Same-Central-Effect Work-Quadrature Loop Preregistration: A Blind Circuit-QED Test of the QTT Access Intertwiner

Attar Ali

Published Sep 1, 2026• 1 citation

Abstract

Can one physical access gate control both extractable work and a closed phase-space commutator without retuning? This record seals a prospective circuit-QED test of the QTT Access Intertwiner. Its paper-native master equation is \[ \boxed{ \begin{aligned} w_j&:=\frac{\Delta\mathcal W_j}{\hbar\omega|\alpha|^2}=\eta_j,\\ \mathcal R_{jk}^{\rm QTT} &=(1-\eta_j)+\eta_j e^{J\phi_k},\\ \mathcal R_{jk}^{\rm QM}&=1,\\ \frac{\partial(\eta_j,\phi_k)} {\partial\mathcal R_{jk}^{\rm target}}&=0. \end{aligned}} \] A bosonic microwave mode is prepared in the symmetric ensemble $|+\alpha\rangle$ or $|-\alpha\rangle$. The preparation bit is written into an authenticated physical register. A randomized hardware route either makes that record available during the terminal window or keeps it unavailable until afterward. The work branch is a physical qualification. If the bit is available, a conditional displacement returns the mode to vacuum and the normalized gross energy drop is $w_j=\eta_j$. Standard information thermodynamics and QTT both expect that row; it is not counted as QTT-exclusive evidence. The second branch is the discriminator. Four calibrated displacements form a closed phase-space group commutator. Ordinary canonical quantum mechanics predicts the same normalized geometric phase for every idle access setting. QTT predicts the exact complex surface $(1-\eta)+\eta e^{J\phi}$ from the same independently constructed central effect. Frozen design: five access settings: $0,1/4,1/2,3/4,1$; four primary loop areas: $\pi/4,\pi/2,3\pi/4,\pi$; positive and negative loop orientations; zero target-fitted QTT coefficients; one global complex-vector comparison under one frozen covariance; late-route, dummy-bit, matched-load, erasure, reversal, zero-area, state-transport, and complete-record controls. A theory verdict is legal only after an experiment-specific activation certificate freezes the physical effect, its complete terminal alphabet, the ordinary circuit model, all calibration quantities and covariances, crosstalk bounds, the work/loop route identity, and at least 90 percent power at a global one-sided five-sigma threshold before target data are opened. Status: STAGE-0 SEALED / PHYSICAL ACTIVATION PENDING / OBSERVATION PENDING. This is a test of a speculative new theory. No observation is claimed. Reader anchors: Observation as Access Artian Hamiltonian Framework QTT Main Book QTT Observatory QTT Derivation Atlas QTT Lexicon The PDF is the default preview. The reconstruction ZIP contains the LaTeX and Markdown sources, immutable protocol seal, frozen prediction surface, activation templates, data schemas, blind classifier, three adversarial reviews, scientific and render audits, verification receipt, and SHA-256 manifest.

DOI: 10.5281/zenodo.22236546

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Fourth-Face Talbot-Lau Completed-Event Preregistration: An Activation-Gated Blind Test of A7U Matter-Wave Transport

