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Big Flare-Up Theory (BFUT) · P19A · Common-Substrate Bell Test Simulator
Interactive Companion · Papers P16, P17, P18, P19, P19A

Same Predictions. Different Physical Explanation. That Is the Point.

What this simulator shows — for every reader

In 1964, John Bell proved that if two particles are completely independent from the moment they separate, the correlations between measurements on them cannot exceed a specific limit — the Bell inequality, or more precisely the CHSH bound of |S| = 2. Experiments by Clauser, Aspect, and Zeilinger (Nobel Prize 2022) showed that real quantum particles violate this bound, reaching up to S = 2√2 ≈ 2.828. This is called Bell violation.

Here is the critical point most explanations miss: BFUT and standard quantum mechanics make identical predictions about the measurement outcomes. Both predict the cosine correlation E(θ) = cos(θ) for a maximally coherent pair, and both predict Bell violation. They agree on every number. What they disagree on is the physical explanation.

Standard quantum mechanics says: the particles are entangled — measuring one instantly affects the other nonlocally. BFUT says: the particles were formed from a single shared Spaticle substrate configuration. Their correlations were built in at formation. No signal passes between them. Bell's assumption of independent local hidden variables never applies, because BFUT's shared substrate is not independent.

The contrast table below makes this explicit. The classical column shows what an independent hidden-variable theory predicts — it cannot reach Bell violation. The BFUT column shows the substrate prediction — it matches quantum mechanics exactly, for a completely different physical reason.

Papers P16 (Proton Geometry) · P17 (Force Emergence) · P18 (Gravitational Domains) · P19 (Standard Model Derivations) · P19A (Quantum Mechanics from Substrate) · Vijay Shankar Sharma · ORCID 0009-0001-9622-6121 · DOI 10.5281/zenodo.20145696
ρ_s = 5.9×10⁻²⁷ kg/m³ Spaticle field equilibrium density — the single physical constant from which all results are derived
Detector B angle b22°
Primary angle of detector B. CHSH test also uses b' = b + 45°. For maximum Bell violation set b = a + 22.5°.
Environmental noise ε0.08
Random substrate disturbance during propagation. Reduces correlation. Real experiments minimise this with cryogenic isolation.
Trials N800
Number of paired measurement events for the outcome distribution and table.
BFUT position: The pair originates from one shared Spaticle substrate configuration. Correlations exist at formation — not generated at measurement. Bell's independence assumption never applies. Same outcomes as QM. Different physical cause.
CHSH test — proper four-angle computation
CHSH score |S|
Classical limit = 2.000
E(a,b) correlation
C·I·cos(b−a)·(1−ε)
Spaticle field
EXISTS or ABSENT
Classical max |S|
Independent HV limit
The key contrast — same predictions, different physical explanation

What is "HV" (Hidden Variable)? A hidden variable theory assumes each particle carries a pre-set, self-contained instruction — a "hidden variable" — that determines how it will respond to any measurement. The particles are assumed to be completely independent of each other after separation. Bell proved mathematically that any such theory is bounded: the CHSH score can never exceed 2. Experiments consistently exceed 2. BFUT is not a hidden variable theory — the shared substrate is a physically extended, globally constrained structure, not an independent local instruction set.

QuestionClassical independent HV
(particles independent at separation)
Standard QM
(nonlocal entanglement)
BFUT
(shared Spaticle substrate)

CHSH result interpretation

Press RUN TEST to compute.

Correlation E(θ) vs angle — three predictions compared
CHSH score |S| vs substrate coherence C — classical limit vs BFUT/QM
Outcome distribution across N trials
Trial table — first 20 events
TrialA outcomeB outcomeSubstrate C·IBFUT accountStandard QM label