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§5.2, p. 1584 — the standard energy of e^{λt}φ(x) is e^{2 Re(λ) t} times a positive constant

Proved
NicaiseDelayWave.InternalInstab.separated_solution_energy

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

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

Let (Ω,ΓD,ΓN)(\Omega, \Gamma_D, \Gamma_N)(Ω,ΓD​,ΓN​) be a mixed domain, let φ:Rn→C\varphi : \mathbb R^n \to \mathbb Cφ:Rn→C be C1C^1C1 on Ω‾\overline\OmegaΩ and not identically zero on Ω\OmegaΩ, and let λ∈C\lambda \in \mathbb Cλ∈C, λ≠0\lambda \neq 0λ=0. Let E(t)\mathcal E(t)E(t) be the standard energy of u(x,t)=eλtφ(x)u(x,t) = e^{\lambda t}\varphi(x)u(x,t)=eλtφ(x),

E(t)=12∫Ω{∣ut(x,t)∣2+∣∇u(x,t)∣2} dx.\mathcal E(t) = \frac12\int_\Omega \Big\{ |u_t(x,t)|^2 + |\nabla u(x,t)|^2 \Big\}\,dx .E(t)=21​∫Ω​{∣ut​(x,t)∣2+∣∇u(x,t)∣2}dx.

Then E(0)>0\mathcal E(0) > 0E(0)>0 and

E(t)=e2 Re(λ) t E(0)for all t∈R.\mathcal E(t) = e^{2\,\mathrm{Re}(\lambda)\, t}\,\mathcal E(0) \qquad \text{for all } t \in \mathbb R .E(t)=e2Re(λ)tE(0)for all t∈R.

In particular the energy is constant and strictly positive when Re λ=0\mathrm{Re}\,\lambda = 0Reλ=0 (Case (a) of §5.2), and it does not tend to 000 when Re λ≥0\mathrm{Re}\,\lambda \ge 0Reλ≥0 (Case (b)). This is the last step of the instability argument.

Formalization Note The paper's "eα+iβφ(x)e^{\alpha+i\beta}\varphi(x)eα+iβφ(x)" (p. 1584) is a misprint for e(α+iβ)tφ(x)e^{(\alpha+i\beta)t}\varphi(x)e(α+iβ)tφ(x). The identity holds for every λ\lambdaλ; the hypothesis λ≠0\lambda \neq 0λ=0 is only needed for E(0)>0\mathcal E(0) > 0E(0)>0 (for λ=0\lambda = 0λ=0 a nonzero constant φ\varphiφ has zero energy).

Preamble
import Mathlib
import Definitions.Def_NicaiseDelayWave_InternalInstab_DelayProblem
Formal statement
namespace NicaiseDelayWave.InternalInstab

/-- Nicaise–Pignotti, §5.2, p. 1584: the standard energy of a separated solution
`u(x, t) = e^{λt} φ(x)` equals `e^{2 Re(λ) t}` times its (strictly positive) value at `t = 0`;
in particular it is constant when `Re λ = 0` (Case (a)) and does not decay when `Re λ ≥ 0`. -/
theorem separated_solution_energy {n : ℕ} (D : NicaiseDelayWave.Shared.MixedDomain n)
    (φ : EuclideanSpace ℝ (Fin n) → ℂ) (hφ₁ : ContDiffOn ℝ 1 φ (closure D.Ω))
    (hφ_ne : ∃ x ∈ D.Ω, φ x ≠ 0) (lam : ℂ) (hlam : lam ≠ 0) :
    0 < stdEnergy D (fun x t => Complex.exp (lam * t) * φ x) 0 ∧
      ∀ t : ℝ, stdEnergy D (fun x t => Complex.exp (lam * t) * φ x) t
        = Real.exp (2 * lam.re * t) * stdEnergy D (fun x t => Complex.exp (lam * t) * φ x) 0 := by sorry

end NicaiseDelayWave.InternalInstab
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), p. 1584, §5.2 ("whose energy is constant and strictly positive"; "Since α ≥ 0, the energy of such a solution is not decaying to zero")
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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