ANISOTROPIC SPACE DYNAMICS · OPEN RESEARCH

OP-QM-004 · Dynamical Origin of Born Statistics

A linearly driven detector’s mean absorbed power is proportional to the envelope modulus squared. Fixed energy per event and negligible leakage, dead time and saturation give an event rate and a conditional position distribution after time/thickness integration. The manuscript also supplies phase-flow equivariance and a nonlinear detector-response expansion. These are established results within their stated conditions.

Based on the final manuscript · 第五章

TheoryTheory · OPENReviewMathematical review · INCOMPLETEEvidenceEvidence · UNTESTEDCanonicalNoStatus, review and sources
OP-QM-004 · P0

NEEDS THEORY · Needs theory

Quantum foundationsStatistical inferencePDE
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01Established results

A linearly driven detector’s mean absorbed power is proportional to the envelope modulus squared. Fixed energy per event and negligible leakage, dead time and saturation give an event rate and a conditional position distribution after time/thickness integration. The manuscript also supplies phase-flow equivariance and a nonlinear detector-response expansion. These are established results within their stated conditions.

ASD-WEB-QM-026
P‾D=gD2ω02Im⁡χD(ω0)∣Ψ∣2,RD≃P‾D/εD\overline P_D=\frac{g_D^2\omega_0}{2}\operatorname{Im}\chi_D(\omega_0)|\Psi|^2,\qquad R_D\simeq\overline P_D/\varepsilon_D

Mathematical result
The first follows from near-monochromatic average work after subtracting independent noise; the second additionally requires fixed absorbed energy per event and negligible leakage, dead time and saturation.
Chapter reference: Ch. 5 (5.3.19) and following text · ASD-BOOK-ddbade997b45

ASD-WEB-QM-027
R(r,t)=ηD(r,t)∣Ψ∣2,RA=∫thicknessR dz,p(Y∣det)=∫TRA(Y,t)dt∫dA∫TRA(Y,t)dt\mathcal R(\mathbf r,t)=\eta_D(\mathbf r,t)|\Psi|^2,\quad\mathcal R_A=\int_{\rm thickness}\mathcal R\,dz,\quad p(Y\mid\mathrm{det})=\frac{\int_{\mathcal T}\mathcal R_A(Y,t)dt}{\int dA\int_{\mathcal T}\mathcal R_A(Y,t)dt}

Mathematical result
Nonzero total detection rate with stated efficiency, thickness and time window. For normal-flux sampling jn=vn|Ψ|²; normalized squared modulus also requires constant or cancelling vn across compared positions.
Chapter reference: Ch. 5 (5.3.20)–(5.3.21) · ASD-BOOK-ddbade997b45

02Research still required

Build nonlinear competition dynamics for the core, accompanying field and detector array to obtain one record per excitation. Test relaxation toward a Born-type distribution from independently specified initial ensembles, retaining efficiency, normal-flux weighting, time windows and noise calibration.

03The next reproducible deliverable

First deliver a complete response model, conservation accounting, event definition and calibration for one detector. Provide a proof, numerical result or counterexample for single-record exclusivity and initial-state convergence, without using the target probability as a preset sampling rule.

04Scope and research links

Equivariance preserves an already matched initial ensemble; it does not prove convergence from arbitrary ensembles. Uniform efficiency alone also does not remove a varying normal-flow velocity from the count distribution.

detection statistics · master equation · detection statistics · electron solution · master equation · quantum

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STATUS & REVIEW
Theory StatusTheory · OPEN
Mathematical ReviewMathematical review · INCOMPLETE
Overall Evidence StatusEvidence · UNTESTEDNOT YET UNIQUELY TESTED · known wave phenomena are requirements; an independent ASD source and universal event statistics remain open.
Canonical ASDNo · Research notesCanonical research framework · effective limits are conditional
Adopted source, conditions and previous versions

第五章 §3.3—§3.4 式(5.3.11)—(5.3.22);§7

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

  • Equivariance preserves an already matched initial ensemble; it does not prove convergence from arbitrary ensembles. Uniform efficiency alone also does not remove a varying normal-flow velocity from the count distribution.

Specific unresolved source issues

  • 式(5.3.21)后的通量归一化需保留法向速度权重;相同速度条件方可约去

Source locators: p1943 · p1945 · p1954 · p1955 · p1959 · p1963 · p2305

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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Previous source, retained as history

QM-0accdcbe7725 · Ch. 5 §§3.3–3.4

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

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第五章 · 第五章 §3.3—§3.4 式(5.3.11)—(5.3.22);§7

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CITATION & SOURCE FILE

ASD: OP-QM-004 · Dynamical Origin of Born Statistics. OP-QM-004-EN. Version 1.0.0; 2026-10-24. https://asd-physics.org/en/open-problems/quantum/born-statistics. 第五章 §3.3—§3.4 式(5.3.11)—(5.3.22);§7. Source ASD-BOOK-ddbade997b45.

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