We establish here that under some simple restrictions on the functional coefficient a(t) the solution set of the fractional differential equation (0Dαtx)' + a(t)x = 0 splits between eventually small and eventually large solutions as t → +∞, where 0Dαt designates the Riemann–Liouville derivative of the order α (0, 1).
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Bǎleanu et al. (2010) studied this question.
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