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10 Bessel FunctionsBessel and Hankel Functions

§10.18 Modulus and Phase Functions

Contents
  1. §10.18(i) Definitions
  2. §10.18(ii) Basic Properties
  3. §10.18(iii) Asymptotic Expansions for Large Argument

§10.18(i) Definitions

For ν≥0 and x>0

10.18.1 Mν⁡(x)⁢ei⁢θν⁡(x) =Hν(1)⁡(x),
10.18.2 Nν⁡(x)⁢ei⁢ϕν⁡(x) =Hν(1)′⁡(x),

where Mν⁡(x) (>0), Nν⁡(x) (>0), θν⁡(x), and ϕν⁡(x) are continuous real functions of ν and x, with the branches of θν⁡(x) and ϕν⁡(x) fixed by

10.18.3 θν⁡(x) →−12⁢π,
ϕν⁡(x) →12⁢π,
x→0+.

§10.18(ii) Basic Properties

10.18.6 Mν⁡(x) =(Jν2⁡(x)+Yν2⁡(x))12,
Nν⁡(x) =(Jν′2⁡(x)+Yν′2⁡(x))12,
10.18.7 θν⁡(x) =Arctan⁡(Yν⁡(x)/Jν⁡(x)),
ϕν⁡(x) =Arctan⁡(Yν′⁡(x)/Jν′⁡(x)).
10.18.9 Nν2⁡(x)=Mν′2⁡(x)+Mν2⁡(x)⁢θν′2⁡(x)=Mν′2⁡(x)+4(π⁢x⁢Mν⁡(x))2,
10.18.10 (x2−ν2)⁢Mν⁡(x)⁢Mν′⁡(x)+x2⁢Nν⁡(x)⁢Nν′⁡(x)+x⁢Nν2⁡(x)=0.
10.18.11 tan⁡(ϕν⁡(x)−θν⁡(x))=Mν⁡(x)⁢θν′⁡(x)Mν′⁡(x)=2π⁢x⁢Mν⁡(x)⁢Mν′⁡(x),
10.18.13 x2⁢Mν′′⁡(x)+x⁢Mν′⁡(x)+(x2−ν2)⁢Mν⁡(x)=4π2⁢Mν3⁢(x),
10.18.14 w′′+(1+14−ν2x2)⁢w=4π2⁢w3,
w=x12⁢Mν⁡(x),
10.18.15 x3⁢w′′′+x⁢(4⁢x2+1−4⁢ν2)⁢w′+(4⁢ν2−1)⁢w=0,
w=x⁢Mν2⁡(x).
10.18.16 θν′2⁡(x)+12⁢θν′′′⁡(x)θν′⁡(x)−34⁢(θν′′⁡(x)θν′⁡(x))2=1−ν2−14x2.

§10.18(iii) Asymptotic Expansions for Large Argument

As x→∞, with ν fixed and μ=4⁢ν2,

10.18.17 Mν2⁡(x) ∼2π⁢x⁢(1+12⁢μ−1(2⁢x)2+1⋅32⋅4⁢(μ−1)⁢(μ−9)(2⁢x)4+1⋅3⋅52⋅4⋅6⁢(μ−1)⁢(μ−9)⁢(μ−25)(2⁢x)6+⋯),
10.18.18 θν⁡(x) ∼x−(12⁢ν+14)⁢π+μ−12⁢(4⁢x)+(μ−1)⁢(μ−25)6⁢(4⁢x)3+(μ−1)⁢(μ2−114⁢μ+1073)5⁢(4⁢x)5+(μ−1)⁢(5⁢μ3−1535⁢μ2+54703⁢μ−3 75733)14⁢(4⁢x)7+⋯.

Also,

10.18.19 Nν2⁡(x)∼2π⁢x⁢(1−12⁢μ−3(2⁢x)2−12⋅4⁢(μ−1)⁢(μ−45)(2⁢x)4−⋯),

the general term in this expansion being

10.18.20 −(2⁢k−3)!!(2⁢k)!!⁢(μ−1)⁢(μ−9)⁢⋯⁢(μ−(2⁢k−3)2)⁢(μ−(2⁢k+1)⁢(2⁢k−1)2)(2⁢x)2⁢k,
k≥2,

and

10.18.21 ϕν⁡(x)∼x−(12⁢ν−14)⁢π+μ+32⁢(4⁢x)+μ2+46⁢μ−636⁢(4⁢x)3+μ3+185⁢μ2−2053⁢μ+18995⁢(4⁢x)5+⋯.

In (10.18.17) and (10.18.18) the remainder after n terms does not exceed the (n+1)th term in absolute value and is of the same sign, provided that n>ν−12 for (10.18.17) and −32≤ν≤32 for (10.18.18).