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Reported shrinking oscillations of the D4 shooting families

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QAlgorithms.Papers.Independent.Intakethird100.P58.d4_branch_oscillations

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

prove2quantum

For the physical D4 reduced equation there exist regular disk profiles indexed by their axis depth s∈(0,1)s\in(0,1)s∈(0,1), with boundary radii ρD(s)\rho_D(s)ρD​(s), and regular cylinder profiles indexed by their endpoint radii t>0t>0t>0, with boundary radii ρC(t)\rho_C(t)ρC​(t). The radius functions are continuous on their parameter intervals. The numerical study reported in the source finds a common finite ρc>0\rho_c>0ρc​>0 with

ρD(s)⟶ρc(s→1−),ρC(t)⟶ρc(t→0+),\rho_D(s)\longrightarrow\rho_c\quad(s\to1^-),\qquad \rho_C(t)\longrightarrow\rho_c\quad(t\to0^+),ρD​(s)⟶ρc​(s→1−),ρC​(t)⟶ρc​(t→0+),

and both radius functions take values strictly above and strictly below ρc\rho_cρc​ in every punctured neighborhood of their limiting parameter.

Finite limiting radius together with these repeated crossings is the qualitative diminishing-envelope interpretation of the reported oscillations. No decay rate, exact critical decimal, or exhaustive count of solutions at a prescribed radius is asserted.

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 pp.17--18: the reported numerical shrinking oscillations of the D4
shooting families. This records a qualitative numerical finding of the source,
not a certified rate or an assertion of exactly two solutions at a fixed radius. -/
theorem d4_branch_oscillations :
    ∃ (R : ℝ → ℝ) (D C : ℝ → ℝ → ℝ) (critical : ℝ),
      0 < critical ∧
      (∀ s ∈ Ioo (0 : ℝ) 1, IsDisk .d4 (R s) s (D s)) ∧
      (∀ t : ℝ, 0 < t → IsCylinder .d4 (C t 0) (C t) ∧ C t 1 = t) ∧
      ContinuousOn R (Ioo (0 : ℝ) 1) ∧
      ContinuousOn (fun t => C t 0) (Ioi (0 : ℝ)) ∧
      ShrinkingOscillations R (Ioo 0 1) 1 critical ∧
      ShrinkingOscillations (fun t => C t 0) (Ioi 0) 0 critical := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P58

end
Source
Topological Entanglement Entropy and Holography, arXiv:0805.1891v2, PDF p. 17, §4.1, Figs.8–9
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What the Lean code literally says, in plain math · gpt-6.1-sol

There exist functions R:R→RR:\mathbb R\to\mathbb RR:R→R and D,C:R→R→RD,C:\mathbb R\to\mathbb R\to\mathbb RD,C:R→R→R, and a real number q>0q>0q>0, with the following properties. To specify their required profile conditions, say that a function p:R→Rp:\mathbb R\to\mathbb Rp:R→R satisfies the regular conditions with parameters A,b∈RA,b\in\mathbb RA,b∈R when A>0A>0A>0, b>0b>0b>0, p(0)=Ap(0)=Ap(0)=A, ppp is continuous and strictly decreasing on [0,b][0,b][0,b], ppp is twice continuously differentiable at every point of [0,b)[0,b)[0,b) as a function on R\mathbb RR, and for every z∈(0,b)z\in(0,b)z∈(0,b),

p(z)>0,ddu(p(u)2u(1−u3)p′(u)u31+u(1−u3)p′(u)2)∣u=z=2p(z)z31+z(1−z3)p′(z)2,p(z)>0,\qquad \left.\frac{d}{du} \left( \frac{p(u)^2u(1-u^3)p'(u)} {u^3\sqrt{1+u(1-u^3)p'(u)^2}} \right)\right|_{u=z} = \frac{2p(z)}{z^3}\sqrt{1+z(1-z^3)p'(z)^2},p(z)>0,dud​(u31+u(1−u3)p′(u)2​p(u)2u(1−u3)p′(u)​)​u=z​=z32p(z)​1+z(1−z3)p′(z)2​,

and, for every real aaa with 0<a<b0<a<b0<a<b, the function z↦p(z)21+z(1−z3)p′(z)2/z3z\mapsto p(z)^2\sqrt{1+z(1-z^3)p'(z)^2}/z^3z↦p(z)21+z(1−z3)p′(z)2​/z3 is Lebesgue interval-integrable from aaa to bbb. For every s∈(0,1)s\in(0,1)s∈(0,1), the function ds(z)=D(s,z)d_s(z)=D(s,z)ds​(z)=D(s,z) satisfies these regular conditions with A=R(s)A=R(s)A=R(s) and b=sb=sb=s, has ds(s)=0d_s(s)=0ds​(s)=0, and its function

Hs(v)=inf⁡{z∈[0,s]:ds(z)=v},H_s(v)=\inf\{z\in[0,s]:d_s(z)=v\},Hs​(v)=inf{z∈[0,s]:ds​(z)=v},

assigned value 000 when the set is empty, is twice continuously differentiable within [0,R(s))[0,R(s))[0,R(s)) and has derivative 000 at 000 within [0,∞)[0,\infty)[0,∞). For every real t>0t>0t>0, the function ct(z)=C(t,z)c_t(z)=C(t,z)ct​(z)=C(t,z) satisfies the regular conditions with A=C(t,0)A=C(t,0)A=C(t,0) and b=1b=1b=1, has ct(1)=t>0c_t(1)=t>0ct​(1)=t>0, and is twice continuously differentiable at 111 as a function on R\mathbb RR. Furthermore, RRR is continuous on (0,1)(0,1)(0,1), the function t↦C(t,0)t\mapsto C(t,0)t↦C(t,0) is continuous on (0,∞)(0,\infty)(0,∞), and

lim⁡s→1−R(s)=q,lim⁡t→0+C(t,0)=q.\lim_{s\to1^-}R(s)=q, \qquad \lim_{t\to0^+}C(t,0)=q.s→1−lim​R(s)=q,t→0+lim​C(t,0)=q.

For every real δ>0\delta>0δ>0, there are s−,s+∈(0,1)s_-,s_+\in(0,1)s−​,s+​∈(0,1) and t−,t+>0t_-,t_+>0t−​,t+​>0 satisfying

0<∣s−−1∣<δ,R(s−)<q,0<∣s+−1∣<δ,q<R(s+),0<t−<δ,C(t−,0)<q,0<t+<δ,q<C(t+,0).\begin{gathered} 0<|s_--1|<\delta,\quad R(s_-)<q,\qquad 0<|s_+-1|<\delta,\quad q<R(s_+),\\ 0<t_-<\delta,\quad C(t_-,0)<q,\qquad 0<t_+<\delta,\quad q<C(t_+,0). \end{gathered}0<∣s−​−1∣<δ,R(s−​)<q,0<∣s+​−1∣<δ,q<R(s+​),0<t−​<δ,C(t−​,0)<q,0<t+​<δ,q<C(t+​,0).​
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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