2021
DOI: 10.1016/j.amc.2021.126177
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Explicit solutions for linear variable–coefficient fractional differential equations with respect to functions

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Cited by 25 publications
(26 citation statements)
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“…-Develop the distribution theory for the estimators of H(t); -Investigate changes of the Hölder exponents depending on evolutions of random fields driven by SPDEs on the sphere, see [27,46,50,51];…”
Section: Discussionmentioning
confidence: 99%
“…-Develop the distribution theory for the estimators of H(t); -Investigate changes of the Hölder exponents depending on evolutions of random fields driven by SPDEs on the sphere, see [27,46,50,51];…”
Section: Discussionmentioning
confidence: 99%
“…Then, more details are given in [7][8][9]. Some propositions were given in the function space is C n [a, b] (see also [10,11]). However, it is not enough or convenient in numerical analysis.…”
Section: Introductionmentioning
confidence: 99%
“…where is a positive real number, g(t) is strictly increasing function on [a, b] and g(a) ≥ 0 . Due to the new features in comparison with the standard fractional derivatives, much attention has been paid to theoretical research and applications, for example, fractional calculus of variations [4], the Laplace transform [5,6], exact solution [7,8] and numerical methods [9]. Motivated by the continuous time random walk understood by means of the standard fractional calculus [10,11], suppose a long-tailed waiting time probability density function [12] which is more general than the power law function Then, one comes across a general time-fractional Fokker-Planck equation with the general fractional integral where T is the temperature, P(x, t) is the probability density function, K is the diffusion coefficient, F(x) represents external force field and k b represents the Boltzmann constant.…”
Section: Introductionmentioning
confidence: 99%