10 Bessel FunctionsSpherical Bessel Functions

§10.54 Integral Representations

10.54.1 𝗃n⁡(z)=zn2n+1⁢n!⁢∫0πcos⁡(z⁢cos⁡θ)⁢(sin⁡θ)2⁢n+1⁢dθ.
10.54.2 𝗃n⁡(z) =(−i)n2⁢∫0πei⁢z⁢cos⁡θ⁢Pn⁡(cos⁡θ)⁢sin⁡θ⁢dθ.
10.54.3 𝗄n⁡(z) =π2⁢∫1∞e−z⁢t⁢Pn⁡(t)⁢dt,
|ph⁡z|<12⁢π.
10.54.4 𝗃n⁡(z) =(−i)n+12⁢π⁢∫i⁢∞(−1+,1+)ei⁢z⁢t⁢Qn⁡(t)⁢dt,
|ph⁡z|<12⁢π.

For the Legendre polynomial Pn and the associated Legendre function Qn see §§18.3 and 14.21(i), with μ=0 and ν=n.

Additional integral representations can be obtained by combining the definitions (10.47.3)–(10.47.9) with the results given in §10.9 and §10.32.