= ZZ [(qjw(ft)u(/3/)l*"y'

Similar documents
Journal of Inequalities in Pure and Applied Mathematics

Numerical approximation to ζ(2n+1)

Chapter 3: Theory of Modular Arithmetic 38

Math 124B February 02, 2012

ON LACUNARY INVARIANT SEQUENCE SPACES DEFINED BY A SEQUENCE OF MODULUS FUNCTIONS

On a quantity that is analogous to potential and a theorem that relates to it

Solution to HW 3, Ma 1a Fall 2016

Integral operator defined by q-analogue of Liu-Srivastava operator

Journal of Number Theory

On the Quasi-inverse of a Non-square Matrix: An Infinite Solution

A Bijective Approach to the Permutational Power of a Priority Queue

k. s k=1 Part of the significance of the Riemann zeta-function stems from Theorem 9.2. If s > 1 then 1 p s

Auchmuty High School Mathematics Department Advanced Higher Notes Teacher Version

Pascal s Triangle (mod 8)

New problems in universal algebraic geometry illustrated by boolean equations

Method for Approximating Irrational Numbers

THE NUMBER OF TWO CONSECUTIVE SUCCESSES IN A HOPPE-PÓLYA URN

H.W.GOULD West Virginia University, Morgan town, West Virginia 26506

On the ratio of maximum and minimum degree in maximal intersecting families

Measure Estimates of Nodal Sets of Polyharmonic Functions

ON THE INVERSE SIGNED TOTAL DOMINATION NUMBER IN GRAPHS. D.A. Mojdeh and B. Samadi

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS

A proof of the binomial theorem

A STUDY OF HAMMING CODES AS ERROR CORRECTING CODES

Compactly Supported Radial Basis Functions

(n 1)n(n + 1)(n + 2) + 1 = (n 1)(n + 2)n(n + 1) + 1 = ( (n 2 + n 1) 1 )( (n 2 + n 1) + 1 ) + 1 = (n 2 + n 1) 2.

A NOTE ON VERY WEAK SOLUTIONS FOR A CLASS OF NONLINEAR ELLIPTIC EQUATIONS

A Hartree-Fock Example Using Helium

(read nabla or del) is defined by, k. (9.7.1*)

of the contestants play as Falco, and 1 6

On the ratio of maximum and minimum degree in maximal intersecting families

MULTIPLE MELLIN AND LAPLACE TRANSFORMS OF I-FUNCTIONS OF r VARIABLES

A Relativistic Electron in a Coulomb Potential

SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF 2 2 OPERATOR MATRICES

PHYS 301 HOMEWORK #10 (Optional HW)

Miskolc Mathematical Notes HU e-issn Tribonacci numbers with indices in arithmetic progression and their sums. Nurettin Irmak and Murat Alp

Results on the Commutative Neutrix Convolution Product Involving the Logarithmic Integral li(

Boundedness for Marcinkiewicz integrals associated with Schrödinger operators

On the Poisson Approximation to the Negative Hypergeometric Distribution

NOTE. Some New Bounds for Cover-Free Families

Markscheme May 2017 Calculus Higher level Paper 3

Multiple Experts with Binary Features

MATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE. We consider second order constant coefficient scalar linear PDEs on R n. These have the form

On absence of solutions of a semi-linear elliptic equation with biharmonic operator in the exterior of a ball

Lecture 28: Convergence of Random Variables and Related Theorems

15 Solving the Laplace equation by Fourier method

Research Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function

Semicanonical basis generators of the cluster algebra of type A (1)

Lecture 23. Representation of the Dirac delta function in other coordinate systems

On the integration of the equations of hydrodynamics

Goodness-of-fit for composite hypotheses.

working pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50

6 PROBABILITY GENERATING FUNCTIONS

Application of Fractional Calculus Operators to Related Areas

Using Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu

Vanishing lines in generalized Adams spectral sequences are generic

NOT E ON DIVIDED DIFFERENCE S

As is natural, our Aerospace Structures will be described in a Euclidean three-dimensional space R 3.

