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OP-00696 Solution claimed

Optimal uniform observation time for mixed finite element waves

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Fix a bounded measurable potential $a : [0,1] \to [0,\infty)$, with its pointwise values specified. For $N \ge 1$ put $h = 1/(N+1)$ and let $$M_h = \frac h4 \operatorname{tridiag}(1,2,1), \qquad K_h = \frac1h \operatorname{tridiag}(-1,2,-1), \qquad L_h = h \operatorname{diag}\bigl(a(h), \dots, a(Nh)\bigr),$$ all of size $N \times N$: the mixed finite element semi-discretisation of Castro and Micu of the wave equation $u'' - u_{xx} + a u = 0$ on $(0,1)$ with homogeneous Dirichlet conditions. For solutions $U = (u_1, \dots, u_N)^T$ of $M_h \ddot U + (K_h + L_h) U = 0$ with initial data $(U^0, U^1)$ let $$\mathcal{E}_h(U^0, U^1) = (U^0)^* (K_h + L_h) U^0 + (U^1)^* M_h U^1, \qquad \mathcal{O}_{h,T}(U) = \int_0^T \Bigl( \Bigl|\frac{u_1(t)}{h}\Bigr|^2 + \Bigl|\frac{\dot u_1(t)}{2}\Bigr|^2 \Bigr) dt,$$ and $$T_*(a) = \inf\bigl\{ T > 0 : \exists\, c(a,T) > 0 \ \forall N \ge 1 \ \forall (U^0, U^1),\ \mathcal{O}_{h,T}(U) \ge c(a,T)\, \mathcal{E}_h(U^0, U^1) \bigr\},$$ the constant being independent of the mesh. For the wave equation itself, $\int_0^T |u_x(t,0)|^2\, dt$ is bounded below by a constant times the energy of the initial data for every $T > 2$. Castro and Micu proved that $T_*(a)$ is finite: there are $T_0, \kappa_0 > 0$ independent of $h$ such that the inequality holds with $c = \kappa_0$ for every $T > T_0$.

Problem. Determine $T_*(a)$. In particular, is $T_*(a) = 2$ for every such potential?

Source: Castro and Micu (2025), after Theorem 1, who call the optimal value of the uniform observation time an open problem. Stated by AIM — Open Applied Problems as the question whether it equals 2.

Imported from github.com/MColbrook/AIM.

Classification

Primary
NA — Numerical Analysis
Secondary
AP, OC
Keywords
AIM Open Applied Problems, boundary observability, mixed finite elements, wave equation

References

@article{castro2025,
  author        = {Castro, Carlos and Micu, Sorin},
  title         = {A mixed finite elements approximation of inverse source problems for the wave equation with variable coefficients using observability},
  journal       = {Numer. Math.},
  volume        = {157},
  number        = {5},
  year          = {2025},
  pages         = {1847--1895},
  doi           = {10.1007/s00211-025-01489-0},
  eprint        = {2501.11352},
  archivePrefix = {arXiv},
}
@misc{aim-mixed-wave-optimal-observation-time,
  author       = {Brunton, Steve and Colbrook, Matthew J. and de Hoop, Maarten V. and Stepaniants, George and Townsend, Alex and Ward, Rachel},
  title        = {{Optimal uniform observation time for mixed finite element waves}},
  howpublished = {AIM --- Open Applied Problems, GitHub repository},
  year         = {2026},
  url          = {https://github.com/MColbrook/AIM/blob/1b7c7fd251c1643bb41f0e3cef38704bcef410fd/problems/605-mixed-wave-optimal-observation-time.md},
  note         = {Entry 605 at commit 1b7c7fd, 2026-10-13},
}

Resolution claims

Marcus Webb

T_*(a) = 2 for every bounded measurable a >= 0: uniform observability holds for every T > 2 and fails for every T < 2..

Full resolution · not verified · fidelity not established · posted on GitHub 2 Oct 2026

Status history

WhenChangeByReason
2026-10-16 Needs verification → Solution claimed — Recorded here: AIM @ a153f46, 606-mixed-wave-observation/PROOF.md.

Citing this problem

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OP-00696, "Optimal uniform observation time for mixed finite element waves", clopen.solutions.