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Coordinate surfaces of parabolic cylindrical coordinates. Parabolic cylinder functions occur when separation of variables is used on Laplace's equation in these coordinates

In mathematics, the parabolic cylinder functions are special functions defined as solutions to the differential equation

$\frac{d^{2}f}{d{z}^2}+(\tilde{a}{z}^2+\tilde{b}z+\tilde{c})f=0.$

This equation is found when the technique of separation of variables is used on Laplace's equation when expressed in parabolic cylindrical coordinates.

The above equation may be brought into two distinct forms (A) and (B) by completing the square and rescaling z, called H. F. Weber's equations Template:Harv:

$\frac{d^{2}f}{d{z}^2}-(\frac{1}{4}{z}^2+a)f=0$    (A)

and

$\frac{d^{2}f}{d{z}^2}+(\frac{1}{4}{z}^2-a)f=0.$     (B)

If

$f(a,z)$

is a solution, then so are

$f(a,-z),f(-a,iz)\text{ and }f(-a,-iz).$

If

$f(a,z)$

is a solution of equation (A), then

$f(-ia,z{e}^{(1/4)\pi i})$

is a solution of (B), and, by symmetry,

$f(-ia,-z{e}^{(1/4)\pi i}),f(ia,-z{e}^{-(1/4)\pi i})\text{ and }f(ia,z{e}^{-(1/4)\pi i})$

are also solutions of (B).

Solutions

There are independent even and odd solutions of the form (A). These are given by (following the notation of Abramowitz and Stegun (1965)):

$y_1(a;z)=\exp (-z^2/4){}_1{F}_1(\frac{1}{2}a+\frac{1}{4};\frac{1}{2};\frac{z^2}{2})(\mathrm{e}\mathrm{v}\mathrm{e}\mathrm{n})$

and

$y_2(a;z)=z\exp (-z^2/4){}_1{F}_1(\frac{1}{2}a+\frac{3}{4};\frac{3}{2};\frac{z^2}{2})(\mathrm{o}\mathrm{d}\mathrm{d})$

where ${}_1{F}_1(a;b;z)=M(a;b;z)$ is the confluent hypergeometric function.

Other pairs of independent solutions may be formed from linear combinations of the above solutions (see Abramowitz and Stegun). One such pair is based upon their behavior at infinity:

$U(a,z)=\frac{1}{2^{\xi }\sqrt{\pi }}[\cos (\xi \pi )\Gamma (1/2-\xi )y_1(a,z)-\sqrt{2}\sin (\xi \pi )\Gamma (1-\xi )y_2(a,z)]$

$V(a,z)=\frac{1}{2^{\xi }\sqrt{\pi }\Gamma [1/2-a]}[\sin (\xi \pi )\Gamma (1/2-\xi )y_1(a,z)+\sqrt{2}\cos (\xi \pi )\Gamma (1-\xi )y_2(a,z)]$

where

$\xi =\frac{1}{2}a+\frac{1}{4}.$

The function U(a, z) approaches zero for large values of |z|  and |arg(z)| < π/2, while V(a, z) diverges for large values of positive real z .

$\underset{|z|\to \mathrm{\infty }}{lim}U(a,z)/e^{-z^2/4}{z}^{-a-1/2}=1(\text{for}|\arg (z)|<\pi /2)$

and

$\underset{|z|\to \mathrm{\infty }}{lim}V(a,z)/\sqrt{\frac{2}{\pi }}{e}^{z^2/4}{z}^{a-1/2}=1(\text{for}\arg (z)=0).$

For half-integer values of a, these (that is, U and V) can be re-expressed in terms of Hermite polynomials; alternatively, they can also be expressed in terms of Bessel functions.

The functions U and V can also be related to the functions D_p(x) (a notation dating back to Whittaker (1902)) that are themselves sometimes called parabolic cylinder functions (see Abramowitz and Stegun (1965)):

$U(a,x)=D_{-a-\frac{1}{2}}(x),$

$V(a,x)=\frac{\Gamma (\frac{1}{2}+a)}{\pi }[\sin (\pi a)D_{-a-\frac{1}{2}}(x)+D_{-a-\frac{1}{2}}(-x)].$

References

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• Weber, H.F. (1869) "Ueber die Integration der partiellen Differentialgleichung ${\partial }^{2}u/\partial x^2+{\partial }^{2}u/\partial y^2+k^{2}u=0$". Math. Ann., 1, 1–36
• Whittaker, E.T. (1902) "On the functions associated with the parabolic cylinder in harmonic analysis" Proc. London Math. Soc.35, 417–427.