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The L² estimate for the Cauchy–Riemann operator on a disc

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DbarRegularity.dbar_l2_estimate

by Mazecto · Oct 11, 2026 · Mathlib 0df444a (Lean v4.33.1)

calderon-zygmundcauchy-riemannelliptic-regularityharmonic-analysissingular-integrals

Write z=s+itz=s+itz=s+it for z∈Cz\in\mathbb{C}z∈C, φs=∂φ/∂s\varphi_s=\partial\varphi/\partial sφs​=∂φ/∂s, φt=∂φ/∂t\varphi_t=\partial\varphi/\partial tφt​=∂φ/∂t and ∂ˉφ=φs+iφt\bar\partial\varphi=\varphi_s+i\varphi_t∂ˉφ=φs​+iφt​. Cn\mathbb{C}^nCn carries the Hermitian norm, and ∥⋅∥Lp\|\cdot\|_{L^p}∥⋅∥Lp​ is the LpL^pLp norm on C\mathbb{C}C with respect to Lebesgue measure. Let R>0R>0R>0 and let φ:C→Cn\varphi:\mathbb{C}\to\mathbb{C}^nφ:C→Cn be smooth with compact support in the open disc BR(0)B_R(0)BR​(0). Then

∥φs∥L22+∥φt∥L22+∥φ∥L22≤(4R2+1) ∥∂ˉφ∥L22.\|\varphi_s\|_{L^2}^2+\|\varphi_t\|_{L^2}^2+\|\varphi\|_{L^2}^2\le(4R^2+1)\,\|\bar\partial\varphi\|_{L^2}^2 .∥φs​∥L22​+∥φt​∥L22​+∥φ∥L22​≤(4R2+1)∥∂ˉφ∥L22​.

Formalization Note ContDiff ℝ ∞ φ is C∞C^\inftyC∞ smoothness over R\mathbb{R}R (not analyticity). φs\varphi_sφs​ and φt\varphi_tφt​ are fderiv ℝ φ z 1 and fderiv ℝ φ z Complex.I, and ∂ˉφ\bar\partial\varphi∂ˉφ is dbar φ. Cn\mathbb{C}^nCn is EuclideanSpace ℂ (Fin n). "Compact support in BR(0)B_R(0)BR​(0)" is tsupport φ ⊆ ball 0 R. The squared norms are the Bochner integrals ∫ z, ‖·‖ ^ 2.

Retired (2026-10-12). As formalized, the three integrals on the left nest (∫ z, (A + ∫ w, (B + ∫ u, C))), so the statement is weaker than intended. The corrected statement is DbarRegularity.dbar_l2_bound.

Preamble
import Definitions.Def_DbarRegularity_Setting
import Mathlib.Analysis.Calculus.ContDiff.Basic
Formal statement
namespace DbarRegularity

open MeasureTheory Metric Filter Topology
open scoped ENNReal NNReal ContDiff

/-- Abbas–Hofer, *Holomorphic Curves and Global Questions in Contact Geometry*, § 4.2, Theorem 4.2.1
(p. 101): for a smooth `φ : ℂ → ℂⁿ` with compact support in the open disc `B_R(0)`,
`‖φ_s‖²_{L²} + ‖φ_t‖²_{L²} + ‖φ‖²_{L²} ≤ (4R² + 1) ‖∂̄φ‖²_{L²}`, where `z = s + i t`. -/
theorem dbar_l2_estimate {n : ℕ} (R : ℝ) (φ : ℂ → EuclideanSpace ℂ (Fin n))
    (hφ : ContDiff ℝ ∞ φ) (hsupp : tsupport φ ⊆ ball 0 R) :
    ∫ z, ‖fderiv ℝ φ z 1‖ ^ 2 + ∫ z, ‖fderiv ℝ φ z Complex.I‖ ^ 2 + ∫ z, ‖φ z‖ ^ 2
      ≤ (4 * R ^ 2 + 1) * ∫ z, ‖dbar φ z‖ ^ 2 := by sorry

end DbarRegularity
Source
C. Abbas, H. Hofer, Holomorphic Curves and Global Questions in Contact Geometry, Birkhäuser Advanced Texts Basler Lehrbücher, Birkhäuser (2019), https://doi.org/10.1007/978-3-030-11803-7, § 4.2, Theorem 4.2.1, p. 101
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What the Lean code literally says, in plain math · claude-opus-5-5

