2017
DOI: 10.1007/s00033-017-0801-0
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On a fractional reaction–diffusion equation

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Cited by 31 publications
(30 citation statements)
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“…Indeed, applying D α to both sides of the equation in (27), one obtains the equation in (1), and evaluating the equation in (27) at t = 0, one gets u t (0, x) = 0. Problem (27) has been recently studied in [3,13]. In space dimension n = 1 it was first studied by Y. Fujita [22].…”
Section: 4mentioning
confidence: 99%
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“…Indeed, applying D α to both sides of the equation in (27), one obtains the equation in (1), and evaluating the equation in (27) at t = 0, one gets u t (0, x) = 0. Problem (27) has been recently studied in [3,13]. In space dimension n = 1 it was first studied by Y. Fujita [22].…”
Section: 4mentioning
confidence: 99%
“…This problem, that represents the heat conductor model with memory [26,40], was originally studied by Y. Fujita [22] for n = 1 (see also [45]). Fujita's method produces an handle representation of solution via multiplier operators and it have been used to study (1) in several directions, see [2,3,13,28].…”
Section: Introductionmentioning
confidence: 99%
“…Numerical solutions of the alternative representation of such direct problem have been studied in [35,36,33,32]. In contrast, the problem of recovering the function u at previous time t ∈ [0, T ) as in (1) is called the backward problem. This kind of equation arises in practical situations in which the initial density of the diffusing substance is not available and we can only measure the density at positive time.…”
Section: Introductionmentioning
confidence: 99%
“…Motivated by the above, in this paper, we study problem (1) and aim to provide an approximate solution. In reality, it is impossible to get the exact final data ϕ and we only have the noisy physical measurement ϕ.…”
Section: Introductionmentioning
confidence: 99%
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