Recovering a potential in damped wave equation from Neumann-to-Dirichlet operator
Recovering a potential in damped wave equation from Neumann-to-Dirichlet operator
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从诺依曼到狄利克雷算子恢复阻尼波动方程中的势
DOI:
10.1088/1361-6420/abb8e8
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发表时间:
2020
期刊:
影响因子:
2.1
通讯作者:
A. Hasanov
中科院分区:
文献类型:
--
作者:
V. Romanov;A. Hasanov
The inverse coefficient problem of recovering the potential q(x) in the damped wave equation m(x)utt+μ(x)ut=r(x)uxx+q(x)u , (x, t) ∈ Ω T ≔ (0, ℓ) × (0, T) subject to the boundary conditions r(0)u x (0, t) = f(t), u(ℓ, t) = 0, from the Dirichlet boundary measured output ν(t) ≔ u(0, t), t ∈ (0, T] is studied. A detailed microlocal analysis of regularity of the direct problem solution in the subdomains defined by the characteristics as well as along these characteristics is provided. Based on this analysis, necessary regularity results and energy estimates are derived. It is proved that the Dirichlet boundary measured output uniquely determines the potential q(x) in the interval [0, h(T/2)] and this solution belongs to C(0, h(T/2)) with T < T*, where h(z) is the root of the equation z=∫0h(z)m(x)/r(x)dx , T*=2∫0ℓm(x)/r(x)dx . Moreover, the global uniqueness theorem is proved. Compactness, invertibility and Lipschitz continuity of the Neumann-to-Dirichlet operator Φf[⋅]:Q⊂C(0,ℓ)↦L2(0,T) , Φ f [q](t) ≔ u(0, t; q) is proved. This allows us to prove an existence of a quasi-solution of the inverse problem defined as a minimum of the Tikhonov functional J(q)≔(1/2)‖Φf[⋅]−ν‖L2(0,T)2 as well as its Fréchet differentiability. An explicit formula for the Fréchet gradient is derived by making use of the unique solution to corresponding adjoint problem. The proposed approach is leads to very effective gradient based computational identification algorithm.