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Can a finite Talbot chamber produce a nonconstant visibility shape after the ordinary interferometer kernel is frozen? \[ \boxed{ \begin{aligned} H_0:&\ \mathbf y_\perp=0,\\ H_{\mathrm{A7U}}:&\ \mathbf y_\perp=P_{\mathrm{prof}}\mathbf g^{\mathrm{phys}},\\ g_r^{\mathrm{phys}}=&\ \log\left|\frac{\int_{\Delta v_r}W_r(v)B_1^{\mathrm{QM/env}}(v)F_1^{\mathrm{A7U}}(v)\,dv}{\int_{\Delta v_r}W_r(v)B_1^{\mathrm{QM/env}}(v)\,dv}\right|,\\ &\ \frac{\partial\mathbf g^{\mathrm{phys}}}{\partial\mathbf y}=0. \end{aligned}} \] Version: 1.2 State: Stage-0 sealed; physical target activation pending; observation pending Concept DOI: 10.5281/zenodo.22010227 Author: Ali Attar, ORCID 0009-0008-9931-2691 Version note: v1.2 is an append-only source-projector-camera scope upgrade. The historical v1.0.1 branch, source equations, seven-bin vector, thresholds, PDF hash, and protocol-seal hash remain preserved. The v1.1 calibration-orthogonality gate also remains unchanged. The new outer wrapper separates the sealed A7U source-harmonic verdict from any stronger interpretation as a measurement of the central Access-Law projector weight. This preregistration asks for a seven-bin, first-harmonic matter-wave shape, not a constant loss of fringe contrast. The source branch is fixed before observation, but the final laboratory prediction is legal only after the ordinary complex Talbot kernel, event weights, operating point, calibration uncertainty object, physics-generated tangent basis, covariance, extraction operator, and the apparatus proof of kappa = 1 are independently frozen. The finite source law is \[ \Delta_n(v)=\left\|n^2\frac{hL}{d^2mv}\right\|_{\mathbb Z},\qquad N_{\Gamma,n}=\left\lceil\Delta_n^{-1}\right\rceil,\qquad F_n^{\mathrm{A7U}}=\sqrt{1-2\kappa_n\frac{2}{N_{\Gamma,n}}\left(1-\frac{1}{N_{\Gamma,n}}\right)}. \] The release seals a high-precision source-only feasibility vector, but proves why that vector cannot be substituted for the physical instrument prediction. Complex Talbot coefficients must be combined inside each velocity-bin integral before taking their modulus. This is the central wrong-falsification firewall: source-only forecast ≠ physical instrument prediction ≠ observation. A central Access-Law interpretation requires the additional prospectively frozen certificate \[ W^\dagger M W=P_a, \qquad C_n^{\mathrm{obs}}=(1-\eta)C_{n,u}+\eta C_{n,a}, \qquad \frac{\partial(W,M,C_{n,u},C_{n,a})}{\partial\mathbf y}=0. \] Without it, the test still adjudicates the activated A7U Talbot-Lau branch, but the lawful projector label is INELIGIBLE_NO_ACCESS_LAW_ETA_VERDICT. This prevents both wrong falsification and false promotion without weakening the sealed test. The calibration-orthogonality gate is \[ U_{\mathrm{phys}}=[\mathbf 1,\partial_{\theta_1}\log|\bar B_1^0|,\ldots],\qquad R_{\mathrm{sens}}^{\mathrm{cal}}= \sqrt{(P_{\mathrm{phys}}\mathbf g^{\mathrm{phys}})^T (P_{\mathrm{phys}}\Sigma P_{\mathrm{phys}}^T)^+ (P_{\mathrm{phys}}\mathbf g^{\mathrm{phys}})}\ge5. \] If the apparatus or data packet does not pass every activation gate, the deterministic result is TARGET-NOT-ACTIVATED or INELIGIBLE_NO_THEORY_VERDICT. The source-only forecast is 96.51% linear in velocity, so a generic constant-only nuisance model is not sufficient; the activated mass, phase, velocity-width, grating, and separation derivatives must be projected explicitly. These pre-data gates cannot be altered after a null. A qualified null therefore remains a real scoped falsifier. The public Pedalino sodium-nanoparticle archive establishes that the high-mass Talbot-Lau platform is real and experimentally mature, but it does not contain the complete velocity-resolved visibility, covariance, ordinary-kernel, and path-provenance packet required for a retrospective execution. Its published ordinary theory curves share a fitted global contrast factor of 0.78, so a constant additional suppression is not separately identifiable. This is therefore a prospective sealed test, not an observation claim. Stable scientific anchors: A7U Molecular Visibility Transport A7U source framework Quantum Traction Theory: Main Book Pedalino et al., Nature experiment Public experimental archive QTT Observatory · DOI map

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Artian's Physical Contact Transfer Test

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Sep 26, 20261 citation

Same-Central-Effect Work-Quadrature Loop Preregistration: A Blind Circuit-QED Test of the QTT Access Intertwiner

Attar Ali

Published Sep 1, 2026• 1 citation

Publisher

Abstract

Can one physical access gate control both extractable work and a closed phase-space commutator without retuning? This record seals a prospective circuit-QED test of the QTT Access Intertwiner. Its paper-native master equation is [ \boxed{ \begin{aligned} w_j&:=\frac{\Delta\mathcal W_j}{\hbar\omega|\alpha|^2}=\eta_j,\ \mathcal R_{jk}^{\rm QTT} &=(1-\eta_j)+\eta_j e^{J\phi_k},\ \mathcal R_{jk}^{\rm QM}&=1,\ \frac{\partial(\eta_j,\phi_k)} {\partial\mathcal R_{jk}^{\rm target}}&=0. \end{aligned}} ] A bosonic microwave mode is prepared in the symmetric ensemble (|+\alpha\rangle) or (|-\alpha\rangle). The preparation bit is written into an authenticated physical register. A randomized hardware route either makes that record available during the terminal window or keeps it unavailable until afterward. The work branch is a physical qualification. If the bit is available, a conditional displacement returns the mode to vacuum and the normalized gross energy drop is (w_j=\eta_j). Standard information thermodynamics and QTT both expect that row; it is not counted as QTT-exclusive evidence. The second branch is the discriminator. Four calibrated displacements form a closed phase-space group commutator. Ordinary canonical quantum mechanics predicts the same normalized geometric phase for every idle access setting. QTT predicts the exact complex surface ((1-\eta)+\eta e^{J\phi}) from the same independently constructed central effect. Frozen design: five access settings: (0,1/4,1/2,3/4,1); four primary loop areas: (\pi/4,\pi/2,3\pi/4,\pi); positive and negative loop orientations; zero target-fitted QTT coefficients; one global complex-vector comparison under one frozen covariance; late-route, dummy-bit, matched-load, erasure, reversal, zero-area, state-transport, and complete-record controls. A theory verdict is legal only after an experiment-specific activation certificate freezes the physical effect, its complete terminal alphabet, the ordinary circuit model, all calibration quantities and covariances, crosstalk bounds, the work/loop route identity, and at least 90 percent power at a global one-sided five-sigma threshold before target data are opened. Status: STAGE-0 SEALED / PHYSICAL ACTIVATION PENDING / OBSERVATION PENDING. This is a test of a speculative new theory. No observation is claimed. Reader anchors: Observation as Access Artian Hamiltonian Framework QTT Main Book QTT Observatory QTT Derivation Atlas QTT Lexicon The PDF is the default preview. The reconstruction ZIP contains the LaTeX and Markdown sources, immutable protocol seal, frozen prediction surface, activation templates, data schemas, blind classifier, three adversarial reviews, scientific and render audits, verification receipt, and SHA-256 manifest.

