Action of a large circle equals the enclosed dλ-energy of a finite-energy plane
ProvedFiniteEnergyPlane.loopAction_ccwLoop_eq_dlambdaEnergyfinite-energypseudoholomorphic-curvessymplectic-geometrysymplectization
Let be a strictly star-shaped level and a smooth -compatible complex structure on , with associated almost complex structure . Let be a finite-energy -holomorphic plane and . Then the action of the counterclockwise loop equals the -energy of on the disc :
Formalization Note The left side is loopAction H u (ccwLoop R), where is the radial projection proj H onto . The right side is dlambdaEnergy H (ball 0 R) u, an element of , converted with toReal (its value is finite here).
Preamble
import Definitions.Def_FiniteEnergyPlane_Setting
Formal statement
namespace FiniteEnergyPlane
open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real
/-- Action of a circle equals the enclosed `dλ`-energy (Hofer 1993, p. 537). For a finite-energy
`J̃`-holomorphic plane `u` and `R > 0`, the action of the counterclockwise loop
`t ↦ proj(u(R e^{2π i t}))` equals the `dλ`-energy `∫_{B(0,R)} u*dλ` of `u` on the disc `B(0, R)`. -/
theorem loopAction_ccwLoop_eq_dlambdaEnergy {n : ℕ} (H : V n → ℝ)
(hH : IsStrictlyStarShapedLevel H) (J : V n → V n →L[ℝ] V n)
(hJ : IsCompatibleXiStructure H J) (u : ℂ → V n) (hu : IsFiniteEnergyCurve H J Set.univ u)
(R : ℝ) (hR : 0 < R) :
loopAction H u (ccwLoop R) = (dlambdaEnergy H (ball 0 R) u).toReal := by
sorry
end FiniteEnergyPlane
Source
H. Hofer, Pseudoholomorphic curves in symplectizations with applications to the Weinstein conjecture in dimension three, Invent. Math. 114 (1993), 515–563, proof of Theorem 31, p. 537