Bessel function

In mathematics, Bessel functions, first defined by the mathematician Daniel Bernoulli and generalized by Friedrich Bessel, are canonical solutions y(x) of Bessel's differential equation:

$x^2 \frac{d^2 y}{dx^2} + x \frac{dy}{dx} + (x^2 - \alpha^2)y = 0$

for an arbitrary real or complex number α (the order of the Bessel function). The most common and important special case is where α is an integer n.

Although α and −α produce the same differential equation, it is conventional to define different Bessel functions for these two orders (e.g., so that the Bessel functions are mostly smooth functions of α). Bessel functions are also known as cylinder functions or cylindrical harmonics because they are found in the solution to Laplace's equation in cylindrical coordinates.

Applications of Bessel function

Bessel's equation arises when finding separable solutions to Laplace's equation and the Helmholtz equation in cylindrical or spherical coordinates. Bessel functions are therefore especially important for many problems of wave propagation and static potentials. In solving problems in cylindrical coordinate systems, one obtains Bessel functions of integer order (α = n); in spherical problems, one obtains half-integer orders (α = n + ½). For example:

Electromagnetic waves in a cylindrical waveguide
Heat conduction in a cylindrical object
Modes of vibration of a thin circular (or annular) artificial membrane (such as a drum or other membranophone)
Diffusion problems on a lattice
Solutions to the radial Schrödinger equation (in spherical and cylindrical coordinates) for a free particle
Solving for patterns of acoustical radiation

Bessel functions also have useful properties for other problems, such as signal processing (e.g., see FM synthesis, Kaiser window, or Bessel filter).

Definitions

Since this is a second-order differential equation, there must be two linearly independent solutions. Depending upon the circumstances, however, various formulations of these solutions are convenient, and the different variations are described below.

Bessel functions of the first kind : J_α

Bessel functions of the first kind, denoted as $J_\alpha(x)$ , are solutions of Bessel's differential equation that are finite at the origin ( $x = 0$ ) for non-negative integer $\alpha$ , and diverge as $x$ approaches zero for negative non-integer $\alpha$ . The solution type (e.g., integer or non-integer) and normalization of $J_\alpha(x)$ are defined by its properties below. It is possible to define the function by its Taylor series expansion around $x = 0$ :^[1]

$J_\alpha(x) = \sum_{m=0}^\infty \frac{(-1)^m}{m! \, \Gamma(m+\alpha+1)} {\left({\frac{x}{2}}\right)}^{2m+\alpha}$

where $\Gamma(z)$ is the gamma function, a generalization of the factorial function to non-integer values. The graphs of Bessel functions look roughly like oscillating sine or cosine functions that decay proportionally to 1/√x (see also their asymptotic forms below), although their roots are not generally periodic, except asymptotically for large x. (The Taylor series indicates that $-J_1(x)$ is the derivative of $J_0(x)$ , much like $-\sin(x)$ is the derivative of $\cos(x)$ ; more generally, the derivative of $J_n(x)$ can be expressed in terms of $J_{n\pm 1}(x)$ by the identities below.)

Plot of Bessel function of the first kind, J_α(x), for integer orders α=0,1,2.

For non-integer α, the functions $J_\alpha (x)$ and $J_{-\alpha} (x)$ are linearly independent, and are therefore the two solutions of the differential equation. On the other hand, for integer order $\alpha$ , the following relationship is valid (note that the Gamma function becomes infinite for negative integer arguments):^[2]

$J_{-n}(x) = (-1)^n J_{n}(x).\,$

This means that the two solutions are no longer linearly independent. In this case, the second linearly independent solution is then found to be the Bessel function of the second kind, as discussed below.

Bessel's integrals

Another definition of the Bessel function, for integer values of $n$ , is possible using an integral representation:

$J_n(x) = \frac{1}{\pi} \int_0^\pi \cos (n \tau - x \sin \tau) \,\mathrm{d}\tau.$

Another integral representation is:

$J_n (x) = \frac{1}{2 \pi} \int_{-\pi}^\pi e^{-\mathrm{i}\,(n \tau - x \sin \tau)} \,\mathrm{d}\tau.$

This was the approach that Bessel used, and from this definition he derived several properties of the function. The definition may be extended to non-integer orders by the addition of another term

$J_\alpha(x) = \frac{1}{\pi} \int_0^\pi \cos(\alpha\tau- x \sin\tau)\,d\tau - \frac{\sin(\alpha\pi)}{\pi} \int_0^\infty e^{-x \sinh(t) - \alpha t} \, dt.$

or for $\alpha > -\frac{1}{2}$ by

$J_\alpha(x) = \frac{1}{\Gamma(\alpha + \frac{1}{2}) \sqrt{\pi}2^\alpha} \int_0^x (x^2-\tau^2)^{\alpha-\frac{1}{2}}\cos \tau \, d\tau.$

Relation to hypergeometric series

The Bessel functions can be expressed in terms of the generalized hypergeometric series as

$J_\alpha(x)=\frac{(x/2)^\alpha}{\Gamma(\alpha+1)} \;_0F_1 (\alpha+1; -x^2/4).$

This expression is related to the development of Bessel functions in terms of the Bessel–Clifford function.

