c ∈ (0, ∞) — scale parameter The (one-dimensional) Holtsmark distribution is a continuous probability distribution.

The Holtsmark distribution is a special case of a stable distribution with the index of stability or shape parameter

The Holtsmark distribution is one of the few examples of a stable distribution for which a closed form expression of the probability density function is known.

The Holtsmark distribution has applications in plasma physics and astrophysics.

[1] In 1919, Norwegian physicist Johan Peter Holtsmark proposed the distribution as a model for the fluctuating fields in plasma due to the motion of charged particles.

[2] It is also applicable to other types of Coulomb forces, in particular to modeling of gravitating bodies, and thus is important in astrophysics.

[3][4] The characteristic function of a symmetric stable distribution is: where

is the shape parameter, or index of stability,

also represents the median and mode of the distribution.

And since α < 2, the variance of the Holtsmark distribution is infinite.

[6] All higher moments of the distribution are also infinite.

[6] Like other stable distributions (other than the normal distribution), since the variance is infinite the dispersion in the distribution is reflected by the scale parameter, c. An alternate approach to describing the dispersion of the distribution is through fractional moments.

[6] In general, the probability density function, f(x), of a continuous probability distribution can be derived from its characteristic function by: Most stable distributions do not have a known closed form expression for their probability density functions.

Only the normal, Cauchy and Lévy distributions have known closed form expressions in terms of elementary functions.

[1] The Holtsmark distribution is one of two symmetric stable distributions to have a known closed form expression in terms of hypergeometric functions.

is equal to 0 and the scale parameter is equal to 1, the Holtsmark distribution has the probability density function: where

functions are pure imaginary complex numbers, but the sum of the two functions is real.

is related to the Bessel functions of fractional order

and its derivative to the Bessel functions of fractional order