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39 Functional Equations<br />

Final: 2013/2/7<br />

5 Katsuyuki Nishimoto<br />

∗ Solutions to <strong>the</strong> homogeneous Bessel equation by means <strong>of</strong> N-fractional<br />

(Descartes Press Co.) calculus operator · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · 15<br />

Summary: In this article, <strong>the</strong> solutions to <strong>the</strong> homogeneous Bessel equation are discussed by<br />

means <strong>of</strong> <strong>the</strong> N-fractional calculus operator (NFCO). That is, we have <strong>the</strong> particular solutions as<br />

follows, for example.<br />

φ [1] = z ν e iz (e −i2z · z −(ν+1/2) ) ν−1/2 (fractional differintegrated form)<br />

= (−i2) ν−1/2z −1/2e−iz 2F0( 1<br />

<br />

2<br />

<br />

( i<br />

<br />

<br />

< 1)<br />

2z<br />

= A · H (2)<br />

ν (z), (A = √ π2 ν−1 e −iπν )<br />

<strong>and</strong><br />

1 i<br />

− ν, 2 + ν; 2z )<br />

φ [6] = z −ν e iz (z ν−1/2 · e −i2z ) −(ν+1/2) (fractional differintegrated form)<br />

= eiπ(ν+1/2) Γ(−2ν)zν e−iz 1F1( 1<br />

( )<br />

2 + ν; 1 + 2ν; 2iz) (|2iz| < 1)<br />

Γ(−2ν−k) <br />

< ∞<br />

Γ(−ν+1/2)<br />

= B ∗ · J (2)<br />

ν (z), (B ∗ = 2 ν Γ(−2ν)Γ(1 + ν)e iπ(ν+1/2) )<br />

where pFq(· · · · · · ) is <strong>the</strong> generalized Gauss hypergeometric function, H (2)<br />

ν (z) is <strong>the</strong> Hankel function,<br />

<strong>and</strong><br />

J (2)<br />

ν (z) = e−iz (z/2) ν<br />

1<br />

Γ(1+ν) 1F1( 2 + ν; 1 + 2ν; 2iz) = Jν(z) (|2iz| < 1)<br />

is <strong>the</strong> first kind Bessel Function.<br />

6 Katsuyuki Nishimoto<br />

∗ The solutions to <strong>the</strong> radial Schrödinger equation <strong>of</strong> <strong>the</strong> hydrogen atom<br />

(Descartes Press Co.) by means <strong>of</strong> N-fractional calculus operator · · · · · · · · · · · · · · · · · · · · · · · · 15<br />

Summary: In this article, <strong>the</strong> solutions to <strong>the</strong> radial Schrödinger equation <strong>of</strong> <strong>the</strong> Hydrogen atom<br />

(in <strong>the</strong> Coulomb field)<br />

φ2 · x 2 + φ1 · 2x + φ · {−(1/4)x 2 + νx + l(l + 1)} = 0<br />

are discussed by means <strong>of</strong> N-fractional calculus operator.<br />

A particular solution to <strong>the</strong> equation above is shown as follows for example.<br />

φ = φ [1] = x l e x/2 (e −x · x ν−(l+1) )l+ν (fractional differintegrated form)<br />

= (e iπ ) l+ν e −x/2 x ν−1 2F0(−l − ν, l + 1 − ν; −1/x)<br />

(| − 1/x| < 1)<br />

where pFq(· · · · · · ); Generalized Gauss hypergeometric functions.<br />

7 Ryu Sasaki (Kyoto Univ.) ♯ Global solutions <strong>of</strong> certain second order differential equations with a<br />

Kouichi Takemura (Chuo Univ.) high degree <strong>of</strong> apparent singularity · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · 10<br />

Summary: Infinitely many explicit solutions <strong>of</strong> certain second order differential equations with an<br />

apparent singularity <strong>of</strong> characteristic exponent −2 are constructed by adjusting <strong>the</strong> parameter <strong>of</strong><br />

<strong>the</strong> multi-indexed Laguerre polynomials.<br />

8 Nobuki Takayama<br />

(Kobe Univ./JST CREST)<br />

♯ Pfaffian systems <strong>of</strong> A-hypergeometric sysytems · · · · · · · · · · · · · · · · · · · · 15<br />

Takayuki Hibi<br />

(Osaka Univ./JST CREST)<br />

Kenta Nishiyama<br />

(Osaka Univ./JST CREST)<br />

Summary: We are interested in bases <strong>of</strong> Rn/(RnHA[s]) as <strong>the</strong> vector space over <strong>the</strong> field C(s, x)<br />

where HA[s] is an A-hypergeometric ideal. Any basis <strong>of</strong> <strong>the</strong> vector space yields an associated<br />

Pfaffian system or an integrable connection associated to HA[s]. Bases can be described by those<br />

<strong>of</strong> simpler quotients Rn/(inw(IA) + ∑ Rn(Ei − si)).

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