Relation to Laguerre polynomials

In terms of the Laguerre polynomials $L_k$ and arbitrarily chosen parameter $t$ , the Bessel function can be expressed as^[3]

$\frac{J_\alpha(x)}{\left( \frac{x}{2}\right)^\alpha}= \frac{e^{-t}}{\Gamma(\alpha+1)} \sum_{k=0} \frac{L_k^{(\alpha)}\left( \frac{x^2}{4 t}\right)}{{k+ \alpha \choose k}} \frac{t^k}{k!}.$

Bessel functions of the second kind : Y_α

The Bessel functions of the second kind, denoted by Y_α(x), are solutions of the Bessel differential equation. They have a singularity at the origin (x = 0).

Plot of Bessel function of the second kind, Y_α(x), for integer orders α = 0, 1, 2.

Y_α(x) is sometimes also called the Neumann function, and is occasionally denoted instead by N_α(x). For non-integer α, it is related to J_α(x) by:

$Y_\alpha(x) = \frac{J_\alpha(x) \cos(\alpha\pi) - J_{-\alpha}(x)}{\sin(\alpha\pi)}.$

In the case of integer order n, the function is defined by taking the limit as a non-integer α tends to 'n':

$Y_n(x) = \lim_{\alpha \to n} Y_\alpha(x),$

which has the result (in integral form)

$Y_n(x) = \frac{1}{\pi} \int_0^\pi \sin(x \sin\theta - n\theta) \, d\theta - \frac{1}{\pi} \int_0^\infty \left[ e^{n t} + (-1)^n e^{-n t} \right] e^{-x \sinh t} \, dt.$

For the case of non-integer α, the definition of Y_α(x) is redundant (as is clear from its definition above). On the other hand, when α is an integer, Y_α(x) is the second linearly independent solution of Bessel's equation; moreover, as was similarly the case for the functions of the first kind, the following relationship is valid:

$Y_{-n}(x) = (-1)^n Y_n(x).\,$

Both J_α(x) and Y_α(x) are holomorphic functions of x on the complex plane cut along the negative real axis. When α is an integer, the Bessel functions J are entire functions of x. If x is held fixed, then the Bessel functions are entire functions of α.

Hankel functions: H_α⁽¹⁾, H_α⁽²⁾

Another important formulation of the two linearly independent solutions to Bessel's equation are the Hankel functions H_α⁽¹⁾(x) and H_α⁽²⁾(x), defined by:^[4]

$H_\alpha^{(1)}(x) = J_\alpha(x) + i Y_\alpha(x)$

$H_\alpha^{(2)}(x) = J_\alpha(x) - i Y_\alpha(x)$

where i is the imaginary unit. These linear combinations are also known as Bessel functions of the third kind; they are two linearly independent solutions of Bessel's differential equation. The Hankel functions of the first and second kind are used to express outward- and inward-propagating cylindrical wave solutions of the cylindrical wave equation, respectively (or vice versa, depending on the sign convention for the frequency). They are named after Hermann Hankel.

Using the previous relationships they can be expressed as:

$H_\alpha^{(1)} (x) = \frac{J_{-\alpha} (x) - e^{-\alpha \pi i} J_\alpha (x)}{i \sin (\alpha \pi)}$

$H_\alpha^{(2)} (x) = \frac{J_{-\alpha} (x) - e^{\alpha \pi i} J_\alpha (x)}{- i \sin (\alpha \pi)}$

if α is an integer, the limit has to be calculated. The following relationships are valid, whether α is an integer or not:^[5]

$H_{-\alpha}^{(1)} (x)= e^{\alpha \pi i} H_\alpha^{(1)} (x)$

$H_{-\alpha}^{(2)} (x)= e^{-\alpha \pi i} H_\alpha^{(2)} (x).$

The Hankel functions admit the following integral representations (useful in the calculus of the propagator of the Klein–Gordon field):^[6]

