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Neumann polynomial : ウィキペディア英語版
Neumann polynomial
In mathematics, a Neumann polynomial, introduced by Carl Neumann for the special case \alpha=0, is a polynomial in 1/''z'' used to expand functions in term of Bessel functions.〔Abramowitz and Stegun, (p. 363, 9.1.82 ) ff.〕
The first few polynomials are
:O_0^(t)=\frac 1 t,
:O_1^(t)=2\frac ,
:O_2^(t)=\frac + 4\frac ,
:O_3^(t)=2\frac + 8\frac ,
:O_4^(t)=\frac + 4\frac + 16\frac .
A general form for the polynomial is
:O_n^(t)= \frac \sum_^ (-1)^\frac \left(\frac 2 t \right)^,
they have the generating function
:\frac \frac 1 = \sum_O_n^(t) J_(z),
where ''J'' are Bessel functions.
To expand a function ''f'' in form
:f(z)=\sum_ a_n J_(z)\,
for |z|
compute
:a_n=\frac 1 \oint_ \fracf(z) O_n^(z)\mathrm d z,
where c' and ''c'' is the distance of the nearest singularity of z^ f(z) from z=0.
==Examples==
An example is the extension
:\left(\tfracz\right)^s= \Gamma(s)\cdot\sum_(-1)^k J_(z)(s+2k)
or the more general Sonine formula〔 II.7.10.1, p.64〕
:e^= \Gamma(s)\cdot\sum_i^k C_k^(\gamma)(s+k)\frac.
where C_k^ is Gegenbauer's polynomial. Then,
:\fracJ_s(z)= \sum_(-1)^(s+2i)J_(z),
:\sum_ t^n J_(z)= \frac} \sum_\frac\right)^j}\frac\right)}= \int_0^\infty e^}\frac \frac\,dx,
the confluent hypergeometric function
:M(a,s,z)= \Gamma (s) \sum_^\infty \left(-\frac\right)^k L_k^(t) \frac\right)}}
and in particular
:\frac= \frace^\sum_L_k^\left(\frac4\right)(4 i z)^k \frac\right)}},
the index shift formula
:\Gamma(\nu-\mu) J_\nu(z)= \Gamma(\mu+1) \sum_\frac \left(\frac z 2\right)^J_(z),
the Taylor expansion (addition formula)
:\frac}= \sum_\frac\frac J_(z)
are of the same type.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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