10.15 Derivatives with Respect to Order10.17 Asymptotic Expansions for Large Argument

§10.16 Relations to Other Functions

Airy Functions

See §§9.6(i) and 9.6(ii).

Parabolic Cylinder Functions

With the notation of §12.14(i),

10.16.3
\mathop{J_{{\frac{1}{4}}}\/}\nolimits\!\left(z\right)=-2^{{-\frac{1}{4}}}\pi^{{-\frac{1}{2}}}z^{{-\frac{1}{4}}}\left(\mathop{W\/}\nolimits\!\left(0,2z^{{\frac{1}{2}}}\right)-\mathop{W\/}\nolimits\!\left(0,-2z^{{\frac{1}{2}}}\right)\right),
\mathop{J_{{-\frac{1}{4}}}\/}\nolimits\!\left(z\right)=2^{{-\frac{1}{4}}}\pi^{{-\frac{1}{2}}}z^{{-\frac{1}{4}}}\left(\mathop{W\/}\nolimits\!\left(0,2z^{{\frac{1}{2}}}\right)+\mathop{W\/}\nolimits\!\left(0,-2z^{{\frac{1}{2}}}\right)\right).
10.16.4
\mathop{J_{{\frac{3}{4}}}\/}\nolimits\!\left(z\right)=-2^{{-\frac{1}{4}}}\pi^{{-\frac{1}{2}}}z^{{-\frac{3}{4}}}\left({\mathop{W\/}\nolimits^{{\prime}}}\!\left(0,2z^{{\frac{1}{2}}}\right)-{\mathop{W\/}\nolimits^{{\prime}}}\!\left(0,-2z^{{\frac{1}{2}}}\right)\right),
\mathop{J_{{-\frac{3}{4}}}\/}\nolimits\!\left(z\right)=-2^{{-\frac{1}{4}}}\pi^{{-\frac{1}{2}}}z^{{-\frac{3}{4}}}\left({\mathop{W\/}\nolimits^{{\prime}}}\!\left(0,2z^{{\frac{1}{2}}}\right)+{\mathop{W\/}\nolimits^{{\prime}}}\!\left(0,-2z^{{\frac{1}{2}}}\right)\right).

Principal values on each side of these equations correspond.

Confluent Hypergeometric Functions

In all cases principal branches correspond at least when |\mathop{\mathrm{ph}\/}\nolimits z|\leq\tfrac{1}{2}\pi.

Generalized Hypergeometric Functions

With \mathop{\mathbf{F}\/}\nolimits{}{} as in §15.2(i), and with z and \nu fixed,

10.16.10 \mathop{J_{{\nu}}\/}\nolimits\!\left(z\right)=(\tfrac{1}{2}z)^{\nu}\lim\mathop{{{\mathbf{F}}}\/}\nolimits\!\left(\lambda,\mu;\nu+1;-z^{2}/(4\lambda\mu)\right),

as \lambda and \mu\to\infty in \Complex. For this result see Watson (1944, §5.7).