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Monotonicity: pseudoholomorphic maps through the center of a small ball have energy at least c r2c\,r^2cr2

Proved
FiniteEnergyPlane.energy_ge_of_mapsTo_ball

by Mazecto · Oct 20, 2026 · Mathlib 0df444a (Lean v4.33.1)

finite-energypseudoholomorphic-curvesreeb-dynamicssymplectic-geometrysymplectization

Let EEE be a finite-dimensional real normed space, JJJ a smooth almost complex structure on an open set O⊆EO\subseteq EO⊆E, and K⊆OK\subseteq OK⊆O compact. There are r0>0r_0>0r0​>0 and c>0c>0c>0 with the following property. Let p∈Kp\in Kp∈K, 0<r≤r00<r\le r_00<r≤r0​, let U⊆CU\subseteq\mathbb{C}U⊆C be open and let uuu be C∞C^\inftyC∞ and JJJ-holomorphic on UUU, with u(U)⊆Br(p)u(U)\subseteq B_r(p)u(U)⊆Br​(p), u:U→Br(p)u:U\to B_r(p)u:U→Br​(p) proper, and p∈u(U)p\in u(U)p∈u(U). Then

∫U∥Du(z)∥2 dz ≥ c r2.\int_U\|Du(z)\|^2\,dz\ \ge\ c\,r^2.∫U​∥Du(z)∥2dz ≥ cr2.

Formalization Note Br(p)B_r(p)Br​(p) is the open ball of the norm of EEE and ∥Du(z)∥\|Du(z)\|∥Du(z)∥ is the operator norm of the real derivative C→E\mathbb{C}\to EC→E. Properness is: U∩u−1(L)U\cap u^{-1}(L)U∩u−1(L) is compact for every compact L⊆Br(p)L\subseteq B_r(p)L⊆Br​(p). Zinger states the lower bound for a compact Riemann surface with boundary whose boundary avoids a metric ball of a JJJ-compatible metric, with an explicit constant; here the constant ccc is unspecified.

Preamble
import Definitions.Def_FiniteEnergyPlane_Setting
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Monotonicity lemma: Zinger, *Notes on J-holomorphic maps*, Proposition 3.12 (local form);
Gromov 1985; quoted in Wendl, p. 152. Let `J` be a smooth almost complex structure on an open set
`O ⊆ E` and `K ⊆ O` compact. There are `r₀ > 0` and `c > 0` such that for every `p ∈ K` and
`0 < r ≤ r₀`, every smooth `J`-holomorphic map `u` on an open set `U ⊆ ℂ` that maps `U` properly
into the ball `B_r(p)` and passes through `p` has Dirichlet energy `∫_U ‖Du‖² ≥ c r²`.
(Zinger: a compact Riemann surface with boundary whose boundary image avoids a metric ball
`B_ρ(x)` of a `J`-compatible metric `g`, energy `E_g`, and the explicit bound
`ord_x u · ρ² / (1 + C(x) ρ)⁴`. Here: an open `U ⊆ ℂ` with a proper map into a norm ball of `E`,
the operator-norm Dirichlet energy, and an unspecified constant `c`.) -/
theorem energy_ge_of_mapsTo_ball {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] (J : E → E →L[ℝ] E) (O : Set E)
    (hJ : JHolomorphic.IsAlmostComplexOn J O) (K : Set E) (hK : IsCompact K) (hKO : K ⊆ O) :
    ∃ r₀ : ℝ, 0 < r₀ ∧ ∃ c : ℝ, 0 < c ∧ ∀ p ∈ K, ∀ r : ℝ, 0 < r → r ≤ r₀ →
      ∀ U : Set ℂ, IsOpen U → ∀ u : ℂ → E, ContDiffOn ℝ ∞ u U →
        JHolomorphic.IsJHolomorphicOn J U u → Set.MapsTo u U (ball p r) →
        (∀ L : Set E, IsCompact L → L ⊆ ball p r → IsCompact (U ∩ u ⁻¹' L)) → p ∈ u '' U →
        ENNReal.ofReal (c * r ^ 2) ≤ ∫⁻ z in U, ENNReal.ofReal (‖fderiv ℝ u z‖ ^ 2) := by
  sorry

end FiniteEnergyPlane
Source
A. Zinger, Notes on J-holomorphic maps, arXiv:1706.00331, Proposition 3.12; C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, https://arxiv.org/abs/1612.01009, p. 152
Read-back

What the Lean code literally says, in plain math · claude-opus-5-5

Read-back: FiniteEnergyPlane.energy_ge_of_mapsTo_ball

Data. Let EEE be a finite-dimensional real normed vector space (any norm; the norm is not assumed to come from an inner product). Let J:E→L(E)J : E \to \mathcal L(E)J:E→L(E) assign to each point x∈Ex \in Ex∈E a continuous R\mathbb RR-linear map Jx:E→EJ_x : E \to EJx​:E→E, and let O⊆EO \subseteq EO⊆E. The hypothesis on (J,O)(J, O)(J,O) ("almost complex on OOO") is:

  • OOO is open,
  • x↦Jxx \mapsto J_xx↦Jx​ is C∞C^\inftyC∞ on OOO (as a map into the normed space of operators),
  • Jx∘Jx=−idEJ_x \circ J_x = -\mathrm{id}_EJx​∘Jx​=−idE​ for every x∈Ox \in Ox∈O.