$H_\alpha^{(1)} (x)= \frac{e^{-\frac{1}{2} \alpha\pi i}}{\pi i}\int_{-\infty}^{+\infty} e^{ix\cosh t - \alpha t} \, dt.$

$H_\alpha^{(2)} (x)= -\frac{e^{-\frac{1}{2} \alpha\pi i}}{\pi i}\int_{-\infty}^{+\infty} e^{-ix\cosh t - \alpha t} \, dt.$

Modified Bessel functions : I_α, K_α

The Bessel functions are valid even for complex arguments x, and an important special case is that of a purely imaginary argument. In this case, the solutions to the Bessel equation are called the modified Bessel functions (or occasionally the hyperbolic Bessel functions) of the first and second kind, and are defined by any of these equivalent alternatives:^[7]

$I_\alpha(x) = i^{-\alpha} J_\alpha(ix) =\sum_{m=0}^{\infty} \frac{1}{m! \Gamma(m+\alpha+1)}\left(\frac{x}{2}\right)^{2m+\alpha}$

$K_\alpha(x) = \frac{\pi}{2} \frac{I_{-\alpha} (x) - I_\alpha (x)}{\sin (\alpha \pi)} = \frac{\pi}{2} i^{\alpha+1} H_\alpha^{(1)}(ix) = -\frac{\pi}{2} i^{\alpha+1} e^{-i \pi \alpha} H_\alpha^{(2)}(-ix).$

There exist many integral representations of these functions. The following for K_α (x), is useful for the calculus of the Feynman propagator in field theory:

$K_\alpha(x) = \frac{1}{2} e^{-\frac{1}{2}\alpha\pi i} \int_{-\infty}^{+\infty} e^{-ix\sinh t -\alpha t} dt$

These are chosen to be real-valued for real and positive arguments x. The series expansion for I_α(x) is thus similar to that for J_α(x), but without the alternating (−1)^m factor.

I_α(x) and K_α(x) are the two linearly independent solutions to the modified Bessel's equation:^[8]

$x^2 \frac{d^2 y}{dx^2} + x \frac{dy}{dx} - (x^2 + \alpha^2)y = 0.$

Unlike the ordinary Bessel functions, which are oscillating as functions of a real argument, I_α and K_α are exponentially growing and decaying functions, respectively. Like the ordinary Bessel function J_α, the function I_α goes to zero at x = 0 for α > 0 and is finite at x = 0 for α = 0. Analogously, K_α diverges at x = 0.

Modified Bessel functions of 1st kind, I_α(x), for α = 0, 1, 2, 3

Modified Bessel functions of 2nd kind, K_α(x), for α = 0, 1, 2, 3

The modified Bessel function of the second kind has also been called by the now-rare names:

Basset function
modified Bessel function of the third kind
modified Hankel function^[9]
MacDonald function

Spherical Bessel functions: j_n, y_n

Spherical Bessel functions of 1st kind, j_n(x), for n = 0, 1, 2

Spherical Bessel functions of 2nd kind, y_n(x), for n = 0, 1, 2

When solving the Helmholtz equation in spherical coordinates by separation of variables, the radial equation has the form:

$x^2 \frac{d^2 y}{dx^2} + 2x \frac{dy}{dx} + [x^2 - n(n+1)]y = 0.$

The two linearly independent solutions to this equation are called the spherical Bessel functions j_n and y_n, and are related to the ordinary Bessel functions J_n and Y_n by:^[10]

$j_{n}(x) = \sqrt{\frac{\pi}{2x}} J_{n+1/2}(x),$

$y_{n}(x) = \sqrt{\frac{\pi}{2x}} Y_{n+1/2}(x) = (-1)^{n+1} \sqrt{\frac{\pi}{2x}} J_{-n-1/2}(x).$

$y_n$ is also denoted $n_n$ or η_n; some authors call these functions the spherical Neumann functions.

