABC of hyper recursions
Journal of Computational and Applied Mathematics 90 2006 270 286 www.elsevier.com/locate/cam The ABC of hyper recursions Amparo Gil a, Javier Segura a,, Nico M. Temme b a Departamento de Matemáticas, Estadística
More informationMarcos J. González Departamento de Matemáticas Puras y Aplicadas, Universidad Simón Bolívar, Sartenejas, Caracas, Venezuela
#A89 INTEGERS 16 (016) ON SIERPIŃSKI NUMBERS OF THE FORM '(N)/ n Marcos J. González Departamento de Matemáticas Puras y Aplicadas, Universidad Simón Bolívar, Sartenejas, Caracas, Venezuela mago@usb.ve
More informationINTEGRAL TRANSFORMS and THEIR APPLICATIONS
INTEGRAL TRANSFORMS and THEIR APPLICATIONS Lokenath Debnath Professor and Chair of Mathematics and Professor of Mechanical and Aerospace Engineering University of Central Florida Orlando, Florida CRC Press
More informationProblem 1A. Find the volume of the solid given by x 2 + z 2 1, y 2 + z 2 1. (Hint: 1. Solution: The volume is 1. Problem 2A.
Problem 1A Find the volume of the solid given by x 2 + z 2 1, y 2 + z 2 1 (Hint: 1 1 (something)dz) Solution: The volume is 1 1 4xydz where x = y = 1 z 2 This integral has value 16/3 Problem 2A Let f(x)
More informationClimbing an Infinite Ladder
Section 5.1 Section Summary Mathematical Induction Examples of Proof by Mathematical Induction Mistaken Proofs by Mathematical Induction Guidelines for Proofs by Mathematical Induction Climbing an Infinite
More information(a) Determine the general solution for φ(ρ) near ρ = 0 for arbitary values E. (b) Show that the regular solution at ρ = 0 has the series expansion
Problem 1. Curious Wave Functions The eigenfunctions of a D7 brane in a curved geometry lead to the following eigenvalue equation of the Sturm Liouville type ρ ρ 3 ρ φ n (ρ) = E n w(ρ)φ n (ρ) w(ρ) = where
More informationClimbing an Infinite Ladder
Section 5.1 Section Summary Mathematical Induction Examples of Proof by Mathematical Induction Mistaken Proofs by Mathematical Induction Guidelines for Proofs by Mathematical Induction Climbing an Infinite
More informationFinite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product
Chapter 4 Hilbert Spaces 4.1 Inner Product Spaces Inner Product Space. A complex vector space E is called an inner product space (or a pre-hilbert space, or a unitary space) if there is a mapping (, )
More information1 Solutions in cylindrical coordinates: Bessel functions
1 Solutions in cylindrical coordinates: Bessel functions 1.1 Bessel functions Bessel functions arise as solutions of potential problems in cylindrical coordinates. Laplace s equation in cylindrical coordinates
More informationHarmonic Analysis. 1. Hermite Polynomials in Dimension One. Recall that if L 2 ([0 2π] ), then we can write as
Harmonic Analysis Recall that if L 2 ([0 2π] ), then we can write as () Z e ˆ (3.) F:L where the convergence takes place in L 2 ([0 2π] ) and ˆ is the th Fourier coefficient of ; that is, ˆ : (2π) [02π]
More informationAdvanced Computational Fluid Dynamics AA215A Lecture 2 Approximation Theory. Antony Jameson
Advanced Computational Fluid Dynamics AA5A Lecture Approximation Theory Antony Jameson Winter Quarter, 6, Stanford, CA Last revised on January 7, 6 Contents Approximation Theory. Least Squares Approximation
More informationHomepage: WWW: george/
LIST OF PUBLICATIONS of George Gasper (George Gasper, Jr.) (2/16/07 version) Department of Mathematics, Northwestern University, Evanston, Illinois 60208, (847) 491-5592 E-mail: george at math.northwestern.edu
More informationMATH 324 Summer 2011 Elementary Number Theory. Notes on Mathematical Induction. Recall the following axiom for the set of integers.
MATH 4 Summer 011 Elementary Number Theory Notes on Mathematical Induction Principle of Mathematical Induction Recall the following axiom for the set of integers. Well-Ordering Axiom for the Integers If
More informationSupplement: Efficient Global Point Cloud Alignment using Bayesian Nonparametric Mixtures
Supplement: Efficient Global Point Cloud Alignment using Bayesian Nonparametric Mixtures Julian Straub Trevor Campbell Jonathan P. How John W. Fisher III Massachusetts Institute of Technology 1. Rotational
More informationSTRONG NONNEGATIVE LINEARIZATION OF ORTHOGONAL POLYNOMIALS
STRONG NONNEGATIVE LINEARIZATION OF ORTHOGONAL POLYNOMIALS Ryszard Szwarc * Institute of Mathematics Wroclaw University pl. Grunwaldzki 2/4 50-384 Wroclaw POLAND and Institute of Mathematics Polish Academy
More informationOn convergent power series
Peter Roquette 17. Juli 1996 On convergent power series We consider the following situation: K a field equipped with a non-archimedean absolute value which is assumed to be complete K[[T ]] the ring of
More informationJacobi-Angelesco multiple orthogonal polynomials on an r-star
M. Leurs Jacobi-Angelesco m.o.p. 1/19 Jacobi-Angelesco multiple orthogonal polynomials on an r-star Marjolein Leurs, (joint work with Walter Van Assche) Conference on Orthogonal Polynomials and Holomorphic
More information