Paper T14D: Separate First-Passage Record Encoding under the Toner–Bacon One-Bit Communication Protocol T14C Residual-Shift Interface, Communication Calibration, and Independent 6.3-Million-Trial Hardening
Paper T14D investigates how a supplied Bell-correlated relational rule can be converted into two separately finalized detector records. The calculation uses the previously established Toner–Bacon one-bit communication protocol together with an angle and residual schedule passed from Paper T14C. Two shared random directions determine Alice’s ideal response and a one-bit message that is used in Bob’s response. Separate noisy first-passage detector processes then convert the ideal responses into records with variable finalization times, rare sign changes, finite-horizon handling, record hashing, and later trial matching. The record generator does not consult the target Bell correlation, a joint probability table, or a globally sampled outcome pair. An independent-seed hardening run generated and retained six million three hundred thousand primary records. The ideal responses produced a Bell value near the expected maximum, while the final records showed the small attenuation predicted by the measured pointer flip rates. The exact attenuation calculation reproduced the final record result to numerical precision. Communication analysis showed that the message carries one-half bit of information about a choice between orthogonal Alice settings when the shared directions are known. Removing T14C frame and state provenance did not change the generated outcomes, while removing the scheduled residual altered Bob’s response in the residual audit. Message removal and cross-trial message permutation damaged the Bell correlation, detector asymmetry produced measurable marginal bias, and no primary records were discarded. The finalized outcome marginals were consistent with the tested no-signalling equalities, although the complete protocol contains explicit communication from Alice to Bob. The result supports a communication-assisted first-passage record-encoding architecture. It does not derive the one-bit update from microscopic Holosphere dynamics, establish Bell locality, or provide a relativistically local model of spacelike measurement
Paper T14D investigates how a supplied Bell-correlated relational rule can be converted into two separately finalized detector records. The calculation uses the previously established Toner–Bacon one-bit communication protocol together with an angle and residual schedule passed from Paper T14C. Two shared random directions determine Alice’s ideal response and a one-bit message that is used in Bob’s response. Separate noisy first-passage detector processes then convert the ideal responses into records with variable finalization times, rare sign changes, finite-horizon handling, record hashing, and later trial matching. The record generator does not consult the target Bell correlation, a joint probability table, or a globally sampled outcome pair. An independent-seed hardening run generated and retained six million three hundred thousand primary records. The ideal responses produced a Bell value near the expected maximum, while the final records showed the small attenuation predicted by the measured pointer flip rates. The exact attenuation calculation reproduced the final record result to numerical precision. Communication analysis showed that the message carries one-half bit of information about a choice between orthogonal Alice settings when the shared directions are known. Removing T14C frame and state provenance did not change the generated outcomes, while removing the scheduled residual altered Bob’s response in the residual audit. Message removal and cross-trial message permutation damaged the Bell correlation, detector asymmetry produced measurable marginal bias, and no primary records were discarded. The finalized outcome marginals were consistent with the tested no-signalling equalities, although the complete protocol contains explicit communication from Alice to Bob. The result supports a communication-assisted first-passage record-encoding architecture. It does not derive the one-bit update from microscopic Holosphere dynamics, establish Bell locality, or provide a relativistically local model of spacelike measurement
Paper T21A develops a role-reversed Bell-measurement framework based on the square and triangular face axes of a cuboctahedron. The three opposite square-face axes form an orthogonal measurement family, while the four opposite triangular-face axes form a centered tetrahedral tight frame. In the square-to-triangle configuration, Alice uses the three square axes and Bob uses the four triangular axes. In the triangle-to-square configuration, the setting families are exchanged. Each twelve-correlation panel independently reconstructs a complete three-by-three correlation tensor. Under a shared calibrated bilinear model, both panels must reconstruct the same tensor. The combined twenty-four-correlation design therefore provides fifteen internal consistency conditions: three closure constraints in each panel and nine cross-panel tensor-equality constraints. The framework separates several effects that may be hidden by a single Bell score, including relative-frame rotation, isotropic visibility loss, anisotropic deformation, station-by-face response, directional detector imbalance, outcome-dependent coincidence selection, role-dependent tensor structure, and full Alice–Bob reciprocity. Uniform factorized loss remains invisible to the role-reversed tensor comparison and must be identified through singles, null outcomes, and joint-detection rates. Nonuniform response among the four triangular settings breaks tetrahedral closure, while outcome-dependent selection can alter conditioned correlations, local marginals, and apparent Bell values without implying signalling or stronger-than-quantum physics. An all-in-one standard-library computational audit verifies the geometry, tensor inverses, null-space dimension, detector identities, role-mode decomposition, and party-reciprocity relation. All forty core tests pass, including Monte Carlo validation of the declared detector models. The paper establishes a reproducible Bell-measurement microscope and a laboratory protocol that can be implemented using existing polarization-entangled photon equipment. It does not claim an observed anomaly, a new Bell bound, or a microscopic derivation of the underlying relational probability law.