The spherical Bessel functions can also be written as:

$j_n(x) = (-x)^n \left(\frac{1}{x}\frac{d}{dx}\right)^n\,\frac{\sin x}{x} ,$

$y_n(x) = -(-x)^n \left(\frac{1}{x}\frac{d}{dx}\right)^n\,\frac{\cos x}{x}.$

The first spherical Bessel function $j_0(x)$ is also known as the (unnormalized) sinc function. The first few spherical Bessel functions are:^[11]

$j_0(x)=\frac{\sin x} {x}$

$j_1(x)=\frac{\sin x} {x^2}- \frac{\cos x} {x}$

$j_2(x)=\left(\frac{3} {x^2} - 1 \right)\frac{\sin x}{x} - \frac{3\cos x} {x^2}$ ^[12]

$j_3(x)=\left(\frac{15}{x^3} - \frac{6}{x} \right)\frac{\sin x}{x} -\left(\frac{15}{x^2} - 1\right) \frac{\cos x} {x},$

and

$y_0(x)=-j_{-1}(x)=-\,\frac{\cos x} {x}$

$y_1(x)=j_{-2}(x)=-\,\frac{\cos x} {x^2}- \frac{\sin x} {x}$

$y_2(x)=-j_{-3}(x)=\left(-\,\frac{3}{x^2}+1 \right)\frac{\cos x}{x}- \frac{3 \sin x} {x^2};$

The general identity is

$J_{n+\frac 1 2}(x)=\sqrt \frac 2 {\pi x} \sum_{i=0}^\frac {n+1} 2 (-1)^{n-i}\left[\sin(x) \left(\frac 2 x\right)^{n-2i} \frac {(n-i)!}{i!} {-\frac 1 2-i \choose n-2i}- \cos(x) \left(\frac 2 x\right)^{n+1-2i} \frac {(n-i)!}{i!} i {-\frac 1 2-i \choose n-2i+1}\right].$

Generating function

The spherical Bessel function have the generating functions ^[13]

$\frac 1 {z} \cos \sqrt{z^2 - 2zt}= \sum_{n=0}^\infty \frac{t^n}{n!} j_{n-1}(z),$

$\frac 1 {z} \sin \sqrt{z^2 + 2zt}= \sum_{n=0}^\infty \frac{(-t)^n}{n!} y_{n-1}(z) .$

Differential relations

In the following $f_n$ is any of $j_n, y_n, h_n^{(1)}, h_n^{(2)}$ for $n=0,\pm 1,\pm 2,\dots$

$\left(\frac{1}{z}\frac{d}{dz}\right)^m\left(z^{n+1}f_n(z)\right)=z^{(n-m)+1}f_{(n-m)}(z).$

Spherical Hankel functions : h_n

There are also spherical analogues of the Hankel functions:

$h_n^{(1)}(x) = j_n(x) + i y_n(x) \,$

$h_n^{(2)}(x) = j_n(x) - i y_n(x). \,$

In fact, there are simple closed-form expressions for the Bessel functions of half-integer order in terms of the standard trigonometric functions, and therefore for the spherical Bessel functions. In particular, for non-negative integers n:

$h_n^{(1)}(x) = (-i)^{n+1} \frac{e^{ix}}{x} \sum_{m=0}^n \frac{i^m}{m!(2x)^m} \frac{(n+m)!}{(n-m)!}$

and $h_n^{(2)}$ is the complex-conjugate of this (for real $x$ ). It follows, for example, that $j_0(x) = \sin(x)/x$ and $y_0(x) = -\cos(x)/x$ , and so on.

Riccati–Bessel functions: S_n, C_n, ξ_n, ζ_n

Riccati–Bessel functions only slightly differ from spherical Bessel functions:

$S_n(x)=x j_n(x)=\sqrt{\pi x/2} \, J_{n+1/2}(x)$

$C_n(x)=-x y_n(x)=-\sqrt{\pi x/2} \, Y_{n+1/2}(x)$

$\xi_n(x) = x h_n^{(1)}(x)=\sqrt{\pi x/2} \, H_{n+1/2}^{(1)}(x)=S_n(x)-iC_n(x)$

$\zeta_n(x)=x h_n^{(2)}(x)=\sqrt{\pi x/2} \, H_{n+1/2}^{(2)}(x)=S_n(x)+iC_n(x).$

They satisfy the differential equation:

$x^2 \frac{d^2 y}{dx^2} + [x^2 - n (n+1)] y = 0.$

This differential equation, and the Riccati–Bessel solutions, arises in the problem of scattering of electromagnetic waves by a sphere, known as Mie scattering after the first published solution by Mie (1908). See e.g., Du (2004)^[14] for recent developments and references.

Following Debye (1909), the notation $\psi_n,\chi_n$ is sometimes used instead of $S_n,C_n$ .

