Parabolic cylinder function

Solutions

There are independent even and odd solutions of the form (). These are given by (following the notation of Abramowitz and Stegun (1965)): y_1(a;z) = \exp(-z^2/4) ;_1F_1 \left(\tfrac12a+\tfrac14; ; \tfrac12; ; ; \frac{z^2}{2}\right),,,,,, (\mathrm{even}) and y_2(a;z) = z\exp(-z^2/4) ;_1F_1 \left(\tfrac12a+\tfrac34; ; \tfrac32; ; ; \frac{z^2}{2}\right),,,,,, (\mathrm{odd}) where ;_1F_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. One such pair is based upon their behavior at infinity: U(a,z)=\frac{1}{2^\xi\sqrt{\pi}} \left[ \cos(\xi\pi)\Gamma(1/2-\xi),y_1(a,z) -\sqrt{2}\sin(\xi\pi)\Gamma(1-\xi),y_2(a,z) \right] V(a,z)=\frac{1}{2^\xi\sqrt{\pi}\Gamma[1/2-a]} \left[ \sin(\xi\pi)\Gamma(1/2-\xi),y_1(a,z) +\sqrt{2}\cos(\xi\pi)\Gamma(1-\xi),y_2(a,z) \right] where \xi = \frac{1}{2}a+\frac{1}{4} .

The function U(a, z) approaches zero for large values of z and {{math|arg(z) \lim_{z\to\infty}U(a,z)/\left(e^{-z^2/4}z^{-a-1/2}\right)=1,,,,(\text{for},\left|\arg(z)\right| and \lim_{z\to\infty}V(a,z)/\left(\sqrt{\frac{2}{\pi}}e^{z^2/4}z^{a-1/2}\right)=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 (a notation dating back to Whittaker (1902)) that are themselves sometimes called parabolic cylinder functions: \begin{align} U(a,x) &= D_{-a-\tfrac12}(x), \ V(a,x) &= \frac{\Gamma(\tfrac12+a)}{\pi}[\sin( \pi a) D_{-a-\tfrac12}(x)+D_{-a-\tfrac12}(-x)] . \end{align}

Function was introduced by Whittaker and Watson as a solution of eq.~() with \tilde a=-\frac14, \tilde b=0, \tilde c=a+\frac12 bounded at +\infty. It can be expressed in terms of confluent hypergeometric functions as :D_a(z)=\frac{1}{\sqrt{\pi }}{2^{a/2} e^{-\frac{z^2}{4}} \left(\cos \left(\frac{\pi a}{2}\right) \Gamma \left(\frac{a+1}{2}\right) , _1F_1\left(-\frac{a}{2};\frac{1}{2};\frac{z^2}{2}\right)+\sqrt{2} z \sin \left(\frac{\pi a}{2}\right) \Gamma \left(\frac{a}{2}+1\right) , _1F_1\left(\frac{1}{2}-\frac{a}{2};\frac{3}{2};\frac{z^2}{2}\right)\right)}. Power series for this function have been obtained by Abadir (1993).

Parabolic Cylinder U(a,z) function

Integral representation

Integrals along the real line, U(a,z)=\frac{e^{-\frac14 z^2}}{\Gamma\left(a+\frac12\right)} \int_0^\infty e^{-zt}t^{a-\frac12}e^{-\frac12 t^2}dt ,,; \Re a-\frac12 ;, U(a,z)=\sqrt{\frac2{\pi}}e^{\frac14 z^2} \int_0^\infty \cos\left(zt+\frac{\pi}{2}a+\frac{\pi}{4}\right) t^{-a-\frac12}e^{-\frac12 t^2}dt ,,; \Re a The fact that these integrals are solutions to equation () can be easily checked by direct substitution.

Derivative

Differentiating the integrals with respect to z gives two expressions for U'(a,z), U'(a,z)=-\frac{z}{2}U(a,z)- \frac{e^{-\frac14 z^2}}{\Gamma\left(a+\frac12\right)} \int_0^\infty e^{-zt}t^{a+\frac12}e^{-\frac12 t^2}dt =-\frac{z}{2}U(a,z)-\left(a+\frac12\right)U(a+1,z) ;, U'(a,z)=\frac{z}{2}U(a,z)- \sqrt{\frac2{\pi}}e^{\frac14 z^2} \int_0^\infty \sin\left(zt+\frac{\pi}{2}a+\frac{\pi}{4}\right) t^{-a+\frac12}e^{-\frac12 t^2}dt = \frac{z}{2}U(a,z)-U(a-1,z) ;. Adding the two gives another expression for the derivative, 2U'(a,z) = -\left(a+\frac12\right)U(a+1,z)-U(a-1,z) ;.

Recurrence relation

Subtracting the first two expressions for the derivative gives the recurrence relation, zU(a,z) = U(a-1,z) - \left(a+\frac12\right)U(a+1,z) ;.

