When do two clock labels become two physical experiments? An A1 reference-switch test is meaningful only if the two terminal labels are implemented by different physical write histories. This paper gives a carrier-independent answer. It represents the apparatus as a complete quantum instrument, reconstructs the laboratory write graph, and asks which physical event last wrote the durable record that survives to closure. Ontological reading. The primitive relevant to this theorem is the completed event: one finite source process closes and leaves a physical ledger record before a laboratory clock assigns its readout label. The candidate (T^\star) terminal carries a durable memory of that completion; the \(\tau\) terminal is defined or overwritten by a laboratory reference. The experiment therefore does not compare two names for time. It compares two physical histories of what last wrote the terminal record. The candidate source terminal is defined without using the desired result: \[ \boxed{ \mathfrak T_{T^\star}: C_E=1,\quad \Xi_L\le\epsilon_L,\quad \Xi_S\ge\eta_S,\quad M_S\ \text{continuous},\quad N_{\rm rec}=0,\quad N_{\rm proj}=1 } \] Here (C_E) certifies a completed source event, (Xi_L) bounds laboratory write susceptibility, (Xi_S) proves that the surviving record still depends on the source memory, (N_{\rm rec}=0) forbids a later reference overwrite, and (N_{\rm proj}=1) permits one final basis-selecting readout. Ordinary free evolution does not pass this constructor. Fifteen predeclared gates compute one activation bit: \[ \boxed{ G_{\rm PT}=\prod_{j=1}^{15}P_j } \] \[ \boxed{ G_{\rm PT}=1 \Longrightarrow \begin{cases} R_{\rm clk}^{\rm ordinary}=1,\\[1mm] R_{\rm clk}^{\rm QTT-A1} =\cos^q\!\left(\frac{\pi}{8}\right), \end{cases} \qquad G_{\rm PT}=0 \Longrightarrow \texttt{INELIGIBLE\_NO\_THEORY\_VERDICT} } \] The detector degree (q) is derived and frozen before target data. A four-history experiment then tests the crossing character ((0,1,1,0)), with the geometric-mean estimator \[ \boxed{ R_{\rm clk} = \sqrt{ \frac{|D_{\tau T^\star}D_{T^\star\tau}|} {|D_{\tau\tau}D_{T^\star T^\star}|} } \frac{1}{C_K N_\times^{\rm ordinary}} } \] The framework proves that software relabelling, passive data reduction, a dark interval, and zero laboratory-write rank by themselves cannot create a second clock terminal. It also makes any apparatus containing a programmed (22.5^\circ), (45^\circ), CHSH-standard, or target-equivalent overlap ineligible before unblinding. The theorem is the shared activation layer for matter-wave Sagnac, Faraday, Berry/holonomy, delocalized quantum-clock, monitored-recurrence, photon-storage, and related reference-switch tests. Platform qualification and empirical A1 judgment remain separate downstream tasks. Concept DOI: 10.5281/zenodo.21739215 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org · Lexicon · Derivation Atlas · Observatory
When do two clock labels become two physical experiments? An A1 reference-switch test is meaningful only if the two terminal labels are implemented by different physical write histories. This paper gives a carrier-independent answer. It represents the apparatus as a complete quantum instrument, reconstructs the laboratory write graph, and asks which physical event last wrote the durable record that survives to closure. Ontological reading. The primitive relevant to this theorem is the completed event: one finite source process closes and leaves a physical ledger record before a laboratory clock assigns its readout label. The candidate (T^\star) terminal carries a durable memory of that completion; the (\tau) terminal is defined or overwritten by a laboratory reference. The experiment therefore does not compare two names for time. It compares two physical histories of what last wrote the terminal record. The candidate source terminal is defined without using the desired result: [ \boxed{ \mathfrak T_{T^\star}: C_E=1,\quad \Xi_L\le\epsilon_L,\quad \Xi_S\ge\eta_S,\quad M_S\ \text{continuous},\quad N_{\rm rec}=0,\quad N_{\rm proj}=1 } ] Here (C_E) certifies a completed source event, (Xi_L) bounds laboratory write susceptibility, (Xi_S) proves that the surviving record still depends on the source memory, (N_{\rm rec}=0) forbids a later reference overwrite, and (N_{\rm proj}=1) permits one final basis-selecting readout. Ordinary free evolution does not pass this constructor. Fifteen predeclared gates compute one activation bit: [ \boxed{ G_{\rm PT}=\prod_{j=1}^{15}P_j } ] [ \boxed{ G_{\rm PT}=1 \Longrightarrow \begin{cases} R_{\rm clk}^{\rm ordinary}=1,\[1mm] R_{\rm clk}^{\rm QTT-A1} =\cos^q!