ANISOTROPIC SPACE DYNAMICS · OPEN RESEARCH

OP-SD-003 · Stable Nonlinear Topology

Competition between positive second- and fourth-gradient energies and a nonnegative volume potential gives a unique positive stationary R_* with positive radial second derivative. The fourth-order mechanism resisting collapse is analytic. The scale parameters of Chapters 4 and 5 are reciprocal, so powers must be compared using their definitions.

Based on the final manuscript · 第四、五章

TheoryTheory · OPENReviewMathematical review · INCOMPLETEEvidenceEvidence · UNTESTEDCanonicalNoStatus, review and sources
OP-SD-003 · P1

NEEDS THEORY · Needs theory

PDETopology
Discuss this task

01Established results

Competition between positive second- and fourth-gradient energies and a nonnegative volume potential gives a unique positive stationary R_* with positive radial second derivative. The fourth-order mechanism resisting collapse is analytic. The scale parameters of Chapters 4 and 5 are reciprocal, so powers must be compared using their definitions.

ASD-WEB-SD-031
EQ=∫[A22∑i∥Li∥2+A44∑i<j∥[Li,Lj]∥2+W(Q,χ)]d3x,Li=Q−1∂iQE_Q=\int\left[\frac{A_2}{2}\sum_i\|L_i\|^2+\frac{A_4}{4}\sum_{i<j}\|[L_i,L_j]\|^2+W(Q,\chi)\right]d^3x,\quad L_i=Q^{-1}\partial_iQ

Constitutive input
A2,A4>0 and norm squared=Tr(X†X)/2; existence and the full stable spectrum remain open.
Chapter reference: Ch. 4 (4.21) · ASD-BOOK-ddbade997b45

ASD-WEB-SD-032
Qλ(x)=Q(x/λ),E(λ)=λE2+λ−1E4+λ3EV,E2−E4+3EV=0(λ=1),E(R)=A2R+A4/R+A0R3,E′(R)=A2−A4/R2+3A0R2,R∗2=A22+12A0A4−A26A0(A0>0),=2A4A2+A22+12A0A4(A0≥0),R∗2=A4/A2(A0=0),E′′(R∗)=2A4R∗3+6A0R∗>0.\begin{aligned}Q_\lambda(\mathbf x)&=Q(\mathbf x/\lambda),\\E(\lambda)&=\lambda E_2+\lambda^{-1}E_4+\lambda^3E_V,\\E_2-E_4+3E_V&=0\quad(\lambda=1),\\E(R)&=A_2R+A_4/R+A_0R^3,\\E'(R)&=A_2-A_4/R^2+3A_0R^2,\\R_*^2&=\frac{\sqrt{A_2^2+12A_0A_4}-A_2}{6A_0}\quad(A_0>0),\\&=\frac{2A_4}{A_2+\sqrt{A_2^2+12A_0A_4}}\quad(A_0\ge0),\\R_*^2&=A_4/A_2\quad(A_0=0),\\E''(R_*)&=\frac{2A_4}{R_*^3}+6A_0R_*>0.\end{aligned}

Mathematical result
Retains Chapter 4’s convention that increasing λ enlarges the profile; R is a physical length. A₂,A₄>0, A₀≥0. The 6A₀ denominator requires A₀>0; the rationalized expression includes A₀=0. Units: A₂ J/m, A₄ J·m, A₀ J/m³. The analytic radial minimum is not a complete three-dimensional solution or full perturbation stability.
Chapter reference: Ch. 4 (4.20)–(4.22); Ch. 5 (5.6.23)–(5.6.25) · ASD-BOOK-ddbade997b45

02Research still required

With one target space, vacuum and boundary, construct the full three-dimensional finite-energy solution and compute a Hessian or periodic-background Floquet spectrum. Check fission, radiation, zero modes and amplitude-zero paths before mapping topology to particle properties.

03The next reproducible deliverable

First reproduce the analytic radius and A_0→0 limit, then deliver a field solution and nonradial spectrum with equation residuals and boundary/grid convergence; state exactly which perturbations beyond radial curvature were tested.

04Scope and research links

The one-parameter scale model solves its radial extremum problem: this must neither be called an absence of an analytic scale nor enlarged into a complete electron/proton stability proof.

stability · master equation · electron solution · master equation · space dynamics · electron solution

On this page
STATUS & REVIEW
Theory StatusTheory · OPEN
Mathematical ReviewMathematical review · INCOMPLETE
Overall Evidence StatusEvidence · UNTESTEDConstraints and proposals are recorded separately; no new experimental fit.
Canonical ASDNo · Research notesContinuum foundation; status specified per claim
Adopted source, conditions and previous versions

第四章式(4.20)—(4.22);第五章式(5.6.21)—(5.6.25)

已得结果、继续研究任务与下一份交付;保留原问题 ID、优先级及状态。

Conditions retained in this adoption

  • The one-parameter scale model solves its radial extremum problem: this must neither be called an absence of an analytic scale nor enlarged into a complete electron/proton stability proof.

Source locators: p1374 · p1375 · p2275 · p2281 · p2282

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

Download source identity manifest

The manifest identifies the source; it is not the complete manuscript. Adopting this source does not upgrade evidence or grant a new licence.

Previous source, retained as history

SD-51779505a476 · Ch. 4 §4.1; Ch. 5 §§4, 6

CH4-9587f3c44d39 · 第四章-ASD空间本体论-出版整理稿.docx
9587f3c44d3974f44e387ed03d92691fa5473a90d7b1c9c989155adf0622849a

CH5-ca737ec4e327 · 第五章-出版整理稿.docx
ca737ec4e327d72c5507bbc8e00295b6e56029c7583ebad8e505cdb9c68c6262

RELATIONSHIP INDEX

Position within the framework

These links index inputs and research relationships. The completion status of each derivation is specified in its text. Untranslated supporting pages open in Chinese.

RESEARCH LEDGER

Revision history

SOURCE & SCOPE

第四、五章 · 第四章式(4.20)—(4.22);第五章式(5.6.21)—(5.6.25)

This research task is based on the cited final Chinese manuscript. It is not a new canonical result. Both languages use the same source snapshot; original equation numbers and website IDs remain distinct.

Knowledge scope
CITATION & SOURCE FILE

ASD: OP-SD-003 · Stable Nonlinear Topology. OP-SD-003-EN. Version 1.0.0; 2026-10-24. https://asd-physics.org/en/open-problems/space-dynamics/stable-topology. 第四章式(4.20)—(4.22);第五章式(5.6.21)—(5.6.25). Source ASD-BOOK-ddbade997b45.

Discuss this page Download this page as MDX
CONTINUE RESEARCH

Continue with the assumptions, equations and sources.

These links carry this page and its source version into the research workspace. Each request pins its knowledge snapshot. Model availability is shown in the workspace; retrieval and private export remain available.