title: Bessel function
text: Bessel functions, first defined by the mathematician Daniel Bernoulli and then generalized by Friedrich Bessel, are canonical solutions  of Bessel's differential equation
  
  for an arbitrary complex number , which represents the order of the Bessel function. Although  and  produce the same differential equation, it is conventional to define different Bessel functions for these two values in such a way that the Bessel functions are mostly smooth functions of .
  
  The most important cases are when  is an integer or half-integer. Bessel functions for integer  are also known as cylinder functions or the cylindrical harmonics because they appear in the solution to Laplace's equation in cylindrical coordinates. Spherical Bessel functions with half-integer  are obtained when solving the Helmholtz equation in spherical coordinates.
  
  Applications of Bessel functions
  The Bessel function is a generalization of the sine function. It can be interpreted as the vibration of a string with variable thickness, variable tension (or both conditions simultaneously); vibrations in a medium with variable properties; vibrations of the disc membrane, etc.
  
  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 (); in spherical problems, one obtains half-integer orders (). For example:
  
   Electromagnetic waves in a cylindrical waveguide
   Pressure amplitudes of inviscid rotational flows
   Heat conduction in a cylindrical object
   Modes of vibration of a thin circular or annular acoustic membrane (such as a drumhead or other membranophone) or thicker plates such as sheet metal (see Kirchhoff–Love plate theory, Mindlin–Reissner plate theory)
   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
   Frequency-dependent friction in circular pipelines
   Dynamics of floating bodies
   Angular resolution
   Diffraction from helical objects, including DNA
   Probability density function of product of two normally distributed random variables
   Analyzing of the surface waves generated by microtremors, in geophysics and seismology. 
  
  Bessel functions also appear in other problems, such as signal processing (e.g., see FM audio synthesis, Kaiser window, or Bessel filter).
  
  Definitions
  Because this is a second-order linear differential equation, there must be two linearly independent solutions. Depending upon the circumstances, however, various formulations of these solutions are convenient. Different variations are summarized in the table below and described in the following sections.
  
  Bessel functions of the second kind and the spherical Bessel functions of the second kind are sometimes denoted by  and , respectively, rather than  and .
  
  Bessel functions of the first kind: 
  
  Bessel functions of the first kind, denoted as , are solutions of Bessel's differential equation. For integer or positive , Bessel functions of the first kind are finite at the origin (); while for negative non-integer , Bessel functions of the first kind diverge as  approaches zero. It is possible to define the function by its series expansion around , which can be found by applying the Frobenius method to Bessel's equation:
  
  where  is the gamma function, a shifted generalization of the factorial function to non-integer values. The Bessel function of the first kind is an entire function if  is an integer, otherwise it is a multivalued function with singularity at zero. The graphs of Bessel functions look roughly like oscillating sine or cosine functions that decay proportionally to  (see also their asymptotic forms below), although their roots are not generally periodic, except asymptotically for large . (The series indicates that  is the derivative of , much like  is the derivative of ; more generally, the derivative of  can be expressed in terms of  by the identities below.)
  
  For non-integer , the functions  and  are linearly independent, and are therefore the two solutions of the differential equation. On the other hand, for integer order , the following relationship is valid (the gamma function has simple poles at each of the non-positive integers):
  
  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 , is possible using an integral representation:
  
  which is also called Hansen-Bessel formula.
  
  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 one of Schläfli's integrals, for :
  
  Relation to hypergeometric series
  The Bessel functions can be expressed in terms of the generalized hypergeometric series as
  
  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  and arbitrarily chosen parameter , the Bessel function can be expressed as
  
  Bessel functions of the second kind: 
  The Bessel functions of the second kind, denoted by , occasionally denoted instead by , are solutions of the Bessel differential equation that have a singularity at the origin () and are multivalued. These are sometimes called Weber functions, as they were introduced by , and also Neumann functions after Carl Neumann.
  
  For non-integer ,  is related to  by
  
  In the case of integer order , the function is defined by taking the limit as a non-integer  tends to :
  
  If  is a nonnegative integer, we have the series
  
  where  is the digamma function, the logarithmic derivative of the gamma function.
  