Nothing is assumed about JxJ_xJx​ for x∉Ox \notin Ox∈/O. Let K⊆EK \subseteq EK⊆E be compact with K⊆OK \subseteq OK⊆O.

Conclusion. There exist constants r0>0r_0 > 0r0​>0 and c>0c > 0c>0 (depending only on EEE with its norm, JJJ, OOO, KKK) such that the following holds for every point p∈Kp \in Kp∈K, every radius rrr with 0<r≤r00 < r \le r_00<r≤r0​, every open set U⊆CU \subseteq \mathbb CU⊆C and every map u:C→Eu : \mathbb C \to Eu:C→E satisfying all of:

  1. uuu is C∞C^\inftyC∞ on UUU (as a map of the real vector space C≅R2\mathbb C \cong \mathbb R^2C≅R2);
  2. uuu is JJJ-holomorphic on UUU: for every z∈Uz \in Uz∈U, uuu is real-differentiable at zzz and
∂su(z)+Ju(z) ∂tu(z)=0,\partial_s u(z) + J_{u(z)}\,\partial_t u(z) = 0,∂s​u(z)+Ju(z)​∂t​u(z)=0,

where ∂su(z)=Du(z)⋅1\partial_s u(z) = Du(z)\cdot 1∂s​u(z)=Du(z)⋅1 and ∂tu(z)=Du(z)⋅i\partial_t u(z) = Du(z)\cdot i∂t​u(z)=Du(z)⋅i (here JJJ is evaluated at u(z)u(z)u(z), whether or not u(z)∈Ou(z) \in Ou(z)∈O); 3. u(U)⊆B(p,r)u(U) \subseteq B(p, r)u(U)⊆B(p,r), the open ball of radius rrr about ppp in the norm of EEE; 4. for every compact L⊆EL \subseteq EL⊆E with L⊆B(p,r)L \subseteq B(p,r)L⊆B(p,r), the set U∩u−1(L)U \cap u^{-1}(L)U∩u−1(L) is compact; 5. p∈u(U)p \in u(U)p∈u(U), i.e. p=u(z)p = u(z)p=u(z) for some z∈Uz \in Uz∈U;

then

c r2  ≤  ∫U∥Du(z)∥2 dz,c\,r^2 \;\le\; \int_U \|Du(z)\|^2 \, dz ,cr2≤∫U​∥Du(z)∥2dz,

where the integral is the Lebesgue integral over UUU with respect to Lebesgue (area) measure on C\mathbb CC, taken in [0,∞][0, \infty][0,∞] (so the inequality also holds trivially if the right side is +∞+\infty+∞), and ∥Du(z)∥\|Du(z)\|∥Du(z)∥ is the operator norm of the real derivative Du(z):C→EDu(z) : \mathbb C \to EDu(z):C→E, with C\mathbb CC normed by the modulus and EEE by its given norm. (The derivative is taken in the ordinary sense on C\mathbb CC; at points of UUU it exists by hypothesis 2.)

Remarks on edge cases. The ball B(p,r)B(p,r)B(p,r) is not required to lie in OOO; only p∈K⊆Op \in K \subseteq Op∈K⊆O. If OOO (hence KKK) is empty, the condition on all p∈Kp \in Kp∈K is vacuous and the statement reduces to the existence of some positive r0,cr_0, cr0​,c. If EEE has odd positive dimension, Jx2=−idJ_x^2 = -\mathrm{id}Jx2​=−id is impossible, so OOO and KKK must be empty and the statement is vacuous in the same way. If E={0}E = \{0\}E={0}, the condition Jx2=−idJ_x^2 = -\mathrm{id}Jx2​=−id holds trivially; in that case hypotheses 3–5 force UUU to be a nonempty open set with U=U∩u−1({p})U = U \cap u^{-1}(\{p\})U=U∩u−1({p}) compact, which cannot occur, so the conclusion is vacuous for every UUU, uuu. Hypotheses 4 and 5 together exclude U=∅U = \emptysetU=∅.

Human review
  • Endorsed by Shuze Chen · Oct 21, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Mazecto · Oct 21, 2026

    Confirmed by the mission captain (proposal self-audit).

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