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Mittag Leffler function

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In mathematics, the Mittag-Leffler function Eα,β is a special function, a complex function which depends on two complex parameters α and β. It may be defined by the following series when the real part of α is strictly positive:

Contents

E α , β ( z ) = k = 0 z k Γ ( α k + β ) .

In the case α and β are real and positive, the series converges for all values of the argument z, so the Mittag-Leffler function is an entire function. This function is named after Gösta Mittag-Leffler. This class of functions are important in the theory of the fractional calculus.

For α > 0, the Mittag-Leffler function Eα,1 is an entire function of order 1/α, and is in some sense the simplest entire function of its order.

The Mittag-Leffler function satisfies the recurrence property

E α , β ( z ) = 1 z E α , β α ( z ) 1 z Γ ( β α ) ,

from which the Poincaré asymptotic expansion

E α , β ( z ) k = 1 1 z k Γ ( β k α )

follows, which is true for z .

Special cases

For α = 0 , 1 / 2 , 1 , 2 we find

The sum of a geometric progression:

E 0 , 1 ( z ) = k = 0 z k = 1 1 z .

Exponential function:

E 1 , 1 ( z ) = k = 0 z k Γ ( k + 1 ) = k = 0 z k k ! = exp ( z ) .

Error function:

E 1 / 2 , 1 ( z ) = exp ( z 2 ) erfc ( z ) .

Hyperbolic cosine:

E 2 , 1 ( z ) = cosh ( z ) .

For α = 0 , 1 , 2 , the integral

0 z E α , 1 ( s 2 ) d s

gives, respectively

arctan ( z ) , π 2 erf ( z ) , sin ( z ) .

Mittag-Leffler's integral representation

E α , β ( z ) = 1 2 π i C t α β e t t α z d t

where the contour C starts and ends at −∞ and circles around the singularities and branch points of the integrand.

Related to the Laplace transform and Mittag-Leffler summation is the expression

0 e t z t β 1 E α , β ( t α ) d t = z β 1 z α

and

0 e t z t β 1 E α , β ( t α ) d t = z α β 1 + z α

on the negative axis.

References

Mittag-Leffler function Wikipedia


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