  There is also a corresponding integral formula (for ):
  
  In the case where ,
  
   is necessary as the second linearly independent solution of the Bessel's equation when  is an integer. But  has more meaning than that. It can be considered as a "natural" partner of . See also the subsection on Hankel functions below.
  
  When  is an integer, moreover, as was similarly the case for the functions of the first kind, the following relationship is valid:
  
  Both  and  are holomorphic functions of  on the complex plane cut along the negative real axis. When  is an integer, the Bessel functions  are entire functions of . If  is held fixed at a non-zero value, then the Bessel functions are entire functions of .
  
  The Bessel functions of the second kind when  is an integer is an example of the second kind of solution in Fuchs's theorem.
  
  Hankel functions: , 
  
  Another important formulation of the two linearly independent solutions to Bessel's equation are the Hankel functions of the first and second kind,  and , defined as
  
  where  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. They are named after Hermann Hankel.
  
  These forms of linear combination satisfy numerous simple-looking properties, like asymptotic formulae or integral representations. Here, "simple" means an appearance of a factor of the form . For real  where ,  are real-valued, the Bessel functions of the first and second kind are the real and imaginary parts, respectively, of the first Hankel function and the real and negative imaginary parts of the second Hankel function. Thus, the above formulae are analogs of Euler's formula, substituting ,  for  and ,  for , , as explicitly shown in the asymptotic expansion.
  
  The Hankel functions 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).
  
  Using the previous relationships, they can be expressed as
  
  If  is an integer, the limit has to be calculated. The following relationships are valid, whether  is an integer or not:
  
  In particular, if  with  a nonnegative integer, the above relations imply directly that
  
  These are useful in developing the spherical Bessel functions (see below).
  
  The Hankel functions admit the following integral representations for :
  
  where the integration limits indicate integration along a contour that can be chosen as follows: from  to 0 along the negative real axis, from 0 to  along the imaginary axis, and from  to  along a contour parallel to the real axis.
  
  Modified Bessel functions: , 
  The Bessel functions are valid even for complex arguments , 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 as
  
  when  is not an integer; when  is an integer, then the limit is used. These are chosen to be real-valued for real and positive arguments . The series expansion for  is thus similar to that for , but without the alternating  factor.
  
   can be expressed in terms of Hankel functions:
  
  Using these two formulae the result to +, commonly known as Nicholson's integral or Nicholson's formula, can be obtained to give the following
  
  given that the condition  is met. It can also be shown that
  
  only when || <  and  but not when .
  
  We can express the first and second Bessel functions in terms of the modified Bessel functions (these are valid if ):
  
   and  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,  and  are exponentially growing and decaying functions respectively. Like the ordinary Bessel function , the function  goes to zero at  for  and is finite at  for . Analogously,  diverges at  with the singularity being of logarithmic type for , and  otherwise.
  
  Two integral formulas for the modified Bessel functions are (for ):
  
  Bessel functions can be described as Fourier transforms of powers of quadratic functions. For example (for ):
  
  It can be proven by showing equality to the above integral definition for . This is done by integrating a closed curve in the first quadrant of the complex plane.
  
  Modified Bessel functions  and  can be represented in terms of rapidly convergent integrals
  
  The modified Bessel function  is useful to represent the Laplace distribution as an Exponential-scale mixture of normal distributions.
  
  The modified Bessel function of the second kind has also been called by the following names (now rare):
  
   Basset function after Alfred Barnard Basset
   Modified Bessel function of the third kind
   Modified Hankel function
   Macdonald function after Hector Munro Macdonald
  
  Spherical Bessel functions: , 
  
  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  and , and are related to the ordinary Bessel functions  and  by
  
   is also denoted  or ; some authors call these functions the spherical Neumann functions.
  
  From the relations to the ordinary Bessel functions it is directly seen that:
  
  The spherical Bessel functions can also be written as (Rayleigh's formulas)
  
  The zeroth spherical Bessel function  is also known as the (unnormalized) sinc function. The first few spherical Bessel functions are:
  
  and
  
  Generating function
  The spherical Bessel functions have the generating functions
  
  Differential relations
  In the following,  is any of , , ,  for
  
  Spherical Hankel functions: , 
  
  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 non-negative integers :
  
  and  is the complex-conjugate of this (for real ). It follows, for example, that  and , and so on.
  