\left(\frac{\pi}{8}\right), \end{cases} \qquad G_{\rm PT}=0 \Longrightarrow \texttt{INELIGIBLE_NO_THEORY_VERDICT} } ] The detector degree (q) is derived and frozen before target data. A four-history experiment then tests the crossing character ((0,1,1,0)), with the geometric-mean estimator [ \boxed{ R_{\rm clk} = \sqrt{ \frac{|D_{\tau T^\star}D_{T^\star\tau}|} {|D_{\tau\tau}D_{T^\star T^\star}|} } \frac{1}{C_K N_\times^{\rm ordinary}} } ] The framework proves that software relabelling, passive data reduction, a dark interval, and zero laboratory-write rank by themselves cannot create a second clock terminal. It also makes any apparatus containing a programmed (22.5^\circ), (45^\circ), CHSH-standard, or target-equivalent overlap ineligible before unblinding. The theorem is the shared activation layer for matter-wave Sagnac, Faraday, Berry/holonomy, delocalized quantum-clock, monitored-recurrence, photon-storage, and related reference-switch tests. Platform qualification and empirical A1 judgment remain separate downstream tasks. Concept DOI: 10.5281/zenodo.21739215 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org · Lexicon · Derivation Atlas · Observatory
A sealed laboratory fork for monitored quantum recurrence Can the location of a first-detection recurrence resonance distinguish two physically qualified time-reference classes after ordinary clock-transfer, Hamiltonian, waveform, detector, and environmental effects have been held fixed? This preregistration converts that question into a reciprocal two-device experiment with a machine-evaluable entrance gate and a finite outcome ledger. For device d and preregistered transition j, the laboratory reports one dimensionless root ratio, ydj=log(xdAj∗xdLj∗),Δ=1TΣy−111TΣy−1y,RMRRS=eΔ. The two frozen point hypotheses are H0:Δ0=0,R0=1,HA1:ΔA1=logcos(8π)=−0.0791735919101875…,RA1=cos(8π)=0.9238795325112867…. The A1 point is dormant unless the proposed physical terminal exists in the apparatus. Version 2.0 therefore places a fifteen-gate constructor ahead of all role-dependent recurrence output: GPT=∏i=115Pi. The gate requires a completed source event, continuous physical source memory, no later laboratory write, a source intervention witness, a target-blind ordinary camera, a numerical rank-two terminal Jacobian, a complete clock graph, and an irreversible pre-data seal. A free-running oscillator alone is not a T⋆ terminal. If any gate fails, the registered result is GPT=0⟹TARGET_NOT_ACTIVATED. The executable packet freezes two devices, two independent oscillator chains, four reciprocal role cells, four recurrence roots, eight supercycles, N=1024, an 81-point primary scan, and 16,384 trajectories per point, role, device, and transition. The estimator is the full finite-N multinomial likelihood, including the no-detection category; no manual fit window, pseudoinverse, post-unblinding regularization, or effect-directed exclusion is permitted. The two equivalence regions have fixed half-width 0.025 in log space, and the primary design gate is SE(Δ)≤0.006. A registered point must also exclude the other by at least five standard deviations. A fresh 400+400 finite-horizon synthetic campaign gives uΔsynth=0.0010808000,uΔsynth∣ΔA1−Δ0∣=73.25. Every synthetic campaign is classified correctly under the printed planning assumptions. This is a software and power receipt, not hardware activation or a laboratory observation. Release status: CLOSED: laboratory instruction layer and machine packet; CLOSED: synthetic activation, fail-closed, power, and outcome-classifier audits; PENDING: platform-specific hardware packet and physical-terminal activation; PENDING: qualified laboratory data and empirical A1 verdict. The reconstruction archive contains the LaTeX source, exact protocol JSON, activation templates and validator, raw-data dictionary, 31 exclusion codes, finite-N power program, six-outcome classifier, independent experimental review and response matrix, visual audit, a 60-check release receipt, and complete SHA-256 hashes. Stable concept DOI: 10.5281/zenodo.21703683 Physical Terminal constructor: 10.5281/zenodo.21739215 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org