Asymptotic expansion

Expanding e^{-\frac12 t^2}=1-\frac12 t^2+\frac18 t^4 - \dots ; in the integrand of the integral representation gives the asymptotic expansion of U(a,z), U(a,z) = e^{-\frac14 z^2}z^{-a-\frac12}\left(1

• \frac{(a+\frac12)(a+\frac32)}{2}\frac{1}{z^2}

• \frac{(a+\frac12)(a+\frac32)(a+\frac52)(a+\frac72)}{8}\frac{1}{z^4}

• \dots\right) .

Power series

Expanding the integral representation in powers of z gives U(a,z)=\frac{\sqrt{\pi},2^{-\frac{a}{2}-\frac14}}{\Gamma\left(\frac{a}{2}+\frac34\right)} -\frac{\sqrt{\pi},2^{-\frac{a}{2}+\frac14}}{\Gamma\left(\frac{a}{2}+\frac14\right)}z +\frac{\sqrt{\pi},2^{-\frac{a}{2}-\frac54}}{\Gamma\left(\frac{a}{2}+\frac34\right)}z^2 - \dots ;.

Values at z=0

From the power series one immediately gets U(a,0)=\frac{\sqrt{\pi},2^{-\frac{a}{2}-\frac14}}{\Gamma\left(\frac{a}{2}+\frac34\right)} ;, U'(a,0)=-\frac{\sqrt{\pi},2^{-\frac{a}{2}+\frac14}}{\Gamma\left(\frac{a}{2}+\frac14\right)} ;.

Parabolic cylinder D_ν(z) function

Parabolic cylinder function D_\nu(z) is the solution to the Weber differential equation, u''+\left(\nu+\frac12-\frac{1}{4} z^2 \right)u=0 ,, that is regular at \Re z\to +\infty with the asymptotics D_\nu(z) \to e^{-\frac14 z^2}z^\nu ,. It is thus given as D_\nu(z)=U(-\nu-1/2,z) and its properties then directly follow from those of the U-function.

Integral representation

D_\nu(z)=\frac{e^{-\frac14 z^2}}{\Gamma(-\nu)} \int_0^\infty e^{-zt} t^{-\nu -1} e^{-\frac12 t^2}dt ,,; \Re \nu 0;, D_\nu(z)=\sqrt{\frac2{\pi}}e^{\frac14 z^2} \int_0^\infty \cos\left(zt-\nu \frac{\pi}{2}\right) t^{\nu}e^{-\frac12 t^2}dt ,,; \Re \nu -1 ;.

Asymptotic expansion

D_\nu(z) = e^{-\frac14 z^2}z^{\nu}\left(1

• \frac{\nu (\nu -1)}{2}\frac{1}{z^2}

• \frac{\nu (\nu -1)(\nu -2)(\nu -3)}{8}\frac{1}{z^4}

• \dots\right),,; \Re z \to +\infty . If \nu is a non-negative integer this series terminates and turns into a polynomial, namely the Hermite polynomial, D_n(z) = e^{-\frac14 z^2};2^{-n/2}H_n\left(\frac{z}{\sqrt{2}}\right),, n=0,1,2,\dots ;.

Connection with quantum harmonic oscillator

Parabolic cylinder D_\nu(z) function appears naturally in the Schrödinger equation for the one-dimensional quantum harmonic oscillator (a quantum particle in the oscillator potential), \left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+\frac12 m \omega^2 x^2 \right]\psi(x) =E\psi(x) ;, where \hbar is the reduced Planck constant, m is the mass of the particle, x is the coordinate of the particle, \omega is the frequency of the oscillator, E is the energy, and \psi(x) is the particle's wave-function. Indeed introducing the new quantities z=\frac{x}{b_o} ,,; \nu=\frac{E}{\hbar\omega}-\frac12 ,,; b_o=\sqrt{\frac{\hbar}{2m\omega}} ,, turns the above equation into the Weber's equation for the function u(z)=\psi(zb_o), u''+\left(\nu+\frac12-\frac{1}{4} z^2 \right)u=0 ,.

References

NIST Digital Library of Mathematical Functions. https://dlmf.nist.gov/, Release 1.2.2 of 2024-09-15. F. W. J. Olver, A. B. Olde Daalhuis, D. W. Lozier, B. I. Schneider, R. F. Boisvert, C. W. Clark, B. R. Miller, B. V. Saunders, H. S. Cohl, and M. A. McClain, eds.

References

1. Abadir, K. M. (1993) "Expansions for some confluent hypergeometric functions." ''Journal of Physics A'', 26, 4059-4066.
2. {{AS ref. 19. 686
3. Rozov, N.Kh.. "Weber equation".
4. {{dlmf. N. M.. Temme
5. Weber, H.F.. (1869). "Ueber die Integration der partiellen Differentialgleichung \partial^2u/\partial x^2+\partial^2u/\partial y^2+k^2u=0". Math. Ann..
6. Whittaker, E.T. (1902) "On the functions associated with the parabolic cylinder in harmonic analysis" ''Proc. London Math. Soc.'', 35, 417–427.
7. Whittaker, E. T. and Watson, G. N. (1990) "The Parabolic Cylinder Function." §16.5 in A Course in Modern Analysis, 4th ed. Cambridge, England: Cambridge University Press, pp. 347-348.