  The spherical Hankel functions appear in problems involving spherical wave propagation, for example in the multipole expansion of the electromagnetic field.
  
  Riccati–Bessel functions: , , , 
  Riccati–Bessel functions only slightly differ from spherical Bessel functions:
  
  They satisfy the differential equation
  
  For example, this kind of differential equation appears in quantum mechanics while solving the radial component of the Schrödinger's equation with hypothetical cylindrical infinite potential barrier. This differential equation, and the Riccati–Bessel solutions, also 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) for recent developments and references.
  
  Following Debye (1909), the notation ,  is sometimes used instead of , .
  
  Asymptotic forms
  The Bessel functions have the following asymptotic forms. For small arguments , one obtains, when  is not a negative integer:
  
  When  is a negative integer, we have
  
  For the Bessel function of the second kind we have three cases:
  
  where  is the Euler–Mascheroni constant (0.5772...).
  
  For large real arguments , one cannot write a true asymptotic form for Bessel functions of the first and second kind (unless  is half-integer) because they have zeros all the way out to infinity, which would have to be matched exactly by any asymptotic expansion. However, for a given value of  one can write an equation containing a term of order :
  
  (For  the last terms in these formulas drop out completely; see the spherical Bessel functions above.) 
  
  The asymptotic forms for the Hankel functions are:
  
  These can be extended to other values of  using equations relating  and  to  and .
  
  It is interesting that although the Bessel function of the first kind is the average of the two Hankel functions,  is not asymptotic to the average of these two asymptotic forms when  is negative (because one or the other will not be correct there, depending on the  used). But the asymptotic forms for the Hankel functions permit us to write asymptotic forms for the Bessel functions of first and second kinds for complex (non-real)  so long as  goes to infinity at a constant phase angle  (using the square root having positive real part):
  
  For the modified Bessel functions, Hankel developed asymptotic (large argument) expansions as well:
  
  There is also the asymptotic form (for large real )
  
  When , all the terms except the first vanish, and we have
  
  For small arguments , we have
  
  Properties
  
  For integer order ,  is often defined via a Laurent series for a generating function:
  
  an approach used by P. A. Hansen in 1843. (This can be generalized to non-integer order by contour integration or other methods.)
  
  A series expansion using Bessel functions (Kapteyn series) is
   
  
  Another important relation for integer orders is the Jacobi–Anger expansion:
  
  and
  
  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
  
  is called Neumann expansion of . The coefficients for  have the explicit form
  
  where  is Neumann's polynomial.
  
  Selected functions admit the special representation
  
  with
  
  due to the orthogonality relation
  
  More generally, if  has a branch-point near the origin of such a nature that
  
  then
  
  or
  
  where  is the Laplace transform of .
  
  Another way to define the Bessel functions is the Poisson representation formula and the Mehler-Sonine formula:
  
  where  and .
  This formula is useful especially when working with Fourier transforms.
  
  Because Bessel's equation becomes Hermitian (self-adjoint) if it is divided by , the solutions must satisfy an orthogonality relationship for appropriate boundary conditions. In particular, it follows that:
  
  where ,  is the Kronecker delta, and  is the th zero of . 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  for fixed  and varying .
  
  An analogous relationship for the spherical Bessel functions follows immediately:
  
  If one defines a boxcar function of  that depends on a small parameter  as:
  
  (where  is the rectangle function) then the Hankel transform of it (of any given order ), , approaches  as  approaches zero, for any given . Conversely, the Hankel transform (of the same order) of  is :
  
  which is zero everywhere except near 1. As  approaches zero, the right-hand side approaches , where  is the Dirac delta function. This admits the limit (in the distributional sense):
  
  A change of variables then yields the closure equation:
  
  for . The Hankel transform can express a fairly arbitrary function as an integral of Bessel functions of different scales. For the spherical Bessel functions the orthogonality relation is:
  
  for .
  
  Another important property of Bessel's equations, which follows from Abel's identity, involves the Wronskian of the solutions:
  
  where  and  are any two solutions of Bessel's equation, and  is a constant independent of  (which depends on α and on the particular Bessel functions considered). In particular,
  
  and
  
  for .
  