A quantum clock can follow two proper-time histories. Can one completed coherence also distinguish two physical reference classes? Quantum-clock interferometry already supplies the standard carrier relation Δϕclock=ω0Δτ. This preregistration keeps that relation intact and asks a separate question. The same atomic transition and path geometry are executed through four physical input/output terminal histories, ττ,τT,Tτ,TT. For each history and reversed proper-time geometry, the laboratory fits the first complex clock-coherence phasor and forms Dab=∣Zab+Zab−∣. The registered reference-switch statistic is Rqc,clk=N×ord1DττDTTDτTDTτ. After a target-blind ordinary cross-history map, the fixed prospective fork is Hordinary:Rqc,clk=1,HQTT−A1:Rqc,clk=cos(8π). The alternatives differ by 7.6120467%. A bare five-standard-deviation separation requires σ(Rqc,clk)≤0.0152241, and the recommended design target is 0.005. The proper-time phase is a common carrier check, not the A1 discriminator. The release includes three adversarial audits. It requires a physical hardware graph for the T and τ terminal classes, derives the readout exponent from a first complex phasor, and qualifies preparation and calibration by their physical transfer, not by angle alone. A target-inserting primary operation or target-trained correction remains ineligible. Any failed eligibility gate returns INELIGIBLE_NO_THEORY_VERDICT rather than a false rejection of A1. Scientific status: theorem and estimator closed; carrier technology plausible; physical four-terminal hardware map and laboratory dataset pending. No existing quantum-clock record is claimed as A1 evidence. Concept DOI: 10.5281/zenodo.21674815 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org · Two Universes · Lexicon · Observatory The public files are the paper PDF first and the complete reconstruction ZIP second. Version 1.1: operation qualification and retained observations The numerical targets, ratio orientation, decision regions and historical seals are unchanged. A 22.5-degree or 45-degree component is no longer excluded by its angle alone: its physical transfer must be independently established. Common-operation cancellation and signal-preserving calibration are proved; both hypotheses must remain identifiable. Every acquired record is retained. After authorized unblinding, QTT-like, ordinary-like and unexpected outcomes are reported, including observations that do not qualify for a theory verdict. This is a prospective amendment, not a retrospective resealing of data. Clock, ruler and signal-recovery qualification. Both registered predictions are constructed at the raw detector with explicit proper-time, coordinate-time, worldline, ruler and synchronization conventions. Each relativistic effect is counted once. Independently calibrated corrections carry their uncertainties through the common comparison; the tested rows cannot train a normalization that forces either answer. Blind recovery is required separately for both alternatives at every predeclared operating setting. The inherited targets and decision rules remain fixed. The included design study makes sensitivity explicit: for the Two-Test Gram classifier, a total ratio uncertainty of 0.0013 gives approximately 88.9% QTT-branch and 94.1% ordinary-branch power under the stated ideal model. These are conditional detection probabilities, not probabilities that a theory is true, and each instrument retains its own classifier. The complete apparatus packet must be sealed before acquisition and target access; historical campaign rules remain preserved. Reconstruction entry point. Start with current/CURRENT_RELATIVISTIC_EXECUTION.md in the ZIP. The shared execution contract refers once to the development filename CURRENT_EXECUTION_RC.md; that reference means CURRENT_RELATIVISTIC_EXECUTION.md in this release. The packaged README names the correct file. This navigation correction does not change the deposited files, scientific requirements or historical seals.
