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Regular D3 cylinder endpoint expansion

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QAlgorithms.Papers.Independent.Intakethird100.P58.d3_tip_expansion

by Gohan · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

In the dimensionless compactified D3 reduced model, fix an endpoint radius r0>0r_0>0r0​>0. There exists a regular cylinder profile r:[0,1]→Rr:[0,1]\to\mathbb Rr:[0,1]→R anchored at the boundary z=0z=0z=0, with r(1)=r0r(1)=r_0r(1)=r0​, satisfying the Euler–Lagrange equation of ∫rz−31+(1−z4)r′2 dz\int r z^{-3}\sqrt{1+(1-z^4)r'^2}\,dz∫rz−31+(1−z4)r′2​dz. Its regulated areas are finite and

r(z)=r0+1−z4r0+o(1−z),z→1−.r(z)=r_0+\frac{1-z}{4r_0}+o(1-z),\qquad z\to1^-.r(z)=r0​+4r0​1−z​+o(1−z),z→1−.

This supplies regular endpoint data for the shooting family. The singular joining limit r0=0r_0=0r0​=0 is excluded.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P58
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P58

open Set Filter MeasureTheory

open scoped Topology

/-- PDF p.11, (3.20)--(3.21): regular D3 cylinders exist and have the
stated endpoint expansion. The divided formula excludes the singular r0=0 limit. -/
theorem d3_tip_expansion (r0 : ℝ) (hr0 : 0 < r0) :
    ∃ r : ℝ → ℝ, IsCylinder .d3 (r 0) r ∧ r 1 = r0 ∧
      Asymptotics.IsLittleO (nhdsWithin (1 : ℝ) (Iio 1))
        (fun z => r z - r0 - (1 - z) / (4 * r0)) (fun z => 1 - z) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P58

end
Source
Topological Entanglement Entropy and Holography, arXiv:0805.1891v2, PDF p. 11, (3.20)–(3.21)
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every real r0>0r_0>0r0​>0, there exists a function r:R→Rr:\mathbb R\to\mathbb Rr:R→R with r(1)=r0r(1)=r_0r(1)=r0​ satisfying the following conditions: r(0)>0r(0)>0r(0)>0, rrr is continuous and strictly decreasing on [0,1][0,1][0,1], rrr is twice continuously differentiable at every point of [0,1][0,1][0,1] as a function on R\mathbb RR, and for every z∈(0,1)z\in(0,1)z∈(0,1),

r(z)>0,ddu(r(u)(1−u4)r′(u)u31+(1−u4)r′(u)2)∣u=z=1+(1−z4)r′(z)2z3.r(z)>0,\qquad \left.\frac{d}{du} \left( \frac{r(u)(1-u^4)r'(u)} {u^3\sqrt{1+(1-u^4)r'(u)^2}} \right)\right|_{u=z} = \frac{\sqrt{1+(1-z^4)r'(z)^2}}{z^3}.r(z)>0,dud​(u31+(1−u4)r′(u)2​r(u)(1−u4)r′(u)​)​u=z​=z31+(1−z4)r′(z)2​​.

For every real aaa with 0<a<10<a<10<a<1, the function

z⟼r(z)z31+(1−z4)r′(z)2z\longmapsto \frac{r(z)}{z^3}\sqrt{1+(1-z^4)r'(z)^2}z⟼z3r(z)​1+(1−z4)r′(z)2​

is Lebesgue interval-integrable from aaa to 111. This function rrr also satisfies

r(z)−r0−1−z4r0=o(1−z)(z→1−),r(z)-r_0-\frac{1-z}{4r_0}=o(1-z) \qquad(z\to1^-),r(z)−r0​−4r0​1−z​=o(1−z)(z→1−),

meaning that the absolute value of the displayed remainder divided by ∣1−z∣|1-z|∣1−z∣ tends to 000.

Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Nov 1, 2026

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

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