Paper T2A develops a real-valued representation of Bell correlations within Holosphere Theory and identifies the assumptions responsible for the classical and quantum Bell limits. The analysis first derives the classical Clauser–Horne–Shimony–Holt bound from measurement independence, ordinary probability, and Bell-local factorization. It then represents the two-party singlet state as a normalized, nonseparable real bipartite state, with local analyzer settings described through real forms of spinor rotations and binary measurement projectors. Applying the Holosphere compatible-path or path-volume probability rule, expressed as the squared norm of the projected state, produces the standard singlet joint probabilities and the cosine correlation between analyzer directions. The optimal four-setting configuration reaches the Tsirelson value while the general real-operator analysis prevents stronger correlations within the declared binary-observable framework. Summing over either remote outcome produces locally unbiased probabilities that are independent of the remote setting, preserving operational no-signalling and preventing faster-than-light communication. The canonical model retains measurement independence and local measurement operations but does not retain outcome independence or Bell-local factorization. The paper also distinguishes exact realification from a microscopic physical derivation. It does not yet derive the singlet state, probability frequencies, detector response, decoherence, or relational persistence from fundamental Holosphere lattice dynamics. Paper T2A therefore establishes a mathematically consistent and reproducible Holosphere representation of ordinary quantum Bell correlations while leaving the specifically Holosphere physical mechanism and independent empirical confirmation as open research requirements.
Paper T14A connects finite partner selection, transported surface information, angular readout,detector response, and environmental coherence within one reduced Holosphere architecture.The source is an occupied contact organization; its three lanes are observables of a collectivemode. A controlled twelve-slot pairing problem has a unique antipodal minimum, with an explicitrobustness bound. The same source amplitudes then enter the selected pair and the local phaserecords directly. An explicitly assigned two-alternative reporting map produces a general angularlaw containing source imbalance and relative phase; its balanced, opposite-sign limit gives thefamiliar Bell correlation.The conservative response and backreaction of Paper T14 extend to four joint channels. Formatched response and a uniform fixed-total readiness preparation, first-release volumes reproducethe normalized channel inventories, with an exact no-record fraction. Environmental branchoverlap suppresses the interference component while leaving a population correlation intact. Thiscorrects a scalar visibility approximation and separates physical loss from selection of coincidentrecords. Exhaustive matching and deterministic amplitude, polytope-volume, and conservationcalculations verify the stated results without generated detection events. The remaining physicalinterface is the realization of the reporting map and joint outcome selection in an occupiedapparatus with separated readout sites.
Paper T14C studies local analyzer geometry in a controlled Holosphere surface model.Compression of the twelve-guide generator onto its first cosine and sine harmonics gives an exactreal two-by-two contrast. Its half-angle eigenvectors and winding-dependent return sign followfrom diagonalization. The harmonic plane is not dynamically invariant: the full odd mode retainsabout 97.3% of its inventory there. An explicit Schur correction recovers both the projecteddirection and omitted inventory on the stated registry grid.Local amplitude calculations distinguish carried complex phase from a real receiver-framerotation without introducing a two-site state. A reciprocal two-channel receiver has a commonloading envelope under equal couplings and opposite detunings; a common detuning offsetproduces a finite reception bias. These are local apparatus conditions, not a separated-recordmechanism.A further projection is calculated directly from the conditional triangular receiving interactionof Paper 122BF. At frozen zero contact phases its two angular modes are degenerate. A singleincoming contact couples to one bright combination and an omitted uniform mode, leaving a darkcombination. This existing contact therefore does not supply the assumed matched two-channelanalyzer. The remaining task is an occupied receiving-mode calculation with a mechanicalsetting, evolving complement, and actual records. No Bell contraction or CHSH value is a resultof this paper.
