[go: up one dir, main page]

29 Lamé FunctionsLamé Functions

§29.5 Special Cases and Limiting Forms

29.5.2 𝐸𝑐ν0⁡(z,0)=2−12,
29.5.3 𝐸𝑐νm⁡(z,0) =cos⁡(m⁢(12⁢π−z)),
m≥1,
𝐸𝑠νm⁡(z,0) =sin⁡(m⁢(12⁢π−z)),
m≥1.

Let μ=max⁡(ν−m,0). Then

29.5.4 limk→1−aνm⁡(k2)=limk→1−bνm+1⁡(k2)=ν⁢(ν+1)−μ2,
29.5.5 limk→1−𝐸𝑐νm⁡(z,k2)𝐸𝑐νm⁡(0,k2)=limk→1−𝐸𝑠νm+1⁡(z,k2)𝐸𝑠νm+1⁡(0,k2)=1(cosh⁡z)μ⁢F⁡(12⁢μ−12⁢ν,12⁢μ+12⁢ν+1212;tanh2⁡z),
m even,
29.5.6 limk→1−𝐸𝑐νm⁡(z,k2)d𝐸𝑐νm⁡(z,k2)/dz|z=0=limk→1−𝐸𝑠νm+1⁡(z,k2)d𝐸𝑠νm+1⁡(z,k2)/dz|z=0=tanh⁡z(cosh⁡z)μ⁢F⁡(12⁢μ−12⁢ν+12,12⁢μ+12⁢ν+132;tanh2⁡z),
m odd,

where F is the hypergeometric function; see §15.2(i).

If k→0+ and ν→∞ in such a way that k2⁢ν⁢(ν+1)=4⁢θ (a positive constant), then

where cem⁡(z,θ) and sem⁡(z,θ) are Mathieu functions; see §28.2(vi).