亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        A Note on the Generalized and Universal Associated Legendre Equations?

        2018-07-09 06:46:24KeeganKirkKyleBryentonandNasserSaad
        Communications in Theoretical Physics 2018年7期

        Keegan L.A.Kirk, Kyle R.Bryenton, and Nasser Saad

        School of Mathematical&Computational Sciences,University of Prince Edward Island,550 University Avenue,Charlottetown,PEI C1A 4P3,Canada

        1 Introduction

        Recently,the Universal Associated Legendre Polynomials

        has been the subject of many interesting studies.[1?7]These polynomials are solutions to the differential equation(see Ref.[2]and the references therein):

        in which b=0,m′=Through partial-fraction decomposition of the rational coefficient of the Pm′?′(r)term,Eq.(2)is shown to be a slight modification of the well-known Generalized Associated Legendre Equation[8?19]

        The differential equation(3)was introduced first by Bateman in his analysis of the harmonic equations(Ref.[8],page 389).Following Bateman’s work,this was later intensively studied in a series of research articles by Kuipers and Meulenbeld for complex-valued parameters k,m,and n.[9?17]The recent book of Virchenko and Fedotova[19]was devoted to the subsequent development of the theory of the Generalized Associated Legendre Functions and their applications.

        As we shall prove in the present work,both differential equations(2)and(3)are members of a more general class of differential equations characterized by

        where aj,bj,j=1,2,3,c3are real parameters and ξ1

        The exact solutions of the differential equation(4)are given,along with their relations to the published solutions of the Generalized and Universal Associated Legendre Differential Equations(2)and(3).New solvable classes of differential equations useful for the analysis of quantum systems are obtained.[20?22]

        2 Exact Solutions

        The differential equation(4)has three regular singular points,r ∈ {ξ1,ξ2,∞}with exponents μ1, μ2,andμ∞,respectively,determined as the roots of the indicial(quadratic)equations:

        According to the classical theory of ordinary differential equations,[23]Eq.(4)is reducible to the hypergeometric equation.To this end,the general solutions of Eq.(4)take the form

        where the exponents μ1and μ2are evaluated using Eqs.(5)and(6)respectively.The substitution of Eq.(8)into Eq.(4)yields the following hypergeometric-type equation for the function f≡f(r):

        Employing the M?bius transformation,z=(αr+ β)/(γr+ δ),for αδ? βγ0,yields

        Thus,if γ=0,the change of variables r→z≡z(r)transforms Eq.(10)into an equation of the same type as that of Eq.(9).This in turn implies

        To express the solutions of this equation in terms of hypergeometric functions,one must impose either of the following necessary conditions on α, β,and δ:

        Should we impose the conditions as given(i),Eq.(11)reduces to(denoting f→)

        (z)=z1?2μ2+(b1+a1ξ2)/(ξ2?ξ1)

        More precisely,the analytic solutions of the differential equation(4),for arbitrary constants A1and A2,are

        where

        Equivalently,the exact solutions of the differential equation(4)may also be expressed as(denoting f→)

        As a result,we are able to obtain Eq.(18)from Eq.(21)and vice versa.This relationship may be confirmed using the linear transformation(Ref.[24],Eq.(15.8.4)):

        After some simplification,it follows that

        For the second solution(17),we may again apply Eq.(24)to obtain

        To obtain the expression in terms ofthe Pfaff transformation(Ref.[24],Eq.(15.8.1)),

        must be used for the hypergeometric functions on the right-hand side of Eq.(26).It is sufficient to focus on either one of the solution sets.

        3 Connection with the Generalized Associated Legendre Equation

        This section serves to demonstrate the relationship between the differential equations(3)and(4).First denote

        then,using partial-fraction decomposition,Eq.(4)reads

        Using Eq.(28),the indicial equations(5)and(6)may be expressed as

        Thus,Eq.(29)reduces to

        with the exact solutions,determined via Eq.(21),given by:

        as found earlier by Kuipers et al.forμ1=n/2 andμ2=?m/2.In this case equation(30)reads

        For ξ2= ?ξ1=1,Eq.(33)reduces to the Generalized Associated Legendre Differential Equation.Different choices of ξ1and ξ2give rise to other interesting classes of differential equations,(e.g. ξ1=0, ξ2=1).The mathematical properties of these other classes(such as the weight-function,the recurrence relation,the orthogonality conditions,etc.)will be the focus of future work.

        4 Connection with the Universal Associated Legendre Equation

        To establish the connection between the solutions of the differential equation(4)and that of the Universal Associated Legendre Equation(2)as given by Eq.(1),we express Eq.(1)in terms of the hypergeometric function.Using the

        Legendre Duplication Formula,Γ(2z)=22z?1Γ(z)Γ(z+1/2)/Eq.(1)can be written as

        Further,by means of the Pochhammer identity Γ(z ? ν)=(?1)νΓ(z)/(1 ? z)ν,we obtain

        With the assumption that ?(1/2)(?′? m′)or(1/2)(1 ? (?′? m′))=0,?1,?2,...,this equation may now be written in terms of the hypergeometric equation

        with the understanding that the limit of the right-hand side is well-defined as r→0.Since

        it easily follows that

        The identity(Ref.[24],Eq.(15.8.6))

        implies

        With a1=2(μ1+μ2?1),the differential equation(4)reads after an application of partial-fraction decomposition,

        Using the identity(Ref.[24],Eq.(15.8.20)):

        the solution of Eq.(39),namely,

        can be written as

        Using the identity(Ref.[24],Eq.(15.8.7)),

        and assuming

        it follows that c=1/2.Finally,the solution(41)now reads

        which reduces,up to a multiplicative constant,to the solution(38)for b1=0, ξ1= ?1 and ξ2=1.