Public photon Bell-test records retain timing structure that is lost in aggregate statistics. This paper tests whether that structure survives quantitative response controls in three experimental archives. In the Weihs data, a rectangular contrast of four channel-pair timing centroids tests whether accepted signal delays can be written as a sum of local channel contributions. For longdist1, the contrast is 1.405 ns and 1.515 ns in disjoint chronological halves, with pointwise 95% block intervals [1.018, 1.791] ns and [1.193, 1.836] ns. Both survive the enumerated centroid scan under the specified 20-block inference at an 8-ns coincidence half-width and remain positive under clock, background, and gate checks. A flexible empirical timing model, however, transfers between chronological halves after clock-drift calibration. In the Christensen archive, the suppressed setting-pair channel is strongly enriched in coincidence tails, but a cross-fitted signal–accidental model predicts 714.6 of 730 counts beyond 300 ns; the residual is 15.4 counts with interval [−54.6, 85.3]. NIST timing-offset records exhibit a terminal-mask excess accompanied by an Alice-side singles-rate change and compatible with a separately calibrated local-setting mixture. The evidence separates reproducible structure, failure of an additive accepted-centroid model, and effects accommodated by explicit response controls. Finite coincidence selection and known switching-related populations prevent the centroid contrast alone from establishing intrinsic polarization–time coupling or a failure of quantum theory. Statistical scope. The analyses are exploratory. Coarser clustering weakens scan-adjusted significance: with ten blocks per half, the highlighted Weihs contrast has adjusted approximate p values of 0.087 and 0.014. The residual is specific to the accepted-centroid model and does not establish a discrepancy beyond all independently calibrated temporal-response models. Files and reproducibility. Bell_manuscript.pdf is the self-contained, 13-page preprint dated 30 October 2026. Bell_Reanalysis_Source.zip contains the editable LaTeX manuscript, numerical figure code, reconstruction and analysis scripts, derived records, source manifests and hashes, full comparison tables, calibration and sensitivity results, and reproduction instructions. The NIST analysis uses 60 prescribed samples of 500,000 trials, rather than complete runs. The full upstream Christensen archive and Weihs time-tag files are retrieved by the supplied fetchers and are not bundled. A clean internal rerun reproduced the checked numerical outputs exactly; external independent reproduction is not claimed. Publication status and assistance. This research preprint has not been peer reviewed. AI tools assisted programming, analysis, and manuscript preparation; responsibility for the work remains with the author. License scope. The manuscript and original figures are licensed under Creative Commons Attribution 4.0 International. Original analysis code is licensed under MIT. Third-party source data and derived excerpts retain applicable source terms and attribution; this deposit does not relicense upstream material.
From a finite event record to Bell correlations and their loss under recording A pair is prepared together, read at two separated instruments, and allowed to leave a material record. This paper builds the correlation law from a real source geometry in Artian's Quantum Traction Theory. Its source-to-access equation is pK(r,s∣a,b)=C(KΩ)C[(Πr(a)⊗Πs(b)⊗I)KΩ] Here C is an additive, basis-invariant event capacity, Omega is the normalized orientation-neutral two-channel source, K is a specified record contact, and the projectors select the two instrument outputs. A real quarter-turn and a qualified shared-reference composition generate the readout algebra. Capacity symmetry fixes its quadratic weight. A separately stated capacity-to-frequency condition connects that weight to laboratory counts. The correlation follows before the Bell comparison For a phase-compensated record contact with overlap g between its two normalized record profiles, the construction gives EK(a,b)=−azbz−g(axbx+ayby),0≤g≤1. The intact-source limit is E = -a dot b. The same calculation yields the fixed-setting and optimized Bell responses: S45=2(1+g),Sopt=21+g2. Fresh independent record contacts multiply their overlaps. The paper derives the repeated-contact law, a capacity-based overlap calibration, uncertainty bounds, and a protocol that separates calibration from the Bell observations being judged. A source-first account with an explicit dependency map A1 supplies event-time labels and the clock-angle correspondence; A4 supplies the real dial; A5-X supplies completed-event support, with its inherited A6/A7 conditions. The two-channel preparation, balanced composition, capacity symmetry, frequency bridge, and record coupling are printed separately. Each theorem states exactly which conditions it uses. The Access uncertainty commutator is treated as a distinct inherited algebraic premise, rather than inferred from Bell correlations. When a receiver follows the source Version 2.0 constructs a matched receiver rather than assigning its transformation by name. Preserving every probability of the stated bilinear contact forces its transport to be the conjugate of the source transport, up to an overall phase: ∣rTVTUs∣2=∣rTs∣2for all r,s⟹V=eiαU. A finite set of basis and sum probes certifies this relation. A robust extension converts imperfect probe probabilities into an operator-error bound. Finite clock and shift operations then produce the comparison loop L=M+ω(I−M),ω=e2πi/d. The matched sector cancels the comparison phase while the unmatched sector retains it. This is a joint comparison law; each local readout can remain incompatible. The paper identifies the binary loop's ambiguity, provides additional probes that distinguish it, and transfers the Bell correlations into a complete detector record when the original carrier is consumed. One contact, two observable roles A specified marker contact supplies both the Bell record overlap and a resolved weak-measurement instrument: γK0K1=sinθ,=diag(cos(θ/2),sin(θ/2)),=diag(sin(θ/2),cos(θ/2)). An independent replay executes this instrument on all 40,032 tree records in the public Feng and colleagues archive, reproducing every stored decoder success/failure score. The main five-setting batch contains 32,000 records; the complete archive has six settings. The reproduced job-cluster residual probabilities are p = 0.0188753 and p = 0.0442603, respectively. These diagnose modest tension with the ideal instrument under the stated retrospective covariance. The matched QTT and quantum representations make the same archival predictions, so this replay is not a significance test between them. The package preserves the complete source-first Bell construction and adds finite receiver certificates, physical transport-error bounds, a common-contact derivation, five vector figures, a twelve-item achievements ledger, and offline reproducibility materials. The next operational question is precise: which independently qualified physical contact fixes both the record overlap and the receiver comparison response? Dependencies: QTT Main Book; finite address-capacity counting; real source histories and composition; A1-CHSH spinor character; Observation as Access.