15.081J/6.251J Introduction to Mathematical Programming. Lecture 6: The Simplex Method II

STUDY OF SOLUTIONS OF LOGARITHMIC ORDER TO HIGHER ORDER LINEAR DIFFERENTIAL-DIFFERENCE EQUATIONS WITH COEFFICIENTS HAVING THE SAME LOGARITHMIC ORDER

arxiv: v1 [physics.pop-ph] 3 Jun 2013

THE EVALUATION OF CERTAIN ARITHMETIC SUMS

Lecture 16 Root Systems and Root Lattices

arxiv: v1 [math.nt] 12 May 2017

Asymptotically Lacunary Statistical Equivalent Sequence Spaces Defined by Ideal Convergence and an Orlicz Function

3.1 Random variables

RADIAL POSITIVE SOLUTIONS FOR A NONPOSITONE PROBLEM IN AN ANNULUS

arxiv: v1 [math.nt] 28 Oct 2017

16 Modeling a Language by a Markov Process

EEO 401 Digital Signal Processing Prof. Mark Fowler

Multiple Criteria Secretary Problem: A New Approach

MODULE 5a and 5b (Stewart, Sections 12.2, 12.3) INTRO: In MATH 1114 vectors were written either as rows (a1, a2,..., an) or as columns a 1 a. ...

JENSEN S INEQUALITY FOR DISTRIBUTIONS POSSESSING HIGHER MOMENTS, WITH APPLICATION TO SHARP BOUNDS FOR LAPLACE-STIELTJES TRANSFORMS

What Form of Gravitation Ensures Weakened Kepler s Third Law?

ESSENTIAL NORM OF AN INTEGRAL-TYPE OPERATOR ON THE UNIT BALL. Juntao Du and Xiangling Zhu

Section 8.2 Polar Coordinates

Chaos and bifurcation of discontinuous dynamical systems with piecewise constant arguments

(received April 9, 1967) Let p denote a prime number and let k P

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution

Analytic Evaluation of two-electron Atomic Integrals involving Extended Hylleraas-CI functions with STO basis

Graphs of Sine and Cosine Functions

ON THE ASYMPTOTIC BEHAVIO R OF SOLUTIONS OF LINEAR DIFFERENCE EQUATION S

arxiv: v1 [math.co] 6 Mar 2008

arxiv: v1 [math.co] 4 May 2017

Application of Parseval s Theorem on Evaluating Some Definite Integrals

Solving Some Definite Integrals Using Parseval s Theorem

763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012

titrrvers:rtt t>1 NO~~H CAROLINA

DonnishJournals

GROWTH ESTIMATES THROUGH SCALING FOR QUASILINEAR PARTIAL DIFFERENTIAL EQUATIONS


Moment-free numerical approximation of highly oscillatory integrals with stationary points

Green s Identities and Green s Functions

C/CS/Phys C191 Shor s order (period) finding algorithm and factoring 11/12/14 Fall 2014 Lecture 22

Divisibility. c = bf = (ae)f = a(ef) EXAMPLE: Since 7 56 and , the Theorem above tells us that

Math 301: The Erdős-Stone-Simonovitz Theorem and Extremal Numbers for Bipartite Graphs

On a generalization of Eulerian numbers

arxiv: v1 [math.ca] 31 Aug 2009

A generalization of the Bernstein polynomials

Transcription:

Expansions Involving Hypegeometic Functions of Two Vaiables By Aun Vema 1. Intoduction. A systematic study of expansions of Appell 's hypegeometic functions of two vaiables has been made by Buchnall and haundy [3]-[5] in 1942. Recently, Ragab [11], obtained two expansions of Kampé de Féiet's double hypegeometic functions which besides incopoating some of the expansions of Buchnall and haundy [3], [4], gave some new expansions also. In 2 of this pape a systematic attempt has been made to extend the expansions concening Appell functions to the Kampé de Féiet's double hypegeometic functions by using the two symbolic opeatos of Buchnall and haundy. In 4 using the method of iteation of seies some of the expansions due to haundy [5], [6], Niblett [10], Wimp and Luke [8] have been extended to the Kampé de Féiet's function. The pape is concluded by showing how the induction by using the Laplace tansfom and its invese can be employed to extend these esults to G-functions of two vaiables defined ecently by Agawal [1]*. It may be pointed out that these expansions ae vey geneal in natue and incopoate a vey lage numbe of expansions fo the functions of two vaiables. 2. Kampé de Féietf [2] intoduced the double hypegeometic functions of highe ode (i.e. with moe paametes) in two vaiables, namely: (1) («J (ft); (/?/) («-); (O = ZZ [(qjw(ft)u(/3/)l*"y' [Ik [1]» [ W [(«.)]» [(«.')]. ' povided p + v < p + a + 1 o p + v = p + c + 1 and x j + \y \ < min (1, 2"-"+I). Hee (aa) means A paametes of the type ax, a2,, aa and [a]n = a[a + l][a + 2] [a + n - 1]; [o]0 = 1. Fo special values of p, v, p, a the function (1) educes to the Appell's fou double hypegeometic functions. Following Buchnall and haundy [3], [4], we define the opeatos A(A) and V(A) as A(A) = "S + h, S 4- h; h, ô + ô' + h whee ô = xd/dx, ô = yd/dy. Now it can be seen without difficulty V(A) = 'h, 5 + h' + h; ô + h,ô' + h Received Febuay 21, 1966. * I am indebted to D. R. P. Agawal fo letting me ead his unpublished manuscipt [1]. t Fo definition and popeties of these functions, see [2]. 590

(2) (3) EXPANSIONS INVOLVING HYPERGEOMETRI FUNTIONS 591 V(a)F A(a)F (4) V(a)A(c)F («) («.); («/) («) (S,); (8/) («m) (8.); (S/) = F ß + 1 I (oy), a v P i(yp) _o- + 1 I (8 ), a; (O, a v + 1 p 4-1 (ft), a; (ft'), a, a <y (O; (8/) Ai 4-1 (am), a v + 1 (0,), e; (ft'), c p 4-1 (tp), c 0-4-1 (8J, a; (ô/), a Then following the method of Buchnall and haundy and using the following identities (5) (6) fh, to + n 4- /i;~] = y \_m + h, n + h } =0 Tm + h,n + h{] [h, m + n + h] y_ %> [l] [ ni][ n] [l] [h) [ m][ n] h m n + l] (Gauss's theoem) (Gauss's theoem with eithe m o n a positive intege) (7) (8) _ y_[ }[h}2[ m][ n] ÍTo [1], [h + - l] [to 4- A] [n + h] (limiting fom of Dougall's theoem) [h,m + n + h to 4- k, n 4- fc m + h,n + h, fc, m 4- n 4- fc ;] [fc A] [fc]2[ m] [ n] -z (9) o [l] [fc + - l] [m + fc], [n 4- fc] [A] (limiting fom of Dougall's theoem) y [h k] [ to], [ n] o [l] [Aj [ fc to n + 1], (Saalschütz's theoem with eithe to o» a positive intege) we get the following five geneal expansions (10) F np. («m) (y,) (SO; (s/) X i7 y [(^)]2[(ft)]Qa][(ft')],, " S[l][W[o]S[(80][(8/)] V ß V + 1 P + l (7 («) + 2 a +, (00 4- ; a +, (0,') + a + 2, + It (80 + ; (ô/) +