        5 Conclusion

        The classical Generalized and the recent Universal Associated Legendre Equations are members of the more broad class of differential equations given by Eq.(4).We established the hypergeometric solutions of this class of equations and demonstrated that they lead to the Generalized and Universal Associated Legendre hypergeometric solutions.These new solutions open the door for further compelling studies,including the examination of their mathematical properties and the investigation of their applicability to problems in mathematical physics.

        [1]Chen Chang-Yuan,You Yuan,Lu Fa-Lin,et al.,Commun.Theor.Phys.62(2014)331.

        [2]Chang-Yuan Chen,Fa-Line Lu,and Dong-Sheng Sun,Appl.Math.Lett.40(2015)90.

        [3]Chen Chang-Yuan,You Yuan,Lu Fa-Lin,et al.,Commun.Theor.Phys.66(2016)158.

        [4]Chen Chang-Yuan,Lu Fa-Lin,Sun Dong-Sheng,et al.,Ann.Physics:Elsevier 371(2016)183.

        [5]G.Ya?ez-Navarro,Guo-Hua Sun,et al.,Commun.Theor.Phys.68(2017)177.

        [6]G.Ya?ez-Navarro,Guo-Hua Sun,Dong-Sheng Sun,et al.,J.Math.Phys.58(2017)052105.

        [7]Wei Li,Chang-Yuan Chen,and Shi-Hai Dong,Adv.High Energy Phys.2017(2017)1,doi:10.1155/2017/7374256.

        [8]H.Bateman,Partial Differential Equations of Mathematical Physics,Cambridge University Press,Cambridge(1932).

        [9]L.Kuipers and B.Meulenbeld,Proc.Kon.Ned.Ak.V.Wet.Amsterdam 80(1957)436.

        [10]L.Kuipers and B.Meulenbeld,Proc.Kon.Ned.Ak.V.Wet.Amsterdam 80(1957)444.

        [11]L.Kuipers,Math.Scand.6(1958)200.

        [12]L.Kuipers and B.Meulenbeld,Arch.Math.66(1958)394.

        [13]L.Kuipers and B.Meulenbeld,Proc.Konkl.Nederl.Akad.Wet.Ser.A 61(1958)557.

        [14]L.Kuipers and B.Meulenbeld,Proc.Kon.Ned.Akad.Wetensch.;Ser.A 61(1958)330.

        [15]L.Kuipers and B.Meulenbeld,Proc.Kon.Ned.Akad.Wetensch.Ser.A 61(958)186.

        [16]L.Kuipers and B.Meulenbeld,Arch.Math.F 66(1958)394.

        [17]L.Kuipers,Monatsschr.Math.63(1958)24.

        [18]N.A.Virchenko and I.A.Fedotova,J.Math.Sci.69(1994)1395.

        [19]N.A.Virchenko and I.A.Fedotova,Generalized Associated Legendre Dunctions and Their Applications,World Scientific,Singapore(2001).

        [20]L.K.Sharma,Proc.Indian Nat.Sci.Acad.A 36(1970)239.

        [21]I.A.Khan,Indian J.Pure Appl.Math.4(1973)90.

        [22]H.Ciftci,R.L.Hall,N.Saad,and E.Dogu,J.Phys.A:Math.Theor.43(2010)415206.

        [23]Earl A.Coddington and N.Levinson,Theory of Ordinary Differential Equations,McGraw-Hill,New York(1955).

        [24]F.W.J.Olver,A.B.Olde Daalhuis,D.W.Lozier,et al.,NIST Digital Library of Mathematical Functions,http://dlmf.nist.gov/15.8,Release 1.0.17 of 2017-12-22.

        国内永久福利在线视频图片| 天堂av无码大芭蕉伊人av孕妇黑人| 国产成人综合久久精品推荐免费 | 午夜无码片在线观看影院| 娇柔白嫩呻吟人妻尤物| 国产亚洲精品视频网站| 一区二区和激情视频| 国产精品久久久久久久免费看| 视频在线观看一区二区三区| 日本一区二三区在线中文| 久久成人国产精品一区二区| 男女下面进入的视频| 色综合久久精品中文字幕| 亚洲一区二区日韩精品| 亚洲一区二区三区尿失禁| 国产熟女高潮视频| 波多吉野一区二区三区av| 国产三级精品av在线| 少妇内射兰兰久久| 91精品视品在线播放| 国产一区二区毛片视频| 国产一区二区三区毛片| 国产精品沙发午睡系列990531| 久久精品国产6699国产精| 青青草视频视频在线观看| 日韩一区二区三区天堂| 国产极品裸体av在线激情网| 国产黄在线观看免费观看不卡| 国产精品综合久久久久久久免费 | 一区二区三区国产天堂| 性无码一区二区三区在线观看| 人成午夜免费大片| 亚洲性爱区免费视频一区| 日韩一区二区三区精品视频| 国产农村乱辈无码| 国产亚洲女在线线精品| 国产精品髙潮呻吟久久av| 在线精品无码字幕无码av| 毛片网站视频| 国产av大片久久中文字幕| 无套内谢老熟女|