10 Bessel FunctionsBessel and Hankel Functions

§10.13 Other Differential Equations

In the following equations ν,λ,p,q, and r are real or complex constants with λ≠0, p≠0, and q≠0.

10.13.1 w′′+(λ2−ν2−14z2)⁢w=0,
w=z12⁢𝒞ν⁡(λ⁢z),
10.13.2 w′′+(λ24⁢z−ν2−14⁢z2)⁢w=0,
w=z12⁢𝒞ν⁡(λ⁢z12),
10.13.3 w′′+λ2⁢zp−2⁢w=0,
w=z12⁢𝒞1/p⁡(2⁢λ⁢z12⁢p/p),
10.13.4 w′′+1∓2⁢νz⁢w′+λ2⁢w=0,
w=z±ν⁢𝒞ν⁡(λ⁢z),
10.13.5 z2⁢w′′+(1−2⁢r)⁢z⁢w′+(λ2⁢q2⁢z2⁢q+r2−ν2⁢q2)⁢w=0,
w=zr⁢𝒞ν⁡(λ⁢zq),
10.13.6 w′′+(λ2⁢e2⁢z−ν2)⁢w=0,
w=𝒞ν⁡(λ⁢ez),
10.13.7 z2⁢(z2−ν2)⁢w′′+z⁢(z2−3⁢ν2)⁢w′+((z2−ν2)2−(z2+ν2))⁢w=0,
w=𝒞ν′⁡(z),
10.13.8 w(2⁢n)=(−1)n⁢λ2⁢n⁢z−n⁢w,
w=z12⁢n⁢𝒞n⁡(2⁢λ⁢ek⁢π⁢i/n⁢z12), k=0,1,…,2⁢n−1.

In (10.13.9)–(10.13.11) 𝒞ν⁡(z), 𝒟μ⁡(z) are any cylinder functions of orders ν,μ, respectively, and ϑ=z⁢(d/dz).

10.13.9 z2⁢w′′′+3⁢z⁢w′′+(4⁢z2+1−4⁢ν2)⁢w′+4⁢z⁢w=0,
w=𝒞ν⁡(z)⁢𝒟ν⁡(z),
10.13.10 z3⁢w′′′+z⁢(4⁢z2+1−4⁢ν2)⁢w′+(4⁢ν2−1)⁢w=0,
w=z⁢𝒞ν⁡(z)⁢𝒟ν⁡(z),
10.13.11 (ϑ4−2⁢(ν2+μ2)⁢ϑ2+(ν2−μ2)2)⁢w+4⁢z2⁢(ϑ+1)⁢(ϑ+2)⁢w=0,
w=𝒞ν⁡(z)⁢𝒟μ⁡(z).

For further differential equations see Kamke (1977, pp. 440–451). See also Watson (1944, pp. 95–100).