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JOURNALS // Izvestiya Vysshikh Uchebnykh Zavedenii. Matematika // Archive

Izv. Vyssh. Uchebn. Zaved. Mat., 2025 Number 11, Pages 70–82 (Mi ivm10137)

Direct and inverse coefficient problems for the fractional diffusion wave equation with the Riemann–Liouville time derivative

H. H. Turdievab, M. O. Rajabovab, S. H. Xoliqovc, B. T. Karamatovc

a V.I. Romanovskiy Institute of Mathematics of the Academy of Science of the Republic of Uzbekistan, 9 University str., Tashkent, 100174, Republic of Uzbekistan
b Bukhara State University, 11 M.Ikbol str., Bukhara, 200100 Republic of Uzbekistan
c Navoi State Pedagogical Institute, 45 Ibn Sino str., Navoi, 210100 Republic of Uzbekistan

Abstract: This article considers the inverse problem in the fractional wave equation with the Riemann–Louville derivative. In this case, the direct problem is an initial nonlocal boundary value problem for this equation with initial Cauchy type and nonlocal boundary conditions. As a redefinition condition, a nonlocal integral condition with respect to the direct solution of the problem is specified. Using the Fourier method, this problem is reduced to equivalent integral equations. Then, using the Mittag-Leffler function and the generalized singular Gronwall inequality, we obtain an a priori estimate of the solution in terms of the unknown coefficient, which we will need to investigate for the inverse problem. The inverse problem is reduced to the equivalent integral of a Volterra type equation. To solve this equation, the contraction mapping principle is used. Local existence and global uniqueness have been proven.

Keywords: Fractional derivative, fractional Riemann–Liouville integral, fractional Riemann–Liouville derivative, direct problem, inverse problem, integral equation, Fourier series, Banach fixed point theorem.

UDC: 517

Received: 25.07.2024
Revised: 25.07.2024
Accepted: 26.09.2024

DOI: 10.26907/0021-3446-2025-11-70-82



© Steklov Math. Inst. of RAS, 2025