DOI: 10.5281/zenodo.22236546

Related papers

QTT Carrier-Deletion Finite-Window and Timing-Access Blind Test Extension

Attar Ali

Erase the apparent carrier. Recover the qubit from its halo. Then ask a different clock. This preregistration separates an ordinary quantum-memory qualification from a distinct timing test. Test A evolves a logical qubit through a frozen local channel, physically resets its original carrier, and asks whether a finite surrounding window can recover it. Test B asks whether that independently reconstructed channel fidelity controls a separate timing-covariance frontier. Test A: where is the recoverable channel? $\mathcal R_i(\omega)=|0\rangle\!\langle0|_i\otimes\operatorname{Tr}_i\omega,$ $Q_{\rm del}=2F_{\rm avg}(\mathcal N_{\rm del},\operatorname{id})-1, \qquad \boxed{F_e^{\rm del}=\frac{1+3Q_{\rm del}}4.}$ Target-only and every smaller halo subwindow remain optimized counterfactuals. A physical reset, sham reset, hidden-record injection, boundary ladder, and complete terminal record are required before the recovery layer qualifies. Test B: does the memory verifier intertwine with an independent timing projector? $\boxed{W^\dagger M_eW=P_{\rm align}}, \qquad \eta_T=\operatorname{Tr}(\rho P_{\rm align}),$ $\mathcal U_T^\star =\inf 2\sqrt{\det\Sigma_{T\Omega}}.$ On the certified canonical branch, the sealed QTT target is $\boxed{ \eta_T=F_e^{\rm del}, \qquad \mathcal U_T^\star=1-F_e^{\rm del}. }$ No complement coefficient is fitted. Five fidelity corridors, a radius/depth ladder, one-third untouched holdouts, topology twins, full covariance, global five-sigma decisions, at least 95% planned power, and transfer to a second record technology are frozen before data. The external computation is a feasibility anchor, not the timing target An, Cao, and Cui report carrier-deletion recovery in a local kicked-Ising memory. Their result qualifies the plausibility of Test A. Their reported $Q=0.516$ is explicitly forbidden from constructing Test B. The public source archive lacks the exact arrays and scripts, so exact replication remains pending. Five terminal outcomes INELIGIBLE_NO_THEORY_VERDICT REGISTERED_QTT_CONSEQUENCE_FALSIFIED QTT_CANDIDATE QUALIFIED_OTHER_OR_CROSS_CHANNEL_ANOMALY AMBIGUOUS_OR_UNDERPOWERED Any failed eligibility gate terminates without a theory verdict. A positive result requires the full multirung shape, not one selected point. An off-target anomaly is preserved rather than discarded or used as a post-hoc rescue. Immutable protocol seal eb0640b25c1d0bde56cacc7f25d9ce4304594833e4aa937ed50293a1faafc849 This is a separate sealed extension. It changes no target, threshold, classifier, protocol hash, or file in the parent test under concept DOI 10.5281/zenodo.21902885. Public anchors Completed-record fan-out and timing-access framework Observation as Access Quantum Traction Theory: Main Book External finite-window recovery paper The PDF is the default preview. The reconstruction archive contains the sealed JSON, classifier, eighteen-gate and raw-terminal templates, Stage-0 handoff, verifier, external audit, adversarial review, metadata, and checksums.Erase the apparent carrier. Recover the qubit from its halo. Then ask a different clock. This preregistration separates an ordinary quantum-memory qualification from a distinct timing test. Test A evolves a logical qubit through a frozen local channel, physically resets its original carrier, and asks whether a finite surrounding window can recover it. Test B asks whether that independently reconstructed channel fidelity controls a separate timing-covariance frontier. Test A: where is the recoverable channel? \[ \mathcal R_i(\omega)=|0\rangle\!\langle0|_i\otimes\operatorname{Tr}_i\omega, \] \[ Q_{\rm del}=2F_{\rm avg}(\mathcal N_{\rm del},\operatorname{id})-1, \qquad \boxed{F_e^{\rm del}=\frac{1+3Q_{\rm del}}4.} \] Target-only and every smaller halo subwindow remain optimized counterfactuals. A physical reset, sham reset, hidden-record injection, boundary ladder, and complete terminal record are required before the recovery layer qualifies. Test B: does the memory verifier intertwine with an independent timing projector? \[ \boxed{W^\dagger M_eW=P_{\rm align}}, \qquad \eta_T=\operatorname{Tr}(\rho P_{\rm align}), \] \[ \mathcal U_T^\star =\inf 2\sqrt{\det\Sigma_{T\Omega}}. \] On the certified canonical branch, the sealed QTT target is \[ \boxed{ \eta_T=F_e^{\rm del}, \qquad \mathcal U_T^\star=1-F_e^{\rm del}. } \] No complement coefficient is fitted. Five fidelity corridors, a radius/depth ladder, one-third untouched holdouts, topology twins, full covariance, global five-sigma decisions, at least 95% planned power, and transfer to a second record technology are frozen before data. The external computation is a feasibility anchor, not the timing target An, Cao, and Cui report carrier-deletion recovery in a local kicked-Ising memory. Their result qualifies the plausibility of Test A. Their reported $Q=0.516$ is explicitly forbidden from constructing Test B. The public source archive lacks the exact arrays and scripts, so exact replication remains pending. Five terminal outcomes INELIGIBLE_NO_THEORY_VERDICT REGISTERED_QTT_CONSEQUENCE_FALSIFIED QTT_CANDIDATE QUALIFIED_OTHER_OR_CROSS_CHANNEL_ANOMALY AMBIGUOUS_OR_UNDERPOWERED Any failed eligibility gate terminates without a theory verdict. A positive result requires the full multirung shape, not one selected point. An off-target anomaly is preserved rather than discarded or used as a post-hoc rescue. Immutable protocol seal eb0640b25c1d0bde56cacc7f25d9ce4304594833e4aa937ed50293a1faafc849 This is a separate sealed extension. It changes no target, threshold, classifier, protocol hash, or file in the parent test under concept DOI 10.5281/zenodo.21902885. Public anchors Completed-record fan-out and timing-access framework Observation as Access Quantum Traction Theory: Main Book External finite-window recovery paper The PDF is the default preview. The reconstruction archive contains the sealed JSON, classifier, eighteen-gate and raw-terminal templates, Stage-0 handoff, verifier, external audit, adversarial review, metadata, and checksums.

