Abstract

We consider a time-fractional diffusion equation for an inverse problem to determine an unknown source term, whereby the input data is obtained at a certain time. In general, the inverse problems are ill-posed in the sense of Hadamard. Therefore, in this study, we propose a mollification regularization method to solve this problem. In the theoretical results, the error estimate between the exact and regularized solutions is given by a priori and a posteriori parameter choice rules. Besides, the proposed regularized methods have been verified by a numerical experiment.

Highlights

  • In this work, we study an inverse source problem for the time-fractional diffusion equation in a infinite domain as follows: β∂ u( x, t) = u xx ( x, t) + φ(t) f ( x ), ( x, t) ∈ R × (0, T ], ∂t β (1)u( x, 0) = 0, x ∈ R, u( x, T ) = g( x ), x ∈ R, where the fractional derivative ∂β u∂t β is the Caputo derivative of order β (0 < β < 1) as defined by d β f (t) = Γ (1 − β ) dt β Zt d f (s) ds, ds (t − s) β (2)

  • To our knowledge, in the case φ(t), dependent on time, the results of the inverse source problem for the time-fractional diffusion equation still has a limited achievement, if φ(t) 6= 0, we know Huy and his group investigated this problem by way of the Tikhonov regularization method, see Reference [13]

  • In the theoretical results, which we have shown, we obtained the error estimates of both a priori and a posteriori parameter choice rule methods based on a priori condition

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Summary

Introduction

We study an inverse source problem for the time-fractional diffusion equation in a infinite domain as follows: β. To our knowledge, in the case φ(t), dependent on time, the results of the inverse source problem for the time-fractional diffusion equation still has a limited achievement, if φ(t) 6= 0, we know Huy and his group investigated this problem by way of the Tikhonov regularization method, see Reference [13]. In these regularization methods, the priori parameter choice rule depends on the noise level and the priori bound.

Some Auxiliary Results
The Priori Parameter Choice
The Discrepancy Principle
Numerical Experiments
Conclusions
Full Text
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