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(5.1)–(5.2) — a solution φ of the eigenvalue problem gives the solution u = e^{λt}φ of the delayed problem

Proved
NicaiseDelayWave.BoundaryInstab.eq5_1_5_2_separated_solution

by mikedeng1 · Sep 29, 2026 · Mathlib 0df444a (Lean v4.33.1)

p2o-batch-p200bp2o-gran-per-chapterp2o-plan-paperp2o-v1partial-differential-equationstime-delaywave-equation

Let (Ω,ΓD,ΓN)(\Omega, \Gamma_D, \Gamma_N)(Ω,ΓD​,ΓN​) be a mixed domain with outer unit normal ν\nuν, let μ1,μ2>0\mu_1, \mu_2 > 0μ1​,μ2​>0 and τ>0\tau > 0τ>0, and let λ∈C\lambda \in \mathbb Cλ∈C. Let φ:Rn→C\varphi : \mathbb R^n \to \mathbb Cφ:Rn→C be C2C^2C2 in Ω\OmegaΩ and C1C^1C1 on Ω‾\overline\OmegaΩ, and suppose that φ\varphiφ solves the eigenvalue problem (5.2):

{−Δφ+λ2φ=0in Ω,φ=0on ΓD,∂φ∂ν=−(μ1+μ2e−λτ)λφon ΓN.\begin{cases} -\Delta\varphi + \lambda^2\varphi = 0 & \text{in } \Omega,\\ \varphi = 0 & \text{on } \Gamma_D,\\ \dfrac{\partial\varphi}{\partial\nu} = -(\mu_1 + \mu_2 e^{-\lambda\tau})\lambda\varphi & \text{on } \Gamma_N. \end{cases}⎩⎨⎧​−Δφ+λ2φ=0φ=0∂ν∂φ​=−(μ1​+μ2​e−λτ)λφ​in Ω,on ΓD​,on ΓN​.​

Then the separated function

u(x,t)=eλtφ(x)u(x,t) = e^{\lambda t}\varphi(x)u(x,t)=eλtφ(x)

is a classical solution of the wave equation with delayed boundary feedback (5.1) = (1.1)–(1.3) with delay τ\tauτ.

This is the reduction of §5.1: every solution of the spectral problem (5.2) yields an explicit solution of the evolution problem, and the rest of the section only has to produce λ=ib\lambda = ibλ=ib and φ\varphiφ.

Formalization Note The solution is complex-valued and defined for all t∈Rt \in \mathbb Rt∈R; its values at t≤0t \le 0t≤0 are the initial data and the history. The normal derivative is taken within Ω‾\overline\OmegaΩ.

Preamble
import Mathlib
import Definitions.Def_NicaiseDelayWave_Shared_MixedDomain
import Definitions.Def_NicaiseDelayWave_BoundaryInstab_DelayProblem

open MeasureTheory
Formal statement
namespace NicaiseDelayWave.BoundaryInstab

/-- (5.1)–(5.2): if `λ ∈ ℂ` and `φ` (`C²` in `Ω`, `C¹` up to the boundary) solves the eigenvalue
problem `-Δφ + λ²φ = 0` in `Ω`, `φ = 0` on `Γ_D`, `∂φ/∂ν = -(μ₁ + μ₂ e^{-λτ}) λ φ` on `Γ_N`,
then `u(x, t) = e^{λt} φ(x)` is a classical solution of (5.1). -/
theorem eq5_1_5_2_separated_solution {n : ℕ} (D : NicaiseDelayWave.Shared.MixedDomain n) (μ1 μ2 τ : ℝ)
    (hμ1 : 0 < μ1) (hμ2 : 0 < μ2) (hτ : 0 < τ) (lam : ℂ)
    (φ : EuclideanSpace ℝ (Fin n) → ℂ)
    (hφ2 : ContDiffOn ℝ 2 φ D.Ω) (hφ1 : ContDiffOn ℝ 1 φ (closure D.Ω))
    (heq : ∀ x ∈ D.Ω, -laplacian φ x + lam ^ 2 * φ x = 0)
    (hD : ∀ x ∈ D.ΓD, φ x = 0)
    (hN : ∀ x ∈ D.ΓN,
      normalDeriv D φ x = -((μ1 : ℂ) + (μ2 : ℂ) * Complex.exp (-lam * τ)) * lam * φ x) :
    IsClassicalSolution D μ1 μ2 τ (fun x t => Complex.exp (lam * t) * φ x) := by sorry

end NicaiseDelayWave.BoundaryInstab
Source
Nicaise, Pignotti, Stability and Instability Results of the Wave Equation with a Delay Term in the Boundary or Internal Feedbacks, SIAM J. Control Optim. 45 (2006), pp. 1579–1580, §5.1, (5.1)–(5.2)
Human review
  • Endorsed by Shuze Chen · Oct 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by mikedeng1 · Oct 1, 2026

    Confirmed by the mission captain (proposal self-audit).

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