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§5.2 Case (a), μ1 = μ2 — the system (5.25) forces α = 0 and β² = Λ²

Proved
NicaiseDelayWave.InternalInstab.case_a_equal_coefficients

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

delay-equationsp2o-batch-p200bp2o-gran-per-chapterp2o-plan-paperp2o-v1real-analysis

Let μ>0\mu > 0μ>0 and τ>0\tau > 0τ>0, and let α,β,Λ∈R\alpha, \beta, \Lambda \in \mathbb Rα,β,Λ∈R satisfy system (5.25) with μ1=μ2=μ\mu_1 = \mu_2 = \muμ1​=μ2​=μ:

α2+β2=Λ2,μe−ατ=2α+μ.\alpha^2 + \beta^2 = \Lambda^2, \qquad \mu e^{-\alpha\tau} = 2\alpha + \mu .α2+β2=Λ2,μe−ατ=2α+μ.

Then

α=0andβ2=Λ2.\alpha = 0 \qquad\text{and}\qquad \beta^2 = \Lambda^2 .α=0andβ2=Λ2.

In the borderline case μ1=μ2\mu_1 = \mu_2μ1​=μ2​ the roots of (5.23) produced by (5.24) are purely imaginary, λ=iβ\lambda = i\betaλ=iβ with β2=Λ2\beta^2 = \Lambda^2β2=Λ2; the corresponding solutions eiβtφ(x)e^{i\beta t}\varphi(x)eiβtφ(x) have constant energy, and the delays are τn,l=(2l+1)π/βn\tau_{n,l} = (2l+1)\pi/\beta_nτn,l​=(2l+1)π/βn​.

Preamble
import Mathlib
Formal statement
namespace NicaiseDelayWave.InternalInstab

/-- Nicaise–Pignotti, §5.2, pp. 1583–1584, Case (a): if `μ₁ = μ₂ = μ > 0` and `τ > 0`, the real
system (5.25) forces `α = 0` and `β² = Λ²`. -/
theorem case_a_equal_coefficients (μ τ α β Λ : ℝ) (hμ : 0 < μ) (hτ : 0 < τ)
    (h₁ : α ^ 2 + β ^ 2 = Λ ^ 2) (h₂ : μ * Real.exp (-α * τ) = 2 * α + μ) :
    α = 0 ∧ β ^ 2 = Λ ^ 2 := 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), pp. 1583–1584, §5.2, Case (a)
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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