Read-back: DbarRegularity.dbar_l2_estimate

Setting. n∈Nn\in\mathbb Nn∈N, R∈RR\in\mathbb RR∈R, φ:C→Cn\varphi:\mathbb C\to\mathbb C^nφ:C→Cn, z=s+itz=s+itz=s+it, Lebesgue measure on C\mathbb CC.

Hypotheses. φ∈C∞\varphi\in C^\inftyφ∈C∞ over R\mathbb RR, and tsupport⁡φ\operatorname{tsupport}\varphitsupportφ (the closure of {φ≠0}\{\varphi\ne0\}{φ=0}) is contained in the open disc BR(0)B_R(0)BR​(0). There is no hypothesis on the sign of RRR.

Definitions used. φs\varphi_sφs​ = fderiv ℝ φ z 1, φt\varphi_tφt​ = fderiv ℝ φ z Complex.I, ∂ˉφ=φs+iφt\bar\partial\varphi=\varphi_s+i\varphi_t∂ˉφ=φs​+iφt​ (dbar).

Conclusion.

∫∣φs∣2+∫∣φt∣2+∫∣φ∣2≤(4R2+1)∫∣∂ˉφ∣2.\int|\varphi_s|^2+\int|\varphi_t|^2+\int|\varphi|^2\le(4R^2+1)\int|\bar\partial\varphi|^2 .∫∣φs​∣2+∫∣φt​∣2+∫∣φ∣2≤(4R2+1)∫∣∂ˉφ∣2.

Degenerate cases. If R≤0R\le0R≤0, the disc is empty, so φ≡0\varphi\equiv0φ≡0 and the inequality reads 0≤00\le00≤0. This is harmless. n=0n=0n=0 is trivial.

Soundness checks.

  1. Lean defaults. ∞ means C∞C^\inftyC∞, not analytic (see the ContDiff scoped notation), so the statement is not vacuous. Since tsupport⁡φ\operatorname{tsupport}\varphitsupportφ is closed and contained in a bounded set in C\mathbb CC, it is compact. All integrands are therefore continuous with compact support and integrable, and no Bochner integral defaults to 0. Directional derivatives along 111 and iii are ∂s\partial_s∂s​ and ∂t\partial_t∂t​. There is no rpow, toReal or ℕ subtraction, and the constant 4R2+14R^2+14R2+1 is a finite real.
  2. There is no existential constant; the explicit constant depends only on RRR. The statement is true. By the L2L^2L2 identity, ∫∣φs∣2+∫∣φt∣2=∫∣∂ˉφ∣2\int|\varphi_s|^2+\int|\varphi_t|^2=\int|\bar\partial\varphi|^2∫∣φs​∣2+∫∣φt​∣2=∫∣∂ˉφ∣2. The Poincaré inequality on a disc (or on an interval of length 2R2R2R in sss) gives ∫∣φ∣2≤cR2∫∣∇φ∣2\int|\varphi|^2\le c R^2\int|\nabla\varphi|^2∫∣φ∣2≤cR2∫∣∇φ∣2 with c=(2/π)2≤4c=(2/\pi)^2\le4c=(2/π)2≤4, so ∫∣φ∣2≤4R2∫∣∂ˉφ∣2\int|\varphi|^2\le4R^2\int|\bar\partial\varphi|^2∫∣φ∣2≤4R2∫∣∂ˉφ∣2.

Remarks. The support condition uses tsupport, which is stronger than "support in the closed disc" and matches "compact support inside the open disc".

Verdict: no mis-formalization observed

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