Asymptotic forms

The Bessel functions have the following asymptotic forms for non-negative α. For small arguments $0 < x \ll \sqrt{\alpha + 1}$ , one obtains:^[15]

$J_\alpha(x) \approx \frac{1}{\Gamma(\alpha+1)} \left( \frac{x}{2} \right) ^\alpha$

$Y_\alpha(x) \approx \begin{cases} \frac{2}{\pi} \left[ \ln (x/2) + \gamma \right] & \text{if } \alpha=0 \\ \\ -\frac{\Gamma(\alpha)}{\pi} \left( \frac{2}{x} \right) ^\alpha & \text{if } \alpha > 0 \end{cases}$

where $\gamma$ is the Euler–Mascheroni constant (0.5772...) and $\Gamma$ denotes the gamma function. For large arguments $x \gg |\alpha^2 - 1/4|$ , they become:^[15]

$J_\alpha(x)\approx \sqrt{\frac{2}{\pi x}} \cos \left( x-\frac{\alpha\pi}{2} - \frac{\pi}{4} \right)$

$Y_\alpha(x) \approx \sqrt{\frac{2}{\pi x}} \sin \left( x-\frac{\alpha\pi}{2} - \frac{\pi}{4} \right).$

(For α=1/2 these formulas are exact; see the spherical Bessel functions above.) Asymptotic forms for the other types of Bessel function follow straightforwardly from the above relations. For example, for large $x \gg |\alpha^2 - 1/4|$ , the modified Bessel functions become:

$I_\alpha(x) \approx \frac{e^x}{\sqrt{2\pi x}} \left(1+ \frac{(1-2 \alpha)(1+2\alpha)}{8x}+ \cdots \right) ,$

$K_\alpha(x) \approx \sqrt{\frac{\pi}{2x}} e^{-x}.$

while for small arguments $0 < x \ll \sqrt{\alpha + 1}$ , they become:

$I_\alpha(x) \approx \frac{1}{\Gamma(\alpha+1)} \left( \frac{x}{2} \right) ^\alpha$

$K_\alpha(x) \approx \begin{cases} - \ln (x/2) - \gamma & \text{if } \alpha=0 \\ \\ \frac{\Gamma(\alpha)}{2} \left( \frac{2}{x} \right) ^\alpha & \text{if } \alpha > 0. \end{cases}$

Properties

For integer order α = n, J_n is often defined via a Laurent series for a generating function:

$e^{(x/2)(t-1/t)} = \sum_{n=-\infty}^\infty J_n(x) t^n,$

an approach used by P. A. Hansen in 1843. (This can be generalized to non-integer order by contour integration or other methods.) Another important relation for integer orders is the Jacobi–Anger expansion:

$e^{iz \cos \phi} = \sum_{n=-\infty}^\infty i^n J_n(z) e^{in\phi},$

which is used to expand a plane wave as a sum of cylindrical waves, or to find the Fourier series of a tone-modulated FM signal.

More generally, a series

$f(z)=a_0^\nu J_\nu (z)+ 2 \cdot \sum_{k=1} a_k^\nu J_{\nu+k}(z)$

is called Neumann expansion of ƒ. The coefficients for $\nu=0$ have the explicit form

$a_k^0=\frac{1}{2 \pi i} \int_{|z|=c} f(z) O_k(z) \, \mathrm d z,$

where $O_k$ is Neumann's polynomial ^[16].

Selected functions admit the special representation

$f(z)=\sum_{k=0} a_k^\nu J_{\nu+2k}(z)$

with

$a_k^\nu=2(\nu+2k) \int_0^\infty f(z) \frac{J_{\nu+2k}(z)}z \mathrm d z$

due to the orthogonality relation $\int_0^\infty J_\alpha(z) J_\beta(z) \frac {\mathrm d z} z= \frac 2 \pi \frac{\sin\left(\frac \pi 2 (\alpha-\beta) \right)}{\alpha^2 -\beta^2}.$

More generally, if ƒ has a branch-point near the origin of such a nature that $f(z)= \sum_{k=0} a_k J_{\nu+k}(z),$ then

$\mathcal L \left\{\sum_{k=0} a_k J_{\nu+k} \right\}(s)= \frac 1 \sqrt{1+s^2} \sum_{k=0} \frac{a_k}{(s+\sqrt{1+s^2})^{\nu+k}}$ or

$\sum_{k=0} a_k \xi^{\nu+k}= \frac{1+\xi^2}{2\xi} \mathcal L \{f \} \left( \frac{1-\xi^2}{2\xi} \right),$

where $\mathcal L \{f \}$ is ƒ's Laplace transform.^[17]

Another way to define the Bessel functions is the Poisson representation formula and the Mehler-Sonine formula:

$\begin{align}J_\nu(z) &= \frac{ (\frac{z}{2})^\nu }{ \Gamma(\nu + \frac{1}{2} ) \sqrt{\pi} } \int_{-1}^{1} e^{izs}(1 - s^2)^{\nu - \frac{1}{2} } ds, \\ &=\frac 2{{\left(\frac z 2\right)}^\nu\cdot \sqrt{\pi} \cdot \Gamma\left(\frac 1 2-\nu\right)} \int_1^\infty \frac{\sin(z u)}{(u^2-1)^{\nu+\frac 1 2}} d u,\end{align}$

where ν > −1/2 and z is a complex number.^[18] This formula is useful especially when working with Fourier transforms.

