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Lemma 3.11 — Liouville's formula (Abel's identity) for the Wronski determinant

Proved
TeschlODE.Linear.liouville_formula

by mikedeng1 · Sep 28, 2026 · Mathlib 0df444a (Lean v4.33.1)

linear-systemsliouville-formulaordinary-differential-equationsp2o-batch-books5p2o-gran-per-chapterp2o-plan-bookp2o-v1wronskian

Let III be an interval, A∈C(I,Rn×n)A \in C(I, \mathbb{R}^{n\times n})A∈C(I,Rn×n), and let U(t)=(φ1(t),…,φn(t))U(t) = (\varphi_1(t), \dots, \varphi_n(t))U(t)=(φ1​(t),…,φn​(t)) be a matrix whose columns are solutions of x˙=A(t)x\dot x = A(t)xx˙=A(t)x on III. Then the Wronski determinant W(t)=det⁡U(t)W(t) = \det U(t)W(t)=detU(t) satisfies

W(t)=W(t0) exp⁡(∫t0ttr⁡(A(s)) ds),t0,t∈I.(3.91)W(t) = W(t_0)\,\exp\Big(\int_{t_0}^{t} \operatorname{tr}(A(s))\,ds\Big), \qquad t_0, t \in I. \qquad (3.91)W(t)=W(t0​)exp(∫t0​t​tr(A(s))ds),t0​,t∈I.(3.91)

In particular det⁡U(t)≠0\det U(t) \neq 0detU(t)=0 at one point of III implies it at every point, and for periodic AAA the determinant of the monodromy matrix is exp⁡(∫0Ttr⁡A)>0\exp\big(\int_0^T \operatorname{tr} A\big) > 0exp(∫0T​trA)>0 (3.122), which is what makes a matrix logarithm of it available in Floquet's theorem.

Formalization Note. The book writes UUU with the solutions as columns ("using the solutions as columns", (3.81)); the Lean hypothesis is that each column fun t i => U t i j is an IsSolution A I. The integral is the interval integral ∫ s in t₀..t, which is oriented (so t<t0t < t_0t<t0​ is allowed) and is a genuine integral because tr⁡A\operatorname{tr} AtrA is continuous on [t0,t]⊆I[t_0,t] \subseteq I[t0​,t]⊆I.

Preamble
import Mathlib
import Definitions.Def_TeschlODE_Linear_IsSolution
Formal statement
namespace TeschlODE.Linear

/-- Teschl, Lemma 3.11 (p. 83), Abel's identity / Liouville's formula (3.91): if the columns of
`U(t)` are `n` solutions of (3.79) on the interval `I`, the Wronski determinant
`W(t) = det U(t)` satisfies `W(t) = W(t₀) exp (∫_{t₀}^{t} tr A(s) ds)` for all `t₀, t ∈ I`. -/
theorem liouville_formula {n : ℕ} (A : ℝ → Matrix (Fin n) (Fin n) ℝ) (I : Set ℝ)
    (hI : I.OrdConnected) (hA : ContinuousOn A I) (U : ℝ → Matrix (Fin n) (Fin n) ℝ)
    (hU : ∀ j : Fin n, IsSolution A I (fun t i => U t i j)) (t₀ t : ℝ) (ht₀ : t₀ ∈ I)
    (ht : t ∈ I) :
    (U t).det = (U t₀).det * Real.exp (∫ s in t₀..t, (A s).trace) := by sorry

end TeschlODE.Linear
Source
Teschl, Ordinary Differential Equations and Dynamical Systems (author's preliminary version of AMS GSM 140, 2012), p. 83, Lemma 3.11
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What the Lean code literally says, in plain math · claude-opus-5-5

Setting. Let n∈Nn \in \mathbb{N}n∈N, let A:R→Rn×nA : \mathbb{R} \to \mathbb{R}^{n\times n}A:R→Rn×n, and let I⊆RI \subseteq \mathbb{R}I⊆R. The theorem assumes:

  • III is order-connected (an interval of any kind);
  • AAA is continuous on III;
  • U:R→Rn×nU : \mathbb{R} \to \mathbb{R}^{n\times n}U:R→Rn×n is a matrix-valued function whose every column is a solution on III. For each column index jjj, the vector function
t↦(U(t)1j,…,U(t)nj)t \mapsto \bigl(U(t)_{1j}, \dots, U(t)_{nj}\bigr)t↦(U(t)1j​,…,U(t)nj​)

has, at every t∈It \in It∈I, derivative A(t)A(t)A(t) times that column relative to III. (Limits are taken only along points of III, so the derivative is one-sided at an endpoint in III.)

  • t0t_0t0​ and ttt are two points of III.

Claim.

det⁡U(t)=det⁡U(t0)⋅exp⁡ ⁣(∫t0ttr⁡A(s) ds).\det U(t) = \det U(t_0)\cdot \exp\!\left(\int_{t_0}^{t} \operatorname{tr} A(s)\,ds\right).detU(t)=detU(t0​)⋅exp(∫t0​t​trA(s)ds).

Here tr⁡\operatorname{tr}tr is the sum of the diagonal entries. The integral is the oriented Lebesgue integral: over (t0,t](t_0, t](t0​,t] if t0≤tt_0 \le tt0​≤t, and minus the integral over (t,t0](t, t_0](t,t0​] if t<t0t < t_0t<t0​. Because III is order-connected, the segment between t0t_0t0​ and ttt lies in III, where AAA is continuous. No linear independence of the columns of UUU is assumed; det⁡U\det UdetU may be zero.

Degenerate cases.

  • t=t0t = t_0t=t0​: the integral is 000, and the claim reads det⁡U(t0)=det⁡U(t0)\det U(t_0) = \det U(t_0)detU(t0​)=detU(t0​).
  • III a single point: only t=t0t = t_0t=t0​ is possible.
  • n=0n = 0n=0: the determinant of the empty matrix is 111 and its trace is 000, so the claim reads 1=1⋅e01 = 1\cdot e^01=1⋅e0.
  • Non-integrable integrand: if tr⁡A\operatorname{tr}AtrA were not integrable on the segment, the integral would be taken to be 000 by convention. Under the continuity hypothesis on the compact segment, however, it is integrable.
Human review
  • Endorsed by Shuze Chen · Oct 2, 2026

    Confirmed by the moderator at approval.

  • Endorsed by mikedeng1 · Oct 2, 2026

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

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