592 ARUN VERMA (ID [-n(gp)u(ft)u(ft')] xj/ :U []2, [(SO], t(8.')] [a], («0 4-2, a + (ft) + ; (0/) 4- + 2 (SO +,a [- a], [(«Qk [(ft)], [(ft')] M (12) = t= > [1], [c + - l][]»[a]i[(8.)m(8,')], M + 1 v + 1 P + 1 <+ 1 (-)[(«Qk[(ft)U(ft')], (13) = ^o [1], [a + - 1], [(tow [(8.)] [(8/)], M + 1 c P a + 1 + - («/) 4-, c + a; y («0 + 2, c 4-2 (00 4-, a 4- ; (0/) +, a 4-4- 2, a + 2 (50 4-, c + 2; (S/) +, c + 2 («) 4-2, a + (ft) 4- ; (0/) 4- (yp) 4-2 (50 4-, a + 2; (ô/) +, a + 2 (14) (-)[a c],[(ao]2,[(ft)][(0/)],[a],,, [1], t]2, [a]2, [(50], [(5/)], M + 1 («) 4-2, c + ; V + 1 (ft) +, a + ; (0/) 4-, a 4- P + 1 (to 4-2, a 4-2 ^ <+ 1 (50 4-, c 4- ; (s/) 4-, c + It may be pointed out that the Eq. (10) on specialization of paametes gives Eqs. (26), (29), (32), (35), (36), (38), (41) and ou (11) gives (27), (33), (37), (39); (12) gives (30) and (42); (13) gives Equations (28), (34) and (40); (14) gives Eqs. (31) and (41) of Buchnall and haundy [3]. The above expansions (12) and (13) wee deduced by Ragab [11] by the iteation of seies. 3. In this section, we fist state and then pove some moe geneal expansions F 'A + G (aa), (go) B + H (6B), (A*); (bb'), (A*') Xx (cc) py D + E (dd), (eb); (dd'), (eb) = AA' ^"^m+n^o)]m+n[(ha)]m[(hh)]n[h + am m + 1],-1 (15) m=0 n=0 X [A' 4- ßn - n + i]n-, A B + 2 F E + 2 X(-xTi-yTF [l]m [1]» [(c)un \{dd)]m l(dd')]n (aa) (bb), 1 4- A/a, -m; (6*'), 1 + h'/ß, -n (f) (eb), A 4- «to m 4-1, A/«; (eb), h' + ßn n + I, A/0 F + G 2 + H D (/O + m + n, (ga) + m -\- n (A/0 4- m, A 4- «to; (A«') + n, h + ßn (ce) + m + n (dd) + to; (dd') + n

(16) (17) (18) F A B 1) M B D EXPANSIONS INVOLVING HYPERGEOMETRI FUNTIONS (aa) (bs); (O (e) (dd); (dd') Xx ß!l (-)+í[(«p)uo(ft)],[(ft')]s 0 í=0 [1], [1]. []+S [(8,)] [(8/)] X xvf (ao (60; (6»') (cc) (du); (db') ' P (7 X. M// +P ß + Ul = (-)+,[(«p)uo(ft)],[(ft')]s í=í í=í [1], [1]. []+8 [(80], [(S.')] E + D u + F = x UO, (bb), (50, -; (6B'), (S/), -s (ce), (am) Z) 4- v (d*), (ft); (dß'), (ft') («p) 4-4- s (00 4- ; (0/) + s + + s (8 ) + ; (O 4- s 1 + A + p l + B + a + p D 4- v M ao (,);(,') p +1 a (c*), (dc) (c), (/0; (c/), (/,') (-)+'[(Q]+0(6Q] 5 [l] [1], [c + - 1], [(6 ')]sxy c' + s - 1]. [(e.)],+8 [(/O], [(//)]. w (c,) 4-» + s c 4- + s!],-+» x'y' c + + s 1, (aa), -, (60, (50; s, (O, («/) (cc), (ofm) (dfl), (ft); (dd'), (ft') («0 4-» 4- s (ft) + ; (0/) 4- s c + 2 4-2s, + + s (50 + ; (5/) 4- s X. M.'/ f (60 4-? ;(60 4- s x E (ee) 4-4- s y.1 4- F c + 2, (/O + ; c + 2s, (/,) p (Ap) 2 + q c+ - 1, -, (50; c + s - 1, -s, (B,') w + D (aw), (dd) u + v (cu), (60; (c,/), (6/)