The functions J_α, Y_α, H_α⁽¹⁾, and H_α⁽²⁾ all satisfy the recurrence relations:

$\frac{2\alpha}{x} Z_\alpha(x) = Z_{\alpha-1}(x) + Z_{\alpha+1}(x)$

$2\frac{dZ_\alpha}{dx} = Z_{\alpha-1}(x) - Z_{\alpha+1}(x)$

where Z denotes J, Y, H⁽¹⁾, or H⁽²⁾. (These two identities are often combined, e.g. added or subtracted, to yield various other relations.) In this way, for example, one can compute Bessel functions of higher orders (or higher derivatives) given the values at lower orders (or lower derivatives). In particular, it follows that:

$\left( \frac{d}{x dx} \right)^m \left[ x^\alpha Z_{\alpha} (x) \right] = x^{\alpha - m} Z_{\alpha - m} (x)$

$\left( \frac{d}{x dx} \right)^m \left[ \frac{Z_\alpha (x)}{x^\alpha} \right] = (-1)^m \frac{Z_{\alpha + m} (x)}{x^{\alpha + m}}.$

Modified Bessel functions follow similar relations :

$e^{(x/2)(t+1/t)} = \sum_{n=-\infty}^\infty I_n(x) t^n,$

and

$e^{z \cos \theta} = I_0(z) + 2\sum_{n=1}^\infty I_n(z) \cos(n\theta),$

The recurrence relation reads

$C_{\alpha-1}(x) - C_{\alpha+1}(x) = \frac{2\alpha}{x} C_\alpha(x)$

$C_{\alpha-1}(x) + C_{\alpha+1}(x) = 2\frac{dC_\alpha}{dx}$

where C_α denotes I_α or e^απiK_α. These recurrence relations are useful for discrete diffusion problems.

Because Bessel's equation becomes Hermitian (self-adjoint) if it is divided by x, the solutions must satisfy an orthogonality relationship for appropriate boundary conditions. In particular, it follows that:

$\int_0^1 x J_\alpha(x u_{\alpha,m}) J_\alpha(x u_{\alpha,n}) dx = \frac{\delta_{m,n}}{2} [J_{\alpha+1}(u_{\alpha,m})]^2 = \frac{\delta_{m,n}}{2} [J_{\alpha}'(u_{\alpha,m})]^2,$

where α > −1, δ_m,n is the Kronecker delta, and u_α,m is the m-th zero of J_α(x). This orthogonality relation can then be used to extract the coefficients in the Fourier–Bessel series, where a function is expanded in the basis of the functions J_α(x u_α,m) for fixed α and varying m.

An analogous relationship for the spherical Bessel functions follows immediately:

$\int_0^1 x^2 j_\alpha(x u_{\alpha,m}) j_\alpha(x u_{\alpha,n}) dx = \frac{\delta_{m,n}}{2} [j_{\alpha+1}(u_{\alpha,m})]^2$

Another orthogonality relation is the closure equation:

$\int_0^\infty x J_\alpha(ux) J_\alpha(vx) dx = \frac{1}{u} \delta(u - v)$

for α > −1/2 and where δ is the Dirac delta function. This property is used to construct an arbitrary function from a series of Bessel functions by means of the Hankel transform. For the spherical Bessel functions the orthogonality relation is:

$\int_0^\infty x^2 j_\alpha(ux) j_\alpha(vx) dx = \frac{\pi}{2u^2} \delta(u - v)$

for α > −1.

Another important property of Bessel's equations, which follows from Abel's identity, involves the Wronskian of the solutions:

$A_\alpha(x) \frac{dB_\alpha}{dx} - \frac{dA_\alpha}{dx} B_\alpha(x) = \frac{C_\alpha}{x},$

where A_α and B_α are any two solutions of Bessel's equation, and C_α is a constant independent of x (which depends on α and on the particular Bessel functions considered). For example, if A_α = J_α and B_α = Y_α, then C_α is 2/π. This also holds for the modified Bessel functions; for example, if A_α = I_α and B_α = K_α, then C_α is −1.

