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Invariant splitting of the linearized flow of a homogeneous convex model

Proved
HryniewiczCriterion.homogeneous_frame_flow_split

by Mazecto · Oct 6, 2026 · Mathlib 0df444a (Lean v4.33.1)

contact-geometryhamiltonian-dynamicssymplectic-geometry

Let KKK be a homogeneous convex model, Q=(x,T)Q=(x,T)Q=(x,T) a periodic orbit of XKX_KXK​ on S=K−1(1)S=K^{-1}(1)S=K−1(1) and ZZZ its normalized variational flow. Let FFF be the symplectic frame of R4\mathbb{R}^4R4 at x(0)x(0)x(0) with columns x(0)x(0)x(0), XK(x(0))/ω0(x(0),XK(x(0)))X_K(x(0))/\omega_0(x(0),X_K(x(0)))XK​(x(0))/ω0​(x(0),XK​(x(0))), Z1(x(0))Z_1(x(0))Z1​(x(0)), Z2(x(0))Z_2(x(0))Z2​(x(0)), and put Y^(t)=F−1Z(t)F\hat Y(t)=F^{-1}Z(t)FY^(t)=F−1Z(t)F. Then:

  1. the contact-plane path φ\varphiφ of (K,Q,Z)(K,Q,Z)(K,Q,Z) is a smooth path in SL(2,R)SL(2,\mathbb{R})SL(2,R) on [0,1][0,1][0,1] with φ(0)=I\varphi(0)=Iφ(0)=I;
  2. Y^(0)=I\hat Y(0)=IY^(0)=I, and Y^′(t)=J S(t) Y^(t)\hat Y'(t)=J\,S(t)\,\hat Y(t)Y^′(t)=JS(t)Y^(t) for all ttt, where JJJ is the matrix with XH=J∇HX_H=J\nabla HXH​=J∇H and S(t)S(t)S(t) is continuous and symmetric positive definite (namely S(t)=FTD2K(x(t))FS(t)=F^{\mathsf T}D^2K(x(t))FS(t)=FTD2K(x(t))F);
  3. after one period, Y^(T)=diag⁡(I2,φ(1))\hat Y(T)=\operatorname{diag}(I_2,\varphi(1))Y^(T)=diag(I2​,φ(1)).

Item 3 is the invariant splitting R4=span⁡{x,XK(x)}⊕ξx\mathbb{R}^4=\operatorname{span}\{x,X_K(x)\}\oplus\xi_xR4=span{x,XK​(x)}⊕ξx​ of HWZ (3.34)–(3.36): by homogeneity the linearized flow maps x(0)x(0)x(0) to x(t)x(t)x(t) and XK(x(0))X_K(x(0))XK​(x(0)) to XK(x(t))X_K(x(t))XK​(x(t)), and it preserves ξ\xiξ.

Preamble
import Definitions.Def_HryniewiczCriterion_GraphAngle

open HryniewiczCriterion
open scoped ContDiff
Formal statement
theorem HryniewiczCriterion.homogeneous_frame_flow_split (K : R4 → ℝ) (hK : IsHomogeneousConvexModel K)
    (Q : PeriodicOrbit K) (Z : ℝ → (R4 →L[ℝ] R4)) (hZ : IsLinearizedFlow K Q.x Z) :
    (ContDiffOn ℝ ∞ (fun t i j => linearizedXiPath K Q Z t i j) (Set.Icc 0 1) ∧
      (∀ t ∈ Set.Icc (0 : ℝ) 1, (linearizedXiPath K Q Z t).det = 1) ∧
      linearizedXiPath K Q Z 0 = 1) ∧
    frameFlowMatrix K Q Z 0 = 1 ∧
    (∃ S : ℝ → Matrix (Fin 4) (Fin 4) ℝ, (∀ i j : Fin 4, Continuous fun t => S t i j) ∧
      (∀ t, (S t).PosDef) ∧
      ∀ t : ℝ, ∀ i j : Fin 4, HasDerivAt (fun s => frameFlowMatrix K Q Z s i j)
        ((symplJ4 * S t * frameFlowMatrix K Q Z t) i j) t) ∧
    frameFlowMatrix K Q Z Q.T = blockOne (linearizedXiPath K Q Z 1) := by sorry
Source
Hofer–Wysocki–Zehnder, The dynamics on three-dimensional strictly convex energy surfaces, Ann. of Math. 148 (1998), https://doi.org/10.2307/120994, Section 3, (3.33)–(3.39), pp. 220–221, with the global frame and contact path of Hryniewicz, https://arxiv.org/html/1105.2077v5, Section 2.1.1, equations (4)–(5) (frame Z1,Z2Z_1,Z_2Z1​,Z2​ of Hryniewicz §3, p. 12).

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