594 ARTJN VERMA To pove (15) equate the coefficients of [(ox)]jf+jy [(bb)]ti [(bb')]n x AT V A p. [1U HI* Ke*)]* [(«-')]* on both the sides and then put M + = to, N 4- s = n afte witing definition fo the Kampé de Féiet's function. We then get 1 = [A 4- am][ti 4- ßN] x the seies (-)+s[(/0 + M + ivwh+.[(ff«) + M 4- N}p+Q++s 0 í=0 5=0 [1]p [1]Q [l] [1]. [(cc) + M + A^]P+e+,+s [(A,) 4- MUP [(Ah') 4- NUq U + A + («- 1) _4- MaUp-i [1 4- A' 4- s(0-1) 4- ATflWi X [(dd) + M],+P [(dd') 4- N]s+Q Next, set -\- P = T, s 4- Q = U and change the ode of summation. Then it is not difficult to see that the coefficient of the tem independent of xy on the ight-hand side is unity. It thus emains to show that the coefficient of x yu on the ight-hand side (T > 0, U > 0) vanish, i.e. n=yy (-)+*[l + A + K«-1)4- Af«]-i [1 + A' 4- s(0-1)4- Nß]y^. í ÚÍ [1], [1], [l]-, [l]uwhich is a known esult due to haundy [6]. It may be emaked that this esult is a genealisation of a esult due to haundy [6] and contains as a special case a esult due to Niblett [10]. To pove (16), equate the coefficients of [(aa)]u+n [(bb)]ul(bb )]n,m n [1]m [1]n 1(cc)}m+n [(do)]* [(dd)u ' M on both the sides and then using the seies definition of the Kampé de Féiet's function and setting 4- m = P and s + n = Q, we get that m n _ []m+at[(5q]m 1(5 )U y y [(«p)]f+o [(ft)]p [(ft')]e p q X V - [(a )W [(ft)]«[(ft')]. í^o ^o []p+0 [(8 )]p [(8,')]c ^ ( P Q I \+s+m+n x/ =0 s-0 [l]_m [l]s-jv [l]p- [1]q Using a lemma due to haundy, we find that îo P = M ; s Q the double seies in the cooked backets is equal to 1 and fo P > s, Q > N its value is zeo and hence the esult is established. This esult incopoates as special case some of the esults due to haundy (Eqs. (8), (9), (10) and (11) of [5]) and fo y = p = 0 this educes to a esult due to Jey L. Fields and Jet Wimp which in tun contains a lage numbe of othe expansions as special cases. To pove (17), equate the coefficient of l(aa)]m+n [(60W l(bb)]s" [l].v [1]* [(cc)w [(do)]m [(dd')w '

EXPANSIONS INVOLVING HYPERGEOMETRI FUNTIONS 595 on both the sides, then use the seies definition of the Kampé de Féiet's function and use the second lemma of haundy [5], afte setting P + = m and Q 4- s = n to get the desied esult. This esult also contains as a special case some of the expansions due to haundy [5] and educes fo y = p = 0 to a esult due to Jey L. Fields and Jet Wimp [7]. The poof of (18) can be developed on exactly simila lines. This esult also gives as special cases some known expansions due to Fields and Wimp. 4. In this section we shall extend the esults deduced in the pevious sections to G-functions of two vaiables. Agawal [1] defined a G-function of two vaiables though a Banes contou integal in the fom p,t,s,q (ao (70; (7/) (so _, -L f f *( +,,)*(, )a;v did* 47T" J so J too whee "(ft,0, (7.O +, (ßm2) V, (7*0 + V, U - (Ä.,+1.,) + 1,1 - (7*1+1.«) -, 1 (0m,+l.O *({+u) = n - (eo +? 4-,; [fn+i.v) f V) (50 4-4- Í?. 77,1 (7.2+l,f) -J' and 0 ^ TOj áí,oáffli í,0á^áí Oáiíáí,0^»áp. The sequence of paametes (0 n), (0m2), (7»0, (7»2) and (e») ae such that none of the poles of the integand coincide. The paths of integation ae indented, if necessay, in such a manne that all the poles of T[ßj Q, j = 1, 2,, Toi, and [0A-' j],k = 1, 2,, m2 lie to the ight and those of [7/4-17], J = 1, 2,, j»2 ; T[yK + ], K = 1, 2,, vi and [l - ey + + ij], j" = 1, 2,, n lie to the left of the imaginay axis. The integal (19) conveges if p + q + s + t < 2(?»! + v! + n), and p + q + s + t < 2(m, + V2 + n), I ag x I < i(mi + vx + n - %[p + q + s + <]), I ag y \ < T(m-2 + v2 + n - %[p + q + s + t\). Now using the technique of Laplace tansfom and its invese as used fo the functions of one vaiable by Luke and Wimp [8] and by the autho fo obtaining geneal expansions of G-functions of Meije [9], one can also wite the extension to (7-functions of all the esults deduced in this pape. Fo instance, one can genealise (10) in the fom

