Digital Library of Mathematical Functions
About the Project
NIST
10 Bessel FunctionsKelvin Functions

§10.61 Definitions and Basic Properties

Contents

§10.61(i) Definitions

Throughout §§10.61–§10.71 it is assumed that x\geq 0, \nu\in\Real, and n is a nonnegative integer.

10.61.1\mathop{\mathrm{ber}_{{\nu}}\/}\nolimits x+i\mathop{\mathrm{bei}_{{\nu}}\/}%
\nolimits x=\mathop{J_{{\nu}}\/}\nolimits\!\left(xe^{{3\pi i/4}}\right)=e^{{%
\nu\pi i}}\mathop{J_{{\nu}}\/}\nolimits\!\left(xe^{{-\pi i/4}}\right)=e^{{\nu%
\pi i/2}}\mathop{I_{{\nu}}\/}\nolimits\!\left(xe^{{\pi i/4}}\right)=e^{{3\nu%
\pi i/2}}\mathop{I_{{\nu}}\/}\nolimits\!\left(xe^{{-3\pi i/4}}\right),

When \nu=0 suffices on \mathop{\mathrm{ber}\/}\nolimits, \mathop{\mathrm{bei}\/}\nolimits, \mathop{\mathrm{ker}\/}\nolimits, and \mathop{\mathrm{kei}\/}\nolimits are usually suppressed.

Most properties of \mathop{\mathrm{ber}_{{\nu}}\/}\nolimits x, \mathop{\mathrm{bei}_{{\nu}}\/}\nolimits x, \mathop{\mathrm{ker}_{{\nu}}\/}\nolimits x, and \mathop{\mathrm{kei}_{{\nu}}\/}\nolimits x follow straightforwardly from the above definitions and results given in preceding sections of this chapter.

§10.61(ii) Differential Equations

§10.61(iii) Reflection Formulas for Arguments

In general, Kelvin functions have a branch point at x=0 and functions with arguments xe^{{\pm\pi i}} are complex. The branch point is absent, however, in the case of \mathop{\mathrm{ber}_{{\nu}}\/}\nolimits and \mathop{\mathrm{bei}_{{\nu}}\/}\nolimits when \nu is an integer. In particular,

10.61.5
\mathop{\mathrm{ber}_{{n}}\/}\nolimits\!\left(-x\right)=(-1)^{n}\mathop{%
\mathrm{ber}_{{n}}\/}\nolimits x,
\mathop{\mathrm{bei}_{{n}}\/}\nolimits\!\left(-x\right)=(-1)^{n}\mathop{%
\mathrm{bei}_{{n}}\/}\nolimits x.

§10.61(iv) Reflection Formulas for Orders

§10.61(v) Orders \pm\frac{1}{2}