(There are a large number of other known integrals and identities that are not reproduced here, but which can be found in the references.)

Multiplication theorem

The Bessel functions obey a multiplication theorem

$\lambda^{-\nu} J_\nu (\lambda z) = \sum_{n=0}^\infty \frac{1}{n!} \left(\frac{(1-\lambda^2)z}{2}\right)^n J_{\nu+n}(z)$

where $\lambda$ and $\nu$ may be taken as arbitrary complex numbers. A similar form may be given for $Y_\nu(z)$ and etc.^[19] ^[20]

Bourget's hypothesis

Bessel himself originally proved that for non-negative integers n, the equation J_n(x) = 0 has an infinite number of solutions in x.^[21] When the functions J_n(x) are plotted on the same graph, though, none of the zeros seem to coincide for different values of n except for the zero at x = 0. This phenomenon is known as Bourget's hypothesis after the nineteenth century French mathematician who studied Bessel functions. Specifically it states that for any integers n ≥ 0 and m ≥ 1, the functions J_n(x) and J_n+m(x) have no common zeros other than the one at x = 0. The theorem was proved by Siegel in 1929.^[22]

Derivatives of J,Y,I,H,K

These formulas may be found in this ^[23] reference.

p − 1 dependency

$\frac{d}{dx}y_p(\alpha x)=\alpha y_{p-1}(\alpha x) - \frac{p}{x} y_p(\alpha x)$

(note that the above equation is for $y = J, Y, I, H^{(1)}, H^{(2)}$ )

$\frac{d}{dx}y_p(\alpha x)=-\alpha y_{p-1}(\alpha x) - \frac{p}{x} y_p(\alpha x)$

(note that the above equation is for $y = K$ )

p + 1 dependency

$\frac{d}{dx}y_p(\alpha x)=-\alpha y_{p+1}(\alpha x) + \frac{p}{x} y_p(\alpha x)$

(note that the above equation is for $y = J, Y, K, H^{(1)}, H^{(2)}$ )

$\frac{d}{dx}y_p(\alpha x)=\alpha y_{p+1}(\alpha x) + \frac{p}{x} y_p(\alpha x)$

(note that the above equation is for $y = I$ )

Other relationships

$\frac{d}{dx}y_p(\alpha x)=\frac{\alpha}{2}[y_{p-1}(\alpha x) - y_{p+1}(\alpha x)]$

(note that the above equation is for $y = J, Y, H^{(1)}, H^{(2)}$ only)

$y_{p-1}(\alpha x) + y_{p+1}(\alpha x)=\frac{2p}{\alpha x}y_p(\alpha x)$

(note that the above equation is for $y = J, Y, H^{(1)}, H^{(2)}$ only)

Selected identities

$I_{-\frac{1}{2}} \left(\frac{z}{2}\right)+ I_{\frac{1}{2}} \left(\frac{z}{2} \right)= \frac{2 e^{\frac{z}{2}}}{\sqrt{\pi z}}�;$
$I_\nu(z)=\sum_{k=0} \frac{z^k}{k!} J_{\nu+k}(z);$
$J_\nu(z)=\sum_{k=0} (-1)^k \frac{z^k}{k!} I_{\nu+k}(z);$
$I_\nu (\lambda z)= \lambda^\nu \sum_{k=0} \frac{\left((\lambda^2-1) \frac z 2 \right)^k}{k!} I_{\nu+k}(z);$
$I_\nu (z_1+z_2)= \sum_{k=-\infty}^\infty I_{\nu-k}(z_1)I_k(z_2);$
$J_\nu(z)=\frac z {2 \nu} (J_{\nu-1}(z)+J_{\nu+1}(z)), \quad I_\nu(z)=\frac z {2 \nu} (I_{\nu-1}(z)-I_{\nu+1}(z));$
$J_\nu'(z)=\frac 1 2 (J_{\nu-1}(z)-J_{\nu+1}(z)), \quad I_\nu'(z)=\frac 1 2 (I_{\nu-1}(z)+I_{\nu+1}(z));$
$\left( \frac x 2\right)^\nu= \sum_{k=0} (-1)^k \frac {\Gamma(k+\nu)}{k!} (2k+\nu) I_{2k+\nu}(x).$