596 ARUN VERMA Gfl.V+t,P+U,V,W tt+ptv+q,p,o+l X!J (ap+o (ft+o;(ftvo 0,(50; 0, (s/)_ («p+p) a,(0,+o; a> (ftv4), a,(ô,);, The poof of this esult is funished by mathematical induction and fo t = u = p = q = 0, v = w = 1 this educes to (10) on using the equation (iii) of 3 and (A) of 4 of Agawal [1]. Similaly all the othe esults can be extended to G-functions of two vaiables. These extended esults wee given ealie by Meije [9], Luke and Wimp [8] and othes. Depatment of Mathematics The Univesity of Goakhpu Goakhpu, India 1-0 [IJ V 1. R. P. Agawal, "An extension of Meije's G-functions," Poc. Nat. Inst. Sei. Sect. A, v. 32, 1965. 2. P. Appell & J. Kampé de Féiet, Fonctions Hype géométiques et Hypespheiques, Gauthie-Villas, Pais, 1926. 3. J. L. Buchnall & T. W. haundy, "Expansions of Appell's double hypegeometic functions," Quat. J. Math. Oxfod Se., v. 11, 1940, pp. 249-270. MR 2, 287. 4. J. L. Buchnall & T. W. haundy, ibid., II, Quat. J. Math. Oxfod Se., v. 12, 1941, pp. 112-128. MR 3, 118. 5. T. W. haundy, "Expansions of hypegeometic functions," Quat. J. Math. Oxfod Se., v. 13, 1942, pp. 159-171. MR 4,197. 6. T. W. haundy, "On lausen's hypegeometic identity," Quat. J. Math. Oxfod Se., 2, v.9, 1958, pp. 265-274. MR 20 #5898. 7. J. L. Fields & J. Wimp, "Expansions of hypegeometic functions in hypegeometic functions," Math. omp., v. 15, 1961, pp. 390-395. MR 23 # A3289. 8. Y. L. Luke & Jet Wimp, "Expansion fomulas fo genealized hypegeometic functions," Rend. ie. Mat. Palemo (2), v. 11, 1962, pp. 351-366. 9.. S. Meije, a) "Expansion theoems fo the G-functions," I, II, Nedel. Akad. Wetensch. Poc. Se. A 55 = Indag. Math., v. 14, 1952, pp. 369-379, 483-487. MR 14, 469; MR 14, 642. b) ibid., Ill, IV, V, Nedel. Akad. Wetensch. Poc. Se. A 56 = Indag. Math., v. 15, 1953, pp. 43-49, 187-193, 349-357. MR 14, 748; MR 14, 979; MR 15, 422. c) ibid., VI, VII, VIII, Nedel. Akad. Wetensch. Poc. Se. A 57 = Indag. Math., v. 16, 1954, pp. 77-82, 83-91, 273-279. MR 15, 791; MR 15, 955. d) ibid., IX, Nedel. Akad. Wetensch. Poc. Se. A 58 = Indag. Math., v. 17, pp. 243-251. MR 16, 1106. 10. J. D. Niblett, "Some hypegeometic identities," Pacifie J. Math., v. 2, 1952, pp. 219-225. MR 13, 940. 11. F. M. Ragab, "Expansions of Kampé de Féiet's double hypegeometic functions of highe ode," J. Reine. An-gew. Math., v. 212, 1963, pp. 113-119. MR 27 #352. 12. A. Vema, "A class of expansions of G-functions and Laplace tansfom," Math. omp., v. 19, 1965, pp. 661-664. (S/)