A geometric phase can verify a loop without being mistaken for the clock effect under test. This paper isolates a clean experimental question in geometric quantum mechanics: can the same completed holonomy be read through two physically distinct terminal-reference architectures without confusing ordinary carrier geometry, calibration, or passive propagation with a new clock projection? For an adiabatic spin-21 loop, the ordinary Berry carrier is γgeo=−2Ω. That relation is retained as a shared geometry check. It is not assigned a direct cos(π/8) deficit. The paper shows why the raw ratio −Ω/2γgeo has the target 1 for both ordinary quantum mechanics and the registered QTT A1 readout statement. The proposed discriminating object is instead a sealed four-history, first-phasor amplitude ratio: Rgeo,clk=N×ord1DττDTTDτTDTτ,Dab=∣Zab(+Ω)Zab(−Ω)∣. Here Zab is the fitted first complex fringe phasor and N×ord is a target-blind, independently certified ordinary cross-history map. The frozen alternatives are Hordinary:Rgeo,clk=1,HQTT-A1:Rgeo,clk=cos(8π). The paper audits the historical neutron-spin and optical-fiber geometric-phase records. They establish useful holonomy carriers but do not contain the physical crossed T/τ terminal histories, target-blind transfer map, raw four phasors, or joint covariance needed for this statistic. No archival QTT confirmation is claimed. The resulting protocol is prospective and falsifiable: a qualified result compatible with one fixed target while excluding the other has a predeclared meaning; any topology, transfer, carrier, covariance, target-contamination, or power failure is ineligible for a theory verdict. The recommended first implementation is a polarized-neutron spin-echo or interferometric platform with a static helical magnetic-field loop. Its spin-21 carrier, field-defined solid angle, and winding reversal provide an independently auditable geometry layer while the terminal-reference switch is tested separately. The fixed separation 1−cos(8π)=0.0761204674887133… requires σ(Rgeo,clk)≤0.0152241 for a bare five-standard- deviation distinction; the laboratory design target is 0.005. Status: PASS_GEOMETRIC_CARRIER_HAS_INDEPENDENT_LOOP_GEOMETRY PASS_SAME_PLATFORM_BERRY_REFERENCE_SWITCH_IS_BOOK_NATIVE ARCHIVE_INELIGIBLE_NO_CROSSED_REFERENCE_HISTORIES PROSPECTIVE_TEST_READY Concept DOI: 10.5281/zenodo.21673340 Main book anchor: Quantum Traction Theory: Main Book v10.01, especially PDF pp. 159--172 and 889--892. Website: quantumtraction.org | Two Universes: time | Lexicon | Observatory | Corpus Tree Included files: PDF paper, Version 1.0 Complete reconstruction ZIP with LaTeX source, laboratory certificates, archival audit, synthetic cancellation fixture, verification scripts, render audit, and SHA-256 manifest Version 1.1: operation qualification and retained observations The numerical targets, ratio orientation, decision regions and historical seals are unchanged. A 22.5-degree or 45-degree component is no longer excluded by its angle alone: its physical transfer must be independently established. Common-operation cancellation and signal-preserving calibration are proved; both hypotheses must remain identifiable. Every acquired record is retained. After authorized unblinding, QTT-like, ordinary-like and unexpected outcomes are reported, including observations that do not qualify for a theory verdict. This is a prospective amendment, not a retrospective resealing of data. Clock, ruler and signal-recovery qualification. Both registered predictions are constructed at the raw detector with explicit proper-time, coordinate-time, worldline, ruler and synchronization conventions. Each relativistic effect is counted once. Independently calibrated corrections carry their uncertainties through the common comparison; the tested rows cannot train a normalization that forces either answer. Blind recovery is required separately for both alternatives at every predeclared operating setting. The inherited targets and decision rules remain fixed. The included design study makes sensitivity explicit: for the Two-Test Gram classifier, a total ratio uncertainty of 0.0013 gives approximately 88.9% QTT-branch and 94.1% ordinary-branch power under the stated ideal model. These are conditional detection probabilities, not probabilities that a theory is true, and each instrument retains its own classifier. The complete apparatus packet must be sealed before acquisition and target access; historical campaign rules remain preserved. Reconstruction entry point. Start with current/CURRENT_RELATIVISTIC_EXECUTION.md in the ZIP. The shared execution contract refers once to the development filename CURRENT_EXECUTION_RC.md; that reference means CURRENT_RELATIVISTIC_EXECUTION.md in this release. The packaged README names the correct file. This navigation correction does not change the deposited files, scientific requirements or historical seals.
