AbstractWe study the large‐time asymptotics for solutionsu(x,t) of the wave equation with Dirichlet boundary data, generated by a time‐harmonic force distribution of frequency ω, in a class of domains with non‐compact boundaries and show that the results obtained in 11 for a special class of local perturbations of Ω0≔ ℝ2× (0,1) can be extended to arbitrary smooth local perturbations Ω of Ω0. In particular, we prove thatuis bounded ast→ ∞ if Ω does not allow admissible standing waves of frequency ω in the sense of 8. This implies in connection with 8. Theorem 3.1 that the logarithmic resonances of the unperturbed domain Ω0at the frequencies ω = πk(k= 1, 2,…) observed in 14 can be simultaneously removed by small perturbations of the boundary. As a main step of our analysis, the determination of admissible solutions of the boundary value problem ΔU+ κ2U= −fin Ω,U= 0 on ∂Ω is reduc
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