  For , the even entire function of genus 1, , has only real zeros. Let
  
  be all its positive zeros, then
  
  (There are a large number of other known integrals and identities that are not reproduced here, but which can be found in the references.)
  
  Recurrence relations
  The functions , , , and  all satisfy the recurrence relations
  
  and
  
  where  denotes , , , or . 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
  
  and
  
  The recurrence relation reads
  
  where  denotes  or . These recurrence relations are useful for discrete diffusion problems.
  
  Transcendence
  In 1929, Carl Ludwig Siegel proved that , , and the quotient {{math|{{sfrac|Jν(x)|Jν(x)}}}} are transcendental numbers when ν is rational and x is algebraic and nonzero. The same proof also implies that  is transcendental under the same assumptions.
  
  Multiplication theorem
  The Bessel functions obey a multiplication theorem
  
  where  and  may be taken as arbitrary complex numbers. For , the above expression also holds if  is replaced by . The analogous identities for modified Bessel functions and  are
  
  and
  
  Zeros of the Bessel function
  
  Bourget's hypothesis
  Bessel himself originally proved that for nonnegative integers , the equation  has an infinite number of solutions in . When the functions  are plotted on the same graph, though, none of the zeros seem to coincide for different values of  except for the zero at . This phenomenon is known as Bourget's hypothesis''' after the 19th-century French mathematician who studied Bessel functions. Specifically it states that for any integers  and , the functions  and  have no common zeros other than the one at . The hypothesis was proved by Carl Ludwig Siegel in 1929.
  
  Transcendence
  Siegel proved in 1929 that when ν is rational, all nonzero roots of  and  are transcendental, as are all the roots of . It is also known that all roots of the higher derivatives  for  are transcendental, except for the special values  and .
  
  Numerical approaches
  For numerical studies about the zeros of the Bessel function, see ,  and .
  
  Numerical values
  The first zero in J0 (i.e, j0,1, j0,2 and j0,3) occurs at arguments of approximately 2.40483, 5.52008 and 8.65373, respectively.
  
  Bessel Functions in Popular Culture
  
  Young Sheldon
  In the season 5 episode "The Yips and an Oddly Hypnotic Bohemian", Young Sheldon (Young Sheldon) is attempting to complete a quantum mechanics test and runs out of time because he cannot remember the zeroes to the Bessel function.
  
  See also
  
   Anger function
   Bessel polynomials
   Bessel–Clifford function
   Bessel–Maitland function
   Fourier–Bessel series
   Hahn–Exton -Bessel function
   Hankel transform
   Incomplete Bessel functions
   Jackson -Bessel function
   Kelvin functions
   Kontorovich–Lebedev transform
   Lentz's algorithm
   Lerche–Newberger sum rule
   Lommel function
   Lommel polynomial
   Neumann polynomial
   Schlömilch's series
   Sonine formula
   Struve function
   Vibrations of a circular membrane
   Weber function (defined at Anger function)
  
  Notes
  
  References
  
   
   Arfken, George B. and Hans J. Weber, Mathematical Methods for Physicists, 6th edition (Harcourt: San Diego, 2005). .
   Bowman, Frank Introduction to Bessel Functions (Dover: New York, 1958). .
   
   .
   .
   B Spain, M. G. Smith, Functions of mathematical physics, Van Nostrand Reinhold Company, London, 1970. Chapter 9 deals with Bessel functions.
   N. M. Temme, Special Functions. An Introduction to the Classical Functions of Mathematical Physics, John Wiley and Sons, Inc., New York, 1996. . Chapter 9 deals with Bessel functions.
   Watson, G. N., A Treatise on the Theory of Bessel Functions, Second Edition'', (1995) Cambridge University Press. .
   .
  
  External links
  
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   Wolfram function pages on Bessel J and Y functions, and modified Bessel I and K functions. Pages include formulas, function evaluators, and plotting calculators.
   
   Bessel functions Jν, Yν, Iν and Kν in Librow Function handbook.
  F. W. J. Olver, L. C. Maximon, Bessel Functions (chapter 10 of the Digital Library of Mathematical Functions).
  
  Special hypergeometric functions
  Fourier analysis