2015
DOI: 10.1515/fca-2015-0006
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Some Analytical and Numerical Properties of the Mittag-Leffler Functions

Abstract: Some analytical properties of the Mittag-Leffler functions, e α (t) ≡ E α (−t α ), are established on some t-intervals. These are lower and upper bounds obtained in terms of simple rational functions (which are related to the Padé approximants of e α (t)), for t > 0 and 0 < α < 1. A new method, to compute such functions, solving numerically a Caputo-type fractional differential equation satisfied by them, is developed. This approach consists in an adaptive predictor-corrector method, based on the K. Diethelm's… Show more

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Cited by 17 publications
(9 citation statements)
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“…In Fig.s 1 and 2, we plotted the numerical solution of (1.14) for several values of the parameters. The numerical method we used is an adaptive improvement of the predictor-corrector method earlier introduced in [7], and developed in [5]. Starting from an arbitrary discretization step, h, we chose locally a step size inversely proportional to the size of the (classical) derivative of the solution being computed, so that, at the i-th step, the time step…”
Section: Numerical Resultsmentioning
confidence: 99%
“…In Fig.s 1 and 2, we plotted the numerical solution of (1.14) for several values of the parameters. The numerical method we used is an adaptive improvement of the predictor-corrector method earlier introduced in [7], and developed in [5]. Starting from an arbitrary discretization step, h, we chose locally a step size inversely proportional to the size of the (classical) derivative of the solution being computed, so that, at the i-th step, the time step…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Mainardi's conjecture 30 : For all t > 0 and fixed α , 0 < α < 1, we have 11+anormalΓfalse(1αfalse)tαEαfalse(atαfalse)11+anormalΓfalse(1+αfalse)1tα,2.56804ptt0. has been proved later in Concezzi and Spigler 31 and in Simon 32 …”
Section: Preliminariesmentioning
confidence: 89%
“…We solve the nonhomogeneous Basset equation (29) for f(t) = sinωt and zero initial condition: y(0) = 0. For this purpose, we firstly use the Laplace transform pair, L sinωt ½ = ω s 2 + ω 2 , and the convolution theorem for the Laplace transform (12). As a result, we obtain the function y(t) defined by Equation (30) with y 0 = 0.…”
Section: Examplementioning
confidence: 99%
“…The analytical solutions of the fractional differential equations are expressed in terms of special functions. In particular, the one‐ and two‐parameter M‐L functions, the Prabhakar function, the R ‐function, and the fractional meta‐trigonometric functions appear in the solutions of fractional differential equations. The M‐L functions E α , E α , β , and Eα,βγ are defined by the power series Eα()z=k=0zknormalΓ()italicαk+1,Eα,β()z=k=0zknormalΓ()italicαk+β,Eα,βγ()z=k=0()γknormalΓ()italicαk+β0.12emzkk!, where α > 0, β > 0, γ > 0, z ∈ C , and Γ(⋅) are the Euler gamma function and ( γ ) k is the Pochhammer polynomial: ( γ ) k = γ ( γ +1)…( γ + k − 1).…”
Section: Introductionmentioning
confidence: 99%
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