Modified Bessel functions : Iα, Kα

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Modified Bessel functions : Iα, Kα The Bessel functions are valid even for complex arguments x, and an important special case is that of a purely imaginary argument.

and are defined by any of these equivalent alternatives: Exist many integral representations of these functions.

The series expansion for I α (x) is thus similar to that for J α (x), but without the alternating ( 1) m factor.

of a real argument, I α and K α are exponentially growing and decaying functions, respectively.

1 Modified Bessel functions : Iα, Kα 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: Exist many integral representations of these functions. The following for K α (x), is useful for the calculus of the Feynmann propagator in the field theory: 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: 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

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

solving the Helmholtz equation in spherical coordinates by separation

independent solutions to this equation are called the spherical Bessel

2 Basset function modified Bessel function of the third kind modified Hankel function [2] MacDonald function Spherical Bessel functions: jn, yn 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: 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: [3]

3 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: The first spherical Bessel function j 0 (x) is also known as the (unnormalized) sinc function. The first few spherical Bessel functions are: [4] and [5] The general identity is Differential relations In the following f n is any of where

4 Spherical Hankel functions : h n There are also spherical analogues of the Hankel functions: 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 nonnegative integers n: and 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 : Sn,Cn,ζn Riccati Bessel functions only slightly differ from spherical Bessel functions: They satisfy the differential equation: 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) [6] for recent developments and references. Following Debye (1909), the notation ψ n,χ 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, one obtains: [7]

5 where γ is the Euler Mascheroni constant ( ) and Γ denotes the gamma function. For large arguments, they become: [7] (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, the modified Bessel functions become: while for small arguments, they become: Properties For integer order α = n, J n is often defined via a Laurent series for a generating function: an approach used by P. A. Hansen in (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:

6 which is used to expand a plane wave as a sum of cylindrical waves, or to find the Fourier series of a tonemodulated FM signal. More generally, a series is called Neumann expansion of ƒ. The coefficients for ν = 0 have the explicit form Selected functions admit the special representation where O k is Neumann's polynomial [8]. with due to the orthogonality relation More generally, if ƒ has a branch-point near the origin of such a nature that f(z) = a k J ν + k (z), k = 0 then or is ƒ's Laplace transform. [9] where Another way to define the Bessel functions is the Poisson representation formula:

7 where k > -1/2 and z is a complex number. [10] 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: 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: Modified Bessel functions follow similar relations : and The recurrence relation reads where C α denotes I α or e απi K 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: 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.)

8 Another orthogonality relation is the closure equation: 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: for α > 0. Another important property of Bessel's equations, which follows from Abel's identity, involves the Wronskian of the solutions: 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.) Connection with Fourier Transform The Fourier transform of Bessels functions have closed forms in the following situations: here U is Kummer's function of the second kind. Multiplication theorem The Bessel functions obey a multiplication theorem where λ and ν may be taken as arbitrary complex numbers. A similar form may be given for Y ν (z) and [11] [12] etc.

9 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. [13] 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 [14] Derivatives of J,Y,I,H,K These formulas may be found in this [15] reference. p - 1 dependency (note that the above equation is for y = J,Y,I,H (1),H (2) ) (note that the above equation is for y = K) p + 1 dependency (note that the above equation is for y = J,Y,K,H (1),H (2) ) (note that the above equation is for y = I) Other relationships (note that the above equation is for y = J,Y,H (1),H (2) only) (note that the above equation is for y = J,Y,H (1),H (2) only)

10 Selected identities

Bessel function - Wikipedia, the free encyclopedia

Bessel function - Wikipedia, the free encyclopedia Bessel function Page 1 of 9 From Wikipedia, the free encyclopedia In mathematics, Bessel functions, first defined by the mathematician Daniel Bernoulli