Journal
INTEGRAL TRANSFORMS AND SPECIAL FUNCTIONS
Volume 17, Issue 9, Pages 637-652Publisher
TAYLOR & FRANCIS LTD
DOI: 10.1080/10652460600725341
Keywords
special functions of mathematical physics; fractional calculus; generalized Mittag-Leffler functions; numerical algorithms
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The generalized Mittag-Leffler function E-alpha,E-beta (z) has been studied for arbitrary complex argument z is an element of C and parameters alpha is an element of R+ and beta is an element of R. This function plays a fundamental role in the theory of fractional differential equations and numerous applications in physics. The Mittag-Leffler function interpolates smoothly between exponential and algebraic functional behaviour. A numerical algorithm for its evaluation has been developed. The algorithm is based on integral representations and exponential asymptotics. Results of extensive numerical calculations for E-alpha,E-beta (z) in the complex z -plane are reported here. We find that all complex zeros emerge from the point z =1 for small alpha. They diverge towards -infinity+(2 k -1)pi i for alpha -> 1(-) and towards -infinity+2 k pi i for alpha -> 1(+) ( k is an element of Z). All the complex zeros collapse pairwise onto the negative real axis for alpha -> 2. We introduce and study also the inverse generalized Mittag-Leffler function L-alpha,L-beta (z) defined as the solution of the equation L-alpha,L-beta (E-alpha,E-beta (z )) = z . We determine its principal branch numerically.
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