The Gauss linking integral is multiplied by when the second loop is traversed times
ProvedHryniewiczCriterion.gaussLinkingIntegral_comp_mul_natdynamical-systemsgeometry-topologysymplectic-geometry
Let be disjoint loops of period , and let miss both. For every ,
Here is gaussLinkingIntegral, the Gauss double integral after stereographic projection from . The integrand is linear in the velocity of the second loop, so substituting turns into . By periodicity this is copies of . For both sides vanish, because the second loop is constant.
Preamble
import Definitions.Def_HryniewiczCriterion_GlobalSection import Definitions.Def_HryniewiczCriterion_SelfLinking open HryniewiczCriterion
Formal statement
theorem HryniewiczCriterion.gaussLinkingIntegral_comp_mul_nat (N : R4) (γ₁ γ₂ : ℝ → R4)
(h₁ : ContDiff ℝ 2 γ₁) (h₂ : ContDiff ℝ 2 γ₂)
(hper₁ : ∀ s, γ₁ (s + 1) = γ₁ s) (hper₂ : ∀ s, γ₂ (s + 1) = γ₂ s)
(hunit₁ : ∀ s, euclidNorm (γ₁ s) = 1) (hunit₂ : ∀ s, euclidNorm (γ₂ s) = 1)
(hdisj : ∀ s t, γ₁ s ≠ γ₂ t) (hN : euclidNorm N = 1) (hNγ : ∀ s, γ₁ s ≠ N ∧ γ₂ s ≠ N)
(k : ℕ) :
gaussLinkingIntegral N γ₁ (fun t => γ₂ (k * t)) = k * gaussLinkingIntegral N γ₁ γ₂ := by sorrySource
Elementary (change of variables in the Gauss linking integral); used for multiply covered orbits in U. Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, J. Symplectic Geom. 12 (2014) 791-862, arXiv:1105.2077, Definition 1.5 and Lemma 3.12.