Notes

↑ Abramowitz and Stegun, p. 360, 9.1.10.
↑ Abramowitz and Stegun, p. 358, 9.1.5.
↑ Szegö, G. Orthogonal Polynomials, 4th ed. Providence, RI: Amer. Math. Soc., 1975.
↑ Abramowitz and Stegun, p. 358, 9.1.3, 9.1.4.
↑ Abramowitz and Stegun, p. 358, 9.1.6.
↑ Abramowitz and Stegun, p. 360, 9.1.25.
↑ Abramowitz and Stegun, p. 375, 9.6.2, 9.6.10, 9.6.11.
↑ Abramowitz and Stegun, p. 374, 9.6.1.
↑ Referred to as such in: Teichroew, D. The Mixture of Normal Distributions with Different Variances, The Annals of Mathematical Statistics. Vol. 28, No. 2 (Jun., 1957), pp. 510–512
↑ Abramowitz and Stegun, p. 437, 10.1.1.
↑ Abramowitz and Stegun, p. 438, 10.1.11, 10.1.12;
↑ Abramowitz and Stegun, p. 438, 10.1.11.
↑ Abramowitz and Stegun, p. 439, 10.1.39.
↑ Hong Du, "Mie-scattering calculation," Applied Optics 43 (9), 1951–1956 (2004)
↑ ^15.0 ^15.1 Arfken & Weber.
↑ Abramowitz and Stegun, p. 363, 9.1.82 ff.
↑ E. T. Whittaker, G. N. Watson, A course in modern Analysis p. 536
↑ I.S. Gradshteyn (И.С. Градштейн), I.M. Ryzhik (И.М. Рыжик); Alan Jeffrey, Daniel Zwillinger, editors. Table of Integrals, Series, and Products, seventh edition. Academic Press, 2007. ISBN 978-0-12-373637-6. Equation 8.411.10
↑ Abramowitz and Stegun, p. 363, 9.1.74.
↑ C. Truesdell, "On the Addition and Multiplication Theorems for the Special Functions", Proceedings of the National Academy of Sciences, Mathematics, (1950) pp.752–757.
↑ F. Bessel, Untersuchung des Theils der planetarischen Störungen, Berlin Abhandlungen (1824), article 14.
↑ Watson, pp. 484–5
↑ "Advanced Calculus for Engineers", F. B. Hildebrand, 6th printing, pp. 163–164 (1956)

References

Abramowitz, Milton; Stegun, Irene A., eds. (1965), "Chapter 9", Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, New York: Dover, pp. 355, MR 0167642, ISBN 978-0486612720, http://www.math.sfu.ca/~cbm/aands/page_355.htm See also chapter 10.
Arfken, George B. and Hans J. Weber, Mathematical Methods for Physicists, 6th edition (Harcourt: San Diego, 2005). ISBN 0-12-059876-0.
Bayin, S.S. Mathematical Methods in Science and Engineering, Wiley, 2006, Chapter 6.
Bayin, S.S., Essentials of Mathematical Methods in Science and Engineering, Wiley, 2008, Chapter 11.
Bowman, Frank Introduction to Bessel Functions (Dover: New York, 1958). ISBN 0-486-60462-4.
G. Mie, "Beiträge zur Optik trüber Medien, speziell kolloidaler Metallösungen", Ann. Phys. Leipzig 25 (1908), p. 377.
Olver, F. W. J.; Maximon, L. C. (2010), "Bessel function", in Olver, Frank W. J.; Lozier, Daniel M.; Boisvert, Ronald F. et al., NIST Handbook of Mathematical Functions, Cambridge University Press, ISBN 978-0521192255, http://dlmf.nist.gov/10
B Spain, M.G. Smith, Functions of mathematical physics, Van Nostrand Reinhold Company, London, 1970. Chapter 9 deals with Bessel functions.
Watson, G.N., A Treatise on the Theory of Bessel Functions, Second Edition, (1995) Cambridge University Press. ISBN 0-521-48391-3.

External links

Lizorkin, P.I. (2001), "Bessel functions", in Hazewinkel, Michiel, Encyclopaedia of Mathematics, Springer, ISBN 978-1556080104, http://eom.springer.de/b/b015840.htm
Karmazina, L.N.; Prudnikov, A.P. (2001), "Cylinder function", in Hazewinkel, Michiel, Encyclopaedia of Mathematics, Springer, ISBN 978-1556080104, http://eom.springer.de/c/c027610.htm
Rozov, =N.Kh. (2001), "Bessel equation", in Hazewinkel, Michiel, Encyclopaedia of Mathematics, Springer, ISBN 978-1556080104, http://eom.springer.de/B/b015830.htm
Wolfram function pages on Bessel J and Y functions, and modified Bessel I and K functions. Pages include formulas, function evaluators, and plotting calculators.
Wolfram Mathworld – Bessel functions of the first kind