Aug 14, 20260 citations

Artian A1 Geometric-Holonomy Reference-Switch Theorem: A Prospective Berry-Carrier Test of the QTT Two-Clock Projection

Attar Ali

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- $\tfrac12$ loop, the ordinary Berry carrier is $\gamma_{\rm geo}=-\frac{\Omega}{2}.$ That relation is retained as a shared geometry check. It is not assigned a direct $\cos(\pi/8)$ deficit. The paper shows why the raw ratio $\frac{\widehat\gamma_{\rm geo}}{-\Omega/2}$ 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: $\boxed{ R_{\rm geo,clk} = \frac{1}{\mathcal N_{\times}^{\rm ord}} \sqrt{ \frac{D_{\tau T}D_{T\tau}} {D_{\tau\tau}D_{TT}} }, \qquad D_{ab}=\sqrt{\left|Z_{ab}(+\Omega)Z_{ab}(-\Omega)\right|}. }$ Here $Z_{ab}$ is the fitted first complex fringe phasor and $\mathcal N_{\times}^{\rm ord}$ is a target-blind, independently certified ordinary cross-history map. The frozen alternatives are $H_{\rm ordinary}:R_{\rm geo,clk}=1, \qquad H_{\rm QTT\text{-}A1}:R_{\rm geo,clk}=\cos\!\left(\frac{\pi}{8}\right).$ 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 $T/\tau$ 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- $\tfrac12$ 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 $1-\cos\!\left(\frac{\pi}{8}\right) =0.0761204674887133\ldots$ requires $\sigma(R_{\rm geo,clk})\leq0.0152241$ 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 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-$\tfrac12$ loop, the ordinary Berry carrier is $\gamma_{\rm geo}=-\frac{\Omega}{2}.$ That relation is retained as a shared geometry check. It is not assigned a direct $\cos(\pi/8)$ deficit. The paper shows why the raw ratio $\frac{\widehat\gamma_{\rm geo}}{-\Omega/2}$ 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: \[ \boxed{ R_{\rm geo,clk} = \frac{1}{\mathcal N_{\times}^{\rm ord}} \sqrt{ \frac{D_{\tau T}D_{T\tau}} {D_{\tau\tau}D_{TT}} }, \qquad D_{ab}=\sqrt{\left|Z_{ab}(+\Omega)Z_{ab}(-\Omega)\right|}. } \] Here $Z_{ab}$ is the fitted first complex fringe phasor and $\mathcal N_{\times}^{\rm ord}$ is a target-blind, independently certified ordinary cross-history map. The frozen alternatives are \[ H_{\rm ordinary}:R_{\rm geo,clk}=1, \qquad H_{\rm QTT\text{-}A1}:R_{\rm geo,clk}=\cos\!\left(\frac{\pi}{8}\right). \] 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 $T/\tau$ 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-$\tfrac12$ 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 \[ 1-\cos\!\left(\frac{\pi}{8}\right) =0.0761204674887133\ldots \] requires $\sigma(R_{\rm geo,clk})\leq0.0152241$ 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.

