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Graph-angle bound for a positive symplectic path with two fixed directions

Proved
HryniewiczCriterion.positive_path_graph_angle_bound

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

contact-geometryhamiltonian-dynamicssymplectic-geometry

Let Y^:R→R4×4\hat Y:\mathbb{R}\to\mathbb{R}^{4\times4}Y^:R→R4×4 solve Y^′=J S(t) Y^\hat Y'=J\,S(t)\,\hat YY^′=JS(t)Y^, Y^(0)=I\hat Y(0)=IY^(0)=I, where S(t)S(t)S(t) is continuous and symmetric positive definite and JJJ is the standard complex structure in the coordinates (q1,p1,q2,p2)(q_1,p_1,q_2,p_2)(q1​,p1​,q2​,p2​). Suppose that at some time T>0T>0T>0 the matrix Y^(T)=diag⁡(I2,g)\hat Y(T)=\operatorname{diag}(I_2,g)Y^(T)=diag(I2​,g) fixes the first two coordinate directions.

For a symplectic matrix MMM let V(M)=W(ΓM) W(Δ)−1V(M)=W(\Gamma_M)\,W(\Delta)^{-1}V(M)=W(ΓM​)W(Δ)−1 be the graph unitary: ΓM={(z,Mz)}\Gamma_M=\{(z,Mz)\}ΓM​={(z,Mz)} is a Lagrangian in (R4⊕R4,−ω0⊕ω0)(\mathbb{R}^4\oplus\mathbb{R}^4,-\omega_0\oplus\omega_0)(R4⊕R4,−ω0​⊕ω0​), Δ=ΓI\Delta=\Gamma_IΔ=ΓI​, and W(L)=UUTW(L)=UU^{\mathsf T}W(L)=UUT for a unitary basis UUU of LLL. Let θ\thetaθ be a continuous determinant angle, det⁡V(Y^(t))=eiθ(t)\det V(\hat Y(t))=e^{i\theta(t)}detV(Y^(t))=eiθ(t) with θ(0)=0\theta(0)=0θ(0)=0. Then

θ(T)  ≥  4π+∑λang⁡(λ),\theta(T)\;\ge\;4\pi+\sum_{\lambda}\operatorname{ang}(\lambda),θ(T)≥4π+λ∑​ang(λ),

where the sum runs over the eigenvalues λ\lambdaλ (with multiplicity) of the 2×22\times22×2 graph unitary of ggg, and ang⁡(λ)∈(0,2π]\operatorname{ang}(\lambda)\in(0,2\pi]ang(λ)∈(0,2π] is the argument with ang⁡(1)=2π\operatorname{ang}(1)=2\piang(1)=2π.

This is a finite-dimensional counterpart of HWZ (3.42)–(3.43): positivity of the generator, together with the two directions fixed at time TTT, forces the graph angle of the path to exceed the minimal value allowed by its endpoint by at least 4π4\pi4π.

Preamble
import Definitions.Def_HryniewiczCriterion_GraphAngle

open HryniewiczCriterion
open scoped ContDiff
Formal statement
theorem HryniewiczCriterion.positive_path_graph_angle_bound (Ŷ S : ℝ → Matrix (Fin 4) (Fin 4) ℝ) (T : ℝ)
    (hT : 0 < T) (hSc : ∀ i j : Fin 4, Continuous fun t => S t i j) (hSpos : ∀ t, (S t).PosDef)
    (h0 : Ŷ 0 = 1)
    (hd : ∀ t : ℝ, ∀ i j : Fin 4, HasDerivAt (fun s => Ŷ s i j) ((symplJ4 * S t * Ŷ t) i j) t)
    (g : Matrix (Fin 2) (Fin 2) ℝ) (hend : Ŷ T = blockOne g) (θ : ℝ → ℝ)
    (hθ : IsDetAngleLift (fun t => graphUnitary4 (Ŷ t)) T θ) :
    4 * Real.pi + eigenAngleSum (graphUnitary2 g) ≤ θ T := 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, proof of Theorem 3.4, (3.42)–(3.43), p. 221–222, recast with the Souriau map W(L)=UUTW(L)=UU^{\mathsf T}W(L)=UUT of the Lagrangian Grassmannian (Arnold; Robbin–Salamon, The Maslov index for paths, Topology 32 (1993)). Reduction lemma; not a verbatim numbered assertion.

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