Neumann polynomial
In mathematics, the Neumann polynomials , introduced by Carl Neumann for the special case α = 0 , are a sequence of polynomials in 1 / t used to expand functions in term of Bessel functions .
The first few polynomials are
O 0 ( α ) ( t ) = 1 t ,
O 1 ( α ) ( t ) = 2 α + 1 t 2 ,
O 2 ( α ) ( t ) = 2 + α t + 4 ( 2 + α ) ( 1 + α ) t 3 ,
O 3 ( α ) ( t ) = 2 ( 1 + α ) ( 3 + α ) t 2 + 8 ( 1 + α ) ( 2 + α ) ( 3 + α ) t 4 ,
O 4 ( α ) ( t ) = ( 1 + α ) ( 4 + α ) 2 t + 4 ( 1 + α ) ( 2 + α ) ( 4 + α ) t 3 + 16 ( 1 + α ) ( 2 + α ) ( 3 + α ) ( 4 + α ) t 5 .
A general form for the polynomial is
O n ( α ) ( t ) = α + n 2 α ∑ k = 0 ⌊ n / 2 ⌋ ( − 1 ) n − k ( n − k ) ! k ! ( − α n − k ) ( 2 t ) n + 1 − 2 k ,
and they have the "generating function"
( z 2 ) α Γ ( α + 1 ) 1 t − z = ∑ n = 0 O n ( α ) ( t ) J α + n ( z ) ,
where J are Bessel functions .
To expand a function f in the form
f ( z ) = ( 2 z ) α ∑ n = 0 a n J α + n ( z )
for | t | < c , compute
a n = Γ ( α + 1 ) 2 π i ∮ | t | = c ′ f ( t ) O n ( α ) ( t ) d t ,
where c ′ < c and c is the distance of the nearest singularity of f(z) from z = 0 .
Examples
An example is the extension
( 1 2 z ) s = Γ ( s ) ⋅ ∑ k = 0 ( − 1 ) k J s + 2 k ( z ) ( s + 2 k ) ( − s k ) ,
or the more general Sonine formula
e i γ z = Γ ( s ) ⋅ ∑ k = 0 i k C k ( s ) ( γ ) ( s + k ) J s + k ( z ) ( z 2 ) s .
where C k ( s ) is Gegenbauer's polynomial . Then,[ citation needed ] [ original research? ]
( z 2 ) 2 k ( 2 k − 1 ) ! J s ( z ) = ∑ i = k ( − 1 ) i − k ( i + k − 1 2 k − 1 ) ( i + k + s − 1 2 k − 1 ) ( s + 2 i ) J s + 2 i ( z ) ,
∑ n = 0 t n J s + n ( z ) = e t z 2 t s ∑ j = 0 ( − z 2 t ) j j ! γ ( j + s , t z 2 ) Γ ( j + s ) = ∫ 0 ∞ e − z x 2 2 t z x t J s ( z 1 − x 2 ) 1 − x 2 s d x ,
the confluent hypergeometric function
M ( a , s , z ) = Γ ( s ) ∑ k = 0 ∞ ( − 1 t ) k L k ( − a − k ) ( t ) J s + k − 1 ( 2 t z ) ( t z ) s − k − 1 ,
and in particular
J s ( 2 z ) z s = 4 s Γ ( s + 1 2 ) π e 2 i z ∑ k = 0 L k ( − s − 1 / 2 − k ) ( i t 4 ) ( 4 i z ) k J 2 s + k ( 2 t z ) t z 2 s + k ,
the index shift formula
Γ ( ν − μ ) J ν ( z ) = Γ ( μ + 1 ) ∑ n = 0 Γ ( ν − μ + n ) n ! Γ ( ν + n + 1 ) ( z 2 ) ν − μ + n J μ + n ( z ) ,
the Taylor expansion (addition formula)
J s ( z 2 − 2 u z ) ( z 2 − 2 u z ) ± s = ∑ k = 0 ( ± u ) k k ! J s ± k ( z ) z ± s ,
(cf.[ failed verification ] ) and the expansion of the integral of the Bessel function,
∫ J s ( z ) d z = 2 ∑ k = 0 J s + 2 k + 1 ( z ) ,
are of the same type.
Notes
↑ Abramowitz and Stegun , p. 363, 9.1.82 ff.
↑ Erdélyi, Arthur; Magnus, Wilhelm; Oberhettinger, Fritz; Tricomi, Francesco G. (1955), Higher Transcendental Functions. Vols. I, II, III , McGraw-Hill, MR 0058756 II.7.10.1, p.64
↑ Gradshteyn, Izrail Solomonovich ; Ryzhik, Iosif Moiseevich ; Geronimus, Yuri Veniaminovich ; Tseytlin, Michail Yulyevich ; Jeffrey, Alan (2015) [October 2014]. "8.515.1.". In Zwillinger, Daniel; Moll, Victor Hugo (eds.). Table of Integrals, Series, and Products . Translated by Scripta Technica, Inc. (8 ed.). Academic Press, Inc. p. 944. ISBN 0-12-384933-0 . LCCN 2014010276 .