Jul 29, 20262 citations

Artian A1 Quantum-Clock Reference-Switch Theorem: A Prospective Delocalized-Clock Test of the QTT Two-Clock Projection

Attar Ali

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 $\Delta\phi_{\rm clock}=\omega_0\Delta\tau.$ 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, $\tau\tau,\qquad \tau T,\qquad T\tau,\qquad TT.$ For each history and reversed proper-time geometry, the laboratory fits the first complex clock-coherence phasor and forms $D_{ab}=\sqrt{|Z_{ab}^{+}Z_{ab}^{-}|}.$ The registered reference-switch statistic is $\boxed{ R_{\rm qc,clk}= \frac{1}{\mathcal N_{\times}^{\rm ord}} \sqrt{\frac{D_{\tau T}D_{T\tau}} {D_{\tau\tau}D_{TT}}}.}$ After a target-blind ordinary cross-history map, the fixed prospective fork is $\boxed{ H_{\rm ordinary}:R_{\rm qc,clk}=1, \qquad H_{\rm QTT-A1}:R_{\rm qc,clk}=\cos\!\left(\frac{\pi}{8}\right).}$ The alternatives differ by 7.6120467%. A bare five-standard-deviation separation requires $\sigma(R_{\rm qc,clk})\leq0.0152241,$ 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 $\tau$ 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 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 $\Delta\phi_{\rm clock}=\omega_0\Delta\tau.$ 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, $\tau\tau,\qquad \tau T,\qquad T\tau,\qquad TT.$ For each history and reversed proper-time geometry, the laboratory fits the first complex clock-coherence phasor and forms $D_{ab}=\sqrt{|Z_{ab}^{+}Z_{ab}^{-}|}.$ The registered reference-switch statistic is \[ \boxed{ R_{\rm qc,clk}= \frac{1}{\mathcal N_{\times}^{\rm ord}} \sqrt{\frac{D_{\tau T}D_{T\tau}} {D_{\tau\tau}D_{TT}}}.} \] After a target-blind ordinary cross-history map, the fixed prospective fork is \[ \boxed{ H_{\rm ordinary}:R_{\rm qc,clk}=1, \qquad H_{\rm QTT-A1}:R_{\rm qc,clk}=\cos\!\left(\frac{\pi}{8}\right).} \] The alternatives differ by 7.6120467%. A bare five-standard-deviation separation requires \[\sigma(R_{\rm qc,clk})\leq0.0152241,\] 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 $\tau$ 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.

Jul 29, 20262 citations

QTT Dynamic-Circuit Completed-Record and Timing-Access Extension

Attar Ali

A Hardware-Ready Route to an Unprogrammed Record-to-Clock Test Dynamic circuits can already write mid-circuit outcomes, condition later operations, and erase coherent markers. This preregistered extension removes the control path that would make the result trivial: a physical record is written and retained, while an independently calibrated timing mode is read without allowing the record label to control its preparation, pulses, scheduler, or measurement basis. The completed-record camera is $\eta_T = F_{\rm joint}^{2} = F^2\!\left( \rho_{RME}^{\rm meas}, \rho_{RME}^{\rm ideal} \right),$ and the registered timing-access frontier is $\mathcal U_T^{\star} = \left|(1-\eta_T)\,\Upsilon_{\rm tr}+b_N\right|.$ The canonical branch, reachable only after every physical and statistical certificate passes, is $\boxed{ \mathcal U_T^{\star}=1-F_{\rm joint}^{2} }.$ The causal firewall is explicit: $\boxed{ R\nrightarrow C, \qquad M\nrightarrow C, \qquad E_{\rm mcm}\nrightarrow C }.$ Thirty activation gates precede any theory verdict. The starting external dynamic-circuit archive reproduces in 161/161 checks at maximum absolute discrepancy $1.11\times10^{-16}$ , but remains standard-quantum qualification only because it lacks the registered independent timing channel. All sixteen deliberate gate mutations force INELIGIBLE_NO_THEORY_VERDICT. The dynamic-circuit ladder counts named laboratory record carriers. It is not the A3 twenty-four-front White-Void family and has no verdict on A2 support, A3 cosmological source volume, or a universal 23 entropy coefficient. Immutable protocol seal: 30324c4b790ac2e7860910535df8a96a2975dd6d6e4e550ba8a2152af18f1968 Verification and status: 28/28 original protocol, classifier, mutation, and power checks passed. 9/9 Version 1.1 target-preservation checks passed. PUBLIC-PREREGISTRATION-SEALED NO-OBSERVATION-YET NO-TARGET-CHANGE-IN-V1.1 Version: 1.1 Concept DOI: 10.5281/zenodo.21904993 Author: Ali Attar Website: quantumtraction.org Reader anchors: Parent blind-test preregistration Source framework Observation as Access QTT Main Book External dynamic-circuit starting platform The Equation on the TombstoneA Hardware-Ready Route to an Unprogrammed Record-to-Clock Test Dynamic circuits can already write mid-circuit outcomes, condition later operations, and erase coherent markers. This preregistered extension removes the control path that would make the result trivial: a physical record is written and retained, while an independently calibrated timing mode is read without allowing the record label to control its preparation, pulses, scheduler, or measurement basis. The completed-record camera is \[ \eta_T = F_{\rm joint}^{2} = F^2\!\left( \rho_{RME}^{\rm meas}, \rho_{RME}^{\rm ideal} \right), \] and the registered timing-access frontier is \[ \mathcal U_T^{\star} = \left|(1-\eta_T)\,\Upsilon_{\rm tr}+b_N\right|. \] The canonical branch, reachable only after every physical and statistical certificate passes, is \[ \boxed{ \mathcal U_T^{\star}=1-F_{\rm joint}^{2} }. \] The causal firewall is explicit: \[ \boxed{ R\nrightarrow C, \qquad M\nrightarrow C, \qquad E_{\rm mcm}\nrightarrow C }. \] Thirty activation gates precede any theory verdict. The starting external dynamic-circuit archive reproduces in 161/161 checks at maximum absolute discrepancy $1.11\times10^{-16}$, but remains standard-quantum qualification only because it lacks the registered independent timing channel. All sixteen deliberate gate mutations force INELIGIBLE_NO_THEORY_VERDICT. The dynamic-circuit ladder counts named laboratory record carriers. It is not the A3 twenty-four-front White-Void family and has no verdict on A2 support, A3 cosmological source volume, or a universal 23 entropy coefficient. Immutable protocol seal: 30324c4b790ac2e7860910535df8a96a2975dd6d6e4e550ba8a2152af18f1968 Verification and status: 28/28 original protocol, classifier, mutation, and power checks passed. 9/9 Version 1.1 target-preservation checks passed. PUBLIC-PREREGISTRATION-SEALED NO-OBSERVATION-YET NO-TARGET-CHANGE-IN-V1.1 Version: 1.1 Concept DOI: 10.5281/zenodo.21904993 Author: Ali Attar Website: quantumtraction.org Reader anchors: Parent blind-test preregistration Source framework Observation as Access QTT Main Book External dynamic-circuit starting platform The Equation on the Tombstone

Aug 12, 20260 citations

Fourth-Face Talbot-Lau Completed-Event Preregistration: An Activation-Gated Blind Test of A7U Matter-Wave Transport

Attar Ali

Can a finite Talbot chamber produce a nonconstant visibility shape after the ordinary interferometer kernel is frozen? $\boxed{ \begin{aligned} H_0:&\ \mathbf y_\perp=0,\\ H_{\mathrm{A7U}}:&\ \mathbf y_\perp=P_{\mathrm{prof}}\mathbf g^{\mathrm{phys}},\\ g_r^{\mathrm{phys}}=&\ \log\left|\frac{\int_{\Delta v_r}W_r(v)B_1^{\mathrm{QM/env}}(v)F_1^{\mathrm{A7U}}(v)\,dv}{\int_{\Delta v_r}W_r(v)B_1^{\mathrm{QM/env}}(v)\,dv}\right|,\\ &\ \frac{\partial\mathbf g^{\mathrm{phys}}}{\partial\mathbf y}=0. \end{aligned}}$ Version: 1.2 State: Stage-0 sealed; physical target activation pending; observation pending Concept DOI: 10.5281/zenodo.22010227 Author: Ali Attar, ORCID 0009-0008-9931-2691 Version note: v1.2 is an append-only source-projector-camera scope upgrade. The historical v1.0.1 branch, source equations, seven-bin vector, thresholds, PDF hash, and protocol-seal hash remain preserved. The v1.1 calibration-orthogonality gate also remains unchanged. The new outer wrapper separates the sealed A7U source-harmonic verdict from any stronger interpretation as a measurement of the central Access-Law projector weight. This preregistration asks for a seven-bin, first-harmonic matter-wave shape, not a constant loss of fringe contrast. The source branch is fixed before observation, but the final laboratory prediction is legal only after the ordinary complex Talbot kernel, event weights, operating point, calibration uncertainty object, physics-generated tangent basis, covariance, extraction operator, and the apparatus proof of kappa = 1 are independently frozen. The finite source law is $\Delta_n(v)=\left\|n^2\frac{hL}{d^2mv}\right\|_{\mathbb Z},\qquad N_{\Gamma,n}=\left\lceil\Delta_n^{-1}\right\rceil,\qquad F_n^{\mathrm{A7U}}=\sqrt{1-2\kappa_n\frac{2}{N_{\Gamma,n}}\left(1-\frac{1}{N_{\Gamma,n}}\right)}.$ The release seals a high-precision source-only feasibility vector, but proves why that vector cannot be substituted for the physical instrument prediction. Complex Talbot coefficients must be combined inside each velocity-bin integral before taking their modulus. This is the central wrong-falsification firewall: source-only forecast ≠ physical instrument prediction ≠ observation. A central Access-Law interpretation requires the additional prospectively frozen certificate $W^\dagger M W=P_a, \qquad C_n^{\mathrm{obs}}=(1-\eta)C_{n,u}+\eta C_{n,a}, \qquad \frac{\partial(W,M,C_{n,u},C_{n,a})}{\partial\mathbf y}=0.$ Without it, the test still adjudicates the activated A7U Talbot-Lau branch, but the lawful projector label is INELIGIBLE_NO_ACCESS_LAW_ETA_VERDICT. This prevents both wrong falsification and false promotion without weakening the sealed test. The calibration-orthogonality gate is $U_{\mathrm{phys}}=[\mathbf 1,\partial_{\theta_1}\log|\bar B_1^0|,\ldots],\qquad R_{\mathrm{sens}}^{\mathrm{cal}}= \sqrt{(P_{\mathrm{phys}}\mathbf g^{\mathrm{phys}})^T (P_{\mathrm{phys}}\Sigma P_{\mathrm{phys}}^T)^+ (P_{\mathrm{phys}}\mathbf g^{\mathrm{phys}})}\ge5.$ If the apparatus or data packet does not pass every activation gate, the deterministic result is TARGET-NOT-ACTIVATED or INELIGIBLE_NO_THEORY_VERDICT. The source-only forecast is 96.51% linear in velocity, so a generic constant-only nuisance model is not sufficient; the activated mass, phase, velocity-width, grating, and separation derivatives must be projected explicitly. These pre-data gates cannot be altered after a null. A qualified null therefore remains a real scoped falsifier. The public Pedalino sodium-nanoparticle archive establishes that the high-mass Talbot-Lau platform is real and experimentally mature, but it does not contain the complete velocity-resolved visibility, covariance, ordinary-kernel, and path-provenance packet required for a retrospective execution. Its published ordinary theory curves share a fitted global contrast factor of 0.78, so a constant additional suppression is not separately identifiable. This is therefore a prospective sealed test, not an observation claim. Stable scientific anchors: A7U Molecular Visibility Transport A7U source framework Quantum Traction Theory: Main Book Pedalino et al., Nature experiment Public experimental archive QTT Observatory · DOI mapCan a finite Talbot chamber produce a nonconstant visibility shape after the ordinary interferometer kernel is frozen? \[ \boxed{ \begin{aligned} H_0:&\ \mathbf y_\perp=0,\\ H_{\mathrm{A7U}}:&\ \mathbf y_\perp=P_{\mathrm{prof}}\mathbf g^{\mathrm{phys}},\\ g_r^{\mathrm{phys}}=&\ \log\left|\frac{\int_{\Delta v_r}W_r(v)B_1^{\mathrm{QM/env}}(v)F_1^{\mathrm{A7U}}(v)\,dv}{\int_{\Delta v_r}W_r(v)B_1^{\mathrm{QM/env}}(v)\,dv}\right|,\\ &\ \frac{\partial\mathbf g^{\mathrm{phys}}}{\partial\mathbf y}=0. \end{aligned}} \] Version: 1.2 State: Stage-0 sealed; physical target activation pending; observation pending Concept DOI: 10.5281/zenodo.22010227 Author: Ali Attar, ORCID 0009-0008-9931-2691 Version note: v1.2 is an append-only source-projector-camera scope upgrade. The historical v1.0.1 branch, source equations, seven-bin vector, thresholds, PDF hash, and protocol-seal hash remain preserved. The v1.1 calibration-orthogonality gate also remains unchanged. The new outer wrapper separates the sealed A7U source-harmonic verdict from any stronger interpretation as a measurement of the central Access-Law projector weight. This preregistration asks for a seven-bin, first-harmonic matter-wave shape, not a constant loss of fringe contrast. The source branch is fixed before observation, but the final laboratory prediction is legal only after the ordinary complex Talbot kernel, event weights, operating point, calibration uncertainty object, physics-generated tangent basis, covariance, extraction operator, and the apparatus proof of kappa = 1 are independently frozen. The finite source law is \[ \Delta_n(v)=\left\|n^2\frac{hL}{d^2mv}\right\|_{\mathbb Z},\qquad N_{\Gamma,n}=\left\lceil\Delta_n^{-1}\right\rceil,\qquad F_n^{\mathrm{A7U}}=\sqrt{1-2\kappa_n\frac{2}{N_{\Gamma,n}}\left(1-\frac{1}{N_{\Gamma,n}}\right)}. \] The release seals a high-precision source-only feasibility vector, but proves why that vector cannot be substituted for the physical instrument prediction. Complex Talbot coefficients must be combined inside each velocity-bin integral before taking their modulus. This is the central wrong-falsification firewall: source-only forecast ≠ physical instrument prediction ≠ observation. A central Access-Law interpretation requires the additional prospectively frozen certificate \[ W^\dagger M W=P_a, \qquad C_n^{\mathrm{obs}}=(1-\eta)C_{n,u}+\eta C_{n,a}, \qquad \frac{\partial(W,M,C_{n,u},C_{n,a})}{\partial\mathbf y}=0. \] Without it, the test still adjudicates the activated A7U Talbot-Lau branch, but the lawful projector label is INELIGIBLE_NO_ACCESS_LAW_ETA_VERDICT. This prevents both wrong falsification and false promotion without weakening the sealed test. The calibration-orthogonality gate is \[ U_{\mathrm{phys}}=[\mathbf 1,\partial_{\theta_1}\log|\bar B_1^0|,\ldots],\qquad R_{\mathrm{sens}}^{\mathrm{cal}}= \sqrt{(P_{\mathrm{phys}}\mathbf g^{\mathrm{phys}})^T (P_{\mathrm{phys}}\Sigma P_{\mathrm{phys}}^T)^+ (P_{\mathrm{phys}}\mathbf g^{\mathrm{phys}})}\ge5. \] If the apparatus or data packet does not pass every activation gate, the deterministic result is TARGET-NOT-ACTIVATED or INELIGIBLE_NO_THEORY_VERDICT. The source-only forecast is 96.51% linear in velocity, so a generic constant-only nuisance model is not sufficient; the activated mass, phase, velocity-width, grating, and separation derivatives must be projected explicitly. These pre-data gates cannot be altered after a null. A qualified null therefore remains a real scoped falsifier. The public Pedalino sodium-nanoparticle archive establishes that the high-mass Talbot-Lau platform is real and experimentally mature, but it does not contain the complete velocity-resolved visibility, covariance, ordinary-kernel, and path-provenance packet required for a retrospective execution. Its published ordinary theory curves share a fitted global contrast factor of 0.78, so a constant additional suppression is not separately identifiable. This is therefore a prospective sealed test, not an observation claim. Stable scientific anchors: A7U Molecular Visibility Transport A7U source framework Quantum Traction Theory: Main Book Pedalino et al., Nature experiment Public experimental archive QTT Observatory · DOI map

Aug 19, 20263 citations

Artian's Physical Contact Transfer Test

Attar Ali

A preregistered one- and two-excitation trapped-ion benchmark $\boxed{p_\eta(\mathbf y\mid u)=\operatorname{Tr}[\mathcal I_{y_m,\eta}^{u_m}\circ\cdots\circ\mathcal I_{y_1,\eta}^{u_1}(\rho_\eta)].}$ One interaction, selected before the data, must predict several observations. This prospective trapped-ion protocol fixes one- and two-excitation time scans, relative-phase scans and an even-curvature null control. It uses 18 contexts, 62 complete raw-count coordinates and 900,000 initiated validation attempts. The same independently constructed contact supplies the time-transfer predictions $p_{10\to01}=\sin^2\Theta,\qquad p_{11\to11}=\cos^2(F\Theta).$ Preparation, detector response, physical insertion class and uncertainty are frozen in a separately timestamped laboratory capsule before acquisition. No validation-fitted exchange frequency, capacity, phase origin or contrast is allowed. Failed attempts and null outcomes remain in the count denominators. A sensitivity gate prevents an unresponsive detector from passing. The finite-sample analysis has separate rejection, equivalence, inconclusive and ineligible decisions. Its total conditional false-rejection budget is 5.7