A sealed two-instrument search for an unprogrammed clock-reference projection This preregistration compares two fixed point hypotheses using independent matter-wave Sagnac and Faraday polarization-coherence instruments. Each instrument uses four physical histories and a camera-corrected Gram quotient: Rdobs=CdNdord1∣Dττ(d)DTT(d)∣∣DτT(d)DTτ(d)∣. After physical activation, the frozen fork is Rdstandard=1,RdQTT=cos(8π)=0.9238795325112867…. Version 3.1 adds a post-seal standard-physics completeness gate for rotating atomic and ring-cavity platforms. The ordinary model must include or bound every applicable centre-of-mass, internal-spin, field, rotational Röntgen, polarization, backscatter, trap, Zeeman, and Stark term. In compact form, Hrotstd=H0−Ω⋅(L+F+ℓF)+HRR+HZ+HStark+Htrap+Hbs+Hpol+⋯, with the rotation-induced hyperfine row HRH=−Ω⋅F,δωRH=−Ω∥ΔmF. The standard-null ledger, parameter provenance, held-out controls, and adequacy thresholds are frozen before target labels. If an applicable row is unresolved, the packet returns INELIGIBLE_NO_THEORY_VERDICT. No target digit, ratio orientation, compatibility band, power floor, or numerical decision threshold is changed. Operation eligibility and reporting are amended as described below. Concept DOI: 10.5281/zenodo.21376520 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org Version 3.2: operation qualification and retained observations The numerical targets, ratio orientation, decision regions and historical seals are unchanged. A 22.5-degree or 45-degree component is no longer excluded by its angle alone: its physical transfer must be independently established. Common-operation cancellation and signal-preserving calibration are proved; both hypotheses must remain identifiable. Every acquired record is retained. After authorized unblinding, QTT-like, ordinary-like and unexpected outcomes are reported, including observations that do not qualify for a theory verdict. This is a prospective amendment, not a retrospective resealing of data. Clock, ruler and signal-recovery qualification. Both registered predictions are constructed at the raw detector with explicit proper-time, coordinate-time, worldline, ruler and synchronization conventions. Each relativistic effect is counted once. Independently calibrated corrections carry their uncertainties through the common comparison; the tested rows cannot train a normalization that forces either answer. Blind recovery is required separately for both alternatives at every predeclared operating setting. The inherited targets and decision rules remain fixed. The included design study makes sensitivity explicit: for the Two-Test Gram classifier, a total ratio uncertainty of 0.0013 gives approximately 88.9% QTT-branch and 94.1% ordinary-branch power under the stated ideal model. These are conditional detection probabilities, not probabilities that a theory is true, and each instrument retains its own classifier. The complete apparatus packet must be sealed before acquisition and target access; historical campaign rules remain preserved. Reconstruction entry point. Start with current/CURRENT_RELATIVISTIC_EXECUTION.md in the ZIP. The shared execution contract refers once to the development filename CURRENT_EXECUTION_RC.md; that reference means CURRENT_RELATIVISTIC_EXECUTION.md in this release. The packaged README names the correct file. This navigation correction does not change the deposited files, scientific requirements or historical seals.
The Artian Hamiltonian Framework for QTT Version: 10.01 Concept DOI: 10.5281/zenodo.20484906 Version DOI: 10.5281/zenodo.20484907 Author: Ali Attar Website: quantumtraction.org Corpus category: Action, Feynman, path integrals, and quantum foundations This paper develops the Hamiltonian of Quantum Traction Theory (QTT) on Artian Geometry as a finite-capacity source generator of completed address events. The laboratory Hamiltonian is not taken as the primitive object: it is the access image of a deeper substrate ledger. Where a textbook Hamiltonian generates time evolution for a system already placed in a laboratory frame, the QTT Hamiltonian must first specify which completed address events are being funded, which clock is being used, which same-universe bundle has closed, and which access channel is permitted to read the result. From the axioms A1–A7 the framework is built in strict constructor order: the completed address event with its noncircular Artian ruler; the real J-dial source Hilbert module; the source Hamiltonian core; the full Artian ledger generator including birth (B_A3), endurance/destruction (D_A2), and bundle-closure (C_A7) maps; the Access Law mapping the source generator to its laboratory image through a clock Jacobian; the Unified Equilibrium Law (UEL) tying energy, action, four-volume support, and gravitational readout to a single Artian capacity endpoint E* = ℏ/t̃_A = ℏc/ℓ_A; the A6 finite-capacity ceilings; and the A7 same-universe bundle closure Q_bundle = 2π. Every standard sector — free particles, photons, fermions, scalar/Higgs, QCD, thermal reservoirs, measurement, and gravity — is placed in the same grammar, in each case separating the source rail from the laboratory readout. Companion rails connect the framework to the wider QTT corpus: unitarity as real-dial geometry, time reversal and Kramers degeneracy from dial conjugation, gauge covariance from local dial re-zeroing, the two-clock half-angle cos(π/8), the Faraday effect as a clock/access test, the endurance-to-Newton route fixing G_A = ℓ_A²c³/ℏ, worked sector dossiers, explicit laboratory-recovery derivations (Schrödinger, Dirac, Maxwell, Boltzmann, path integral), and a sector-by-sector status ledger. Every load-bearing relation is parameter-free, reducing to fundamental constants and fixed integers or angles forced by the axioms; no fitted scalar enters the source layer. A no-smuggling discipline forbids inserting an observed value into the Hamiltonian and naming it afterward. The discipline is deliberately plain: source first, access second, audit last — and a residual is treated not as a nuisance term but as a request for a missing source rail, access map, or axiom-level correction. In the last version we added: systematic page-level anchoring to the QTT monograph (v10.01) for every construction, a visual reading map of the constructor order, and refined epistemic labelling, making each claim auditable against its source. Main status labels: GREEN: Σ-OPEN-ZENODO-RECORD-PUBLISHED GREEN: Σ-CONCEPT-DOI-STABLE-CITATION GREEN: Σ-VERSION-DOI-RECONSTRUCTION-AVAILABLE SCOPE: Σ-CLAIM-STATUS-DEFINED-IN-PAPER Audit and claim scope: Concept DOI is the stable citation target for this research family. Version DOI and Zenodo record ID identify this exact public release for reconstruction. This description is a record-level guide; the paper itself controls theorem status, assumptions, and falsifiers. Related QTT anchors: Main book concept DOI: 10.5281/zenodo.17527179 Corpus Tree row: quantumtraction.org/doi-map/#record-20484907 Blog Map row: quantumtraction.org/blog-map/#corpus-record-20484907 Derivation Atlas: quantumtraction.org/derivation-atlas/ Lexicon: quantumtraction.org/lexicon/ Related QTT DOI (isVersionOf): 10.5281/zenodo.17527179 Included files: qtt_artian_hamiltonian_framework_v3_01.pdf
A timing signature is not physics until its reference operator survives a representation audit. CV⋆=FR2,UT⋆=1−FR2,CV⋆+UT⋆=1 This framework separates three objects that must not be merged: a completed historical event, the record support still accessible to a laboratory, and a separately calibrated timing observable. Standard quantum theory closes the optimized coherent-recovery envelope. QTT adds a distinct, falsifiable timing complement only after a physical intertwining certificate proves that the laboratory record operator and the central timing projector are the same physical object in two representations. A public 11,009-trace test of explanatory burden Version 1.4 executes the complete usable public archive associated with Gosling et al., Probing the memory of a superconducting qubit environment. Every trace is split chronologically into training, a discarded guard interval, and held-out testing. The ordinary one-TLS Solomon camera learns two rates per trace, while the memoryless comparator learns one. median(RMSE0RMSE0−RMSETLS)=0.36015,P(TLSwins)=11,00910,169=0.92370 The fitted TLS camera is therefore a successful held-out effective model. Its resolved trajectory is not a parameter-free derivation: the values of Γq and Γqt are learned from each target-bearing trace's training segment. Version 1.4 makes that distinction machine-auditable through the target-fit burden vector BM=(Nc,Nd,Nw,Nn,Nu,Nh),BM=0⟹the fitted output is not derived parameter-free. The QTT result A public QTT source statement from 12 November 2025, before the Gosling preprint, already required complete reset to erase distributed record support beyond the visible carrier. That statement contains no Gosling-fitted rate, hidden-mode count, target window, or trajectory coefficient. The resulting comparative verdict is QTT-ZERO-FIT-SOURCE-EXPLANATORY-VICTORY/TRAJECTORY-VERDICT-OPEN. This is a scientific victory at the source/ontology layer, not a claim that QTT has already predicted the same resolved qubit trajectory. The stronger same-observable verdict remains locked because the public archive does not independently provide the residual record fidelity Fres, leakage diagnostic D, timing complement UT, or physical intertwiner W. The paper prints the exact next experiment that would close or falsify that bridge. Reproducibility 11,009 row-level held-out results are included. The 840 traces favoring or tying the memoryless camera are retained. No false significance is assigned to correlated sweep windows. All three official archive objects pass their published MD5 checks. The release verifier passes 30/30 scientific and provenance checks. Three adversarial reviews cover observable equality, leakage and selection, chronology, and claim scope. Version: 1.4 Concept DOI: 10.5281/zenodo.21902886 Author: Ali Attar Website: quantumtraction.org Reader anchors Completed-record timing blind test Dynamic-circuit record-timing extension Observation as Access Quantum Traction Theory: Main Book Gosling public data archive The PDF is the default preview. The reconstruction archive contains the LaTeX source, row-level CSV, public-data integrity receipt, chronology certificate, fit-burden certificate, analysis scripts, exact source checks, adversarial and render audits, metadata, and checksum manifest.