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Homogeneous convex model of a level with positive ambient Hessian

Proved
HryniewiczCriterion.exists_homogeneous_convex_model

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

contact-geometryhamiltonian-dynamicssymplectic-geometry

Let H:R4→RH:\mathbb{R}^4\to\mathbb{R}H:R4→R be smooth with strictly star-shaped unit level S=H−1(1)S=H^{-1}(1)S=H−1(1), and assume the Hessian of HHH is positive definite on all of R4\mathbb{R}^4R4 at every point of SSS. Then there is a function KKK with the same unit level which is a homogeneous convex model: KKK is smooth on R4∖{0}\mathbb{R}^4\setminus\{0\}R4∖{0}, positively homogeneous of degree two (K(rx)=r2K(x)K(rx)=r^2K(x)K(rx)=r2K(x) for r>0r>0r>0), positive away from the origin, and its Hessian is positive definite on all vectors at every point of SSS.

Moreover, for every periodic orbit PPP of XHX_HXH​ on SSS (prime or multiply covered) with normalized variational flow YYY, there are a periodic orbit QQQ of XKX_KXK​ and a normalized variational flow ZZZ along it such that the contact-plane paths of (H,P,Y)(H,P,Y)(H,P,Y) and (K,Q,Z)(K,Q,Z)(K,Q,Z) in the global frame Z1,Z2Z_1,Z_2Z1​,Z2​ have the same winding interval.

This is the normalization step of HWZ (3.31)–(3.32), where KKK is the square of the Minkowski functional of the domain bounded by SSS. It lets the index estimate be proved for degree-two homogeneous Hamiltonians only, for which the linearized flow has an invariant splitting.

Preamble
import Definitions.Def_HryniewiczCriterion_GraphAngle

open HryniewiczCriterion
open scoped ContDiff
Formal statement
theorem HryniewiczCriterion.exists_homogeneous_convex_model (H : R4 → ℝ) (hS : IsStrictlyStarShapedLevel H)
    (hpos : ∀ x : R4, H x = 1 → ∀ v : R4, v ≠ 0 → 0 < fderiv ℝ (fderiv ℝ H) x v v) :
    ∃ K : R4 → ℝ, IsHomogeneousConvexModel K ∧ energySurface K = energySurface H ∧
      ∀ (P : PeriodicOrbit H) (Y : ℝ → (R4 →L[ℝ] R4)), IsLinearizedFlow H P.x Y →
        ∃ (Q : PeriodicOrbit K) (Z : ℝ → (R4 →L[ℝ] R4)), IsLinearizedFlow K Q.x Z ∧
          windingInterval (linearizedXiPath K Q Z) = windingInterval (linearizedXiPath H P Y) := 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, (3.31)–(3.32) and Lemma 3.5, pp. 219–220; contact path convention of Hryniewicz, https://arxiv.org/html/1105.2077v5, Section 2.1.1, equations (4)–(5). Reduction lemma isolating the choice of the homogeneous defining function; not a verbatim numbered assertion.

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