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Modified Bessel Equation and Modified Bessel Function 📂Functions

Modified Bessel Equation and Modified Bessel Function

Buildup

The differential equation below is referred to as the modified Bessel equation.

x2y+xy(x2ν2)y=0 x^2 y^{\prime \prime} + xy^{\prime}-(x^2-\nu^2)y=0

It is a form of the Bessel equation where the sign of the term yy has been changed to ++ \rightarrow -. The solution to this differential equation is given by the formula for differential equations that have Bessel equation solutions, as follows.

y=Zν(ix)=AJν(ix)+BNν(ix) y=Z_{\nu}(ix)=AJ_{\nu}(ix)+BN_{\nu}(ix)

The two commonly used forms of the solution are referred to as modified Bessel functions. In particular, IνI_{\nu} is called the modified Bessel function of the first kind, and KνK_{\nu} is called the modified Bessel function of the second kind.

Definition

The modified Bessel function of the first kind IνI_{\nu} and the modified Bessel function of the second kind KνK_{\nu} are defined as follows.

Iν(x)=iνJν(ix)Kν(x)=π2iν+1[Jν(ix)+iNν(ix)]=π2iν+1Hp(1)(ix)=π2Iν(x)Iν(x)sin(νπ) \begin{align*} I_{\nu}(x)&=i^{-\nu}J_{\nu}(ix) \\ \\ K_{\nu}(x) &= \frac{\pi}{2}i^{\nu+1}\left[ J_{\nu}(ix)+iN_{\nu}(ix) \right] \\ &= \frac{\pi}{2}i^{\nu+1}H_{p}^{(1)}(ix) \\ &=\frac{\pi}{2}\frac{I_{-\nu}(x)-I_{\nu}(x)}{\sin (\nu\pi )} \end{align*}

Here, JνJ_{\nu} Hν(1)(x)H_{\nu}^{(1)}(x) are Hankel functions.

Explanation

The reason for multiplication by ii upfront is to ensure that for real xx, the values of Iν(x)I_{\nu}(x) and Kν(x)K_{\nu}(x) are real. This situation is similar to that in which the solutions of y+y=0y^{\prime \prime}+y=0 are cosx\cos x and sinx\sin x, and the solutions of yy=0y^{\prime \prime}-y=0 are coshx=cos(ix)\cosh x=\cos (ix) and sinh(x)=sin(ix)\sinh (x)=\sin (ix). Due to these characteristics of the equations, IνI_{\nu} and KνK_{\nu} are also referred to as hyperbolic Bessel functions.

Integral Form

An integral form was made known by Olver et al. in 20101.

Iν(z)=(z2)νπΓ(ν+12)11ezt(1t2)ν12dt I_{\nu} (z) = {{ \left( {{ z } \over { 2 }} \right)^{\nu} } \over { \sqrt{\pi} \Gamma \left( \nu + {{ 1 } \over { 2 }} \right) }} \int_{-1}^{1} e^{zt} \left( 1 - t^{2} \right)^{\nu - {{ 1 } \over { 2 }}} dt

Such modified Bessel functions are crucial not only in mathematical physics but also in areas like directional statistics, and they appear in the Matérn function, which is one of the plausible choices for the semivariogram in spatial statistical analysis.


  1. Sungkyu Jung. “Geodesic projection of the von Mises–Fisher distribution for projection pursuit of directional data.” Electron. J. Statist. 15 (1) 984 - 1033, 2021. https://doi.org/10.1214/21-EJS1807 ↩︎