Mittag-Leffler function

The Mittag-Leffler function can be used to interpolate continuously between a Gaussian and a Lorentzian function.

In mathematics, the Mittag-Leffler function E_α,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:

E_{{\alpha ,\beta }}(z)=\sum _{{k=0}}^{\infty }{\frac {z^{k}}{\Gamma (\alpha k+\beta )}}.

where $\Gamma$ is the Gamma function .

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 E_α,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_{\alpha ,\beta }(z)={\frac {1}{z}}E_{\alpha ,\beta -\alpha }(z)-{\frac {1}{z\Gamma (\beta -\alpha ),}}

from which the Poincaré asymptotic expansion

E_{\alpha ,\beta }(z)\sim -\sum _{k=1}{\frac {1}{z^{k}\Gamma (\beta -k\alpha )}}

follows, which is true for $z\to -\infty$ .

Special cases

For $\alpha =0,1/2,1,2$ we find

The sum of a geometric progression:

E_{{0,1}}(z)=\sum _{{k=0}}^{\infty }z^{k}={\frac {1}{1-z}}.

Exponential function:

E_{{1,1}}(z)=\sum _{{k=0}}^{\infty }{\frac {z^{k}}{\Gamma (k+1)}}=\sum _{{k=0}}^{\infty }{\frac {z^{k}}{k!}}=\exp(z).

Error function:

E_{{1/2,1}}(z)=\exp(z^{2})\operatorname {erfc}(-z).

Hyperbolic cosine:

E_{{2,1}}(z)=\cosh({\sqrt {z}}).

For $\alpha =0,1,2$ , the integral

\int _{0}^{z}E_{\alpha ,1}(-s^{2})\,{\mathrm {d} }s

gives, respectively

\arctan(z),

{\tfrac {\sqrt {\pi }}{2}}\operatorname {erf} (z),

\sin(z).

Mittag-Leffler's integral representation

E_{{\alpha ,\beta }}(z)={\frac {1}{2\pi i}}\int _{C}{\frac {t^{{\alpha -\beta }}e^{t}}{t^{\alpha }-z}}\,dt

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

\int _{0}^{\infty }e^{-tz}t^{\beta -1}E_{\alpha ,\beta }(t^{\alpha })dt={\frac {z^{-\beta }}{1-z^{-\alpha }}}

and

\int _{0}^{\infty }e^{-tz}t^{\beta -1}E_{\alpha ,\beta }(-t^{\alpha })\,dt={\frac {z^{\alpha -\beta }}{1+z^{\alpha }}}

on the negative axis.

References

Mittag-Leffler, M.G.: Sur la nouvelle fonction E(x). C. R. Acad. Sci. Paris 137, 554–558 (1903)
Mittag-Leffler, M.G.: Sopra la funzione E˛.x/. Rend. R. Acc. Lincei, (Ser. 5) 13, 3–5 (1904)
Gorenflo R., Kilbas A.A., Mainardi F., Rogosin S.V., Mittag-Leffler Functions, Related Topics and Applications (Springer, New York, 2014) 443 pages ISBN 978-3-662-43929-6
Olver, F. W. J.; Maximon, L. C. (2010), "Mittag-Leffler function", in Olver, Frank W. J.; Lozier, Daniel M.; Boisvert, Ronald F.; Clark, Charles W., NIST Handbook of Mathematical Functions, Cambridge University Press, ISBN 978-0521192255, MR 2723248
Igor Podlubny (1998). "chapter 1". Fractional Differential Equations. An Introduction to Fractional Derivatives, Fractional Differential Equations, Some Methods of Their Solution and Some of Their Applications. Mathematics in Science and Engineering. Academic Press. ISBN 0-12-558840-2.
Kai Diethelm (2010). "chapter 4". The analysis of fractional differential equations: an application-oriented exposition using differential operators of Caputo type. Lecture Notes in Mathematics. Heidelberg and New York: Springer-Verlag. ISBN 978-3-642-14573-5.
Eric W. Weisstein, "Mittag-Leffler function, ", From MathWorld—A Wolfram Web Resource.
H. J. Haubold, A. M. Mathai, R. K. Saxena Mittag-Leffler Functions and Their Applications

External links

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Mittag-Leffler function

Special cases

Mittag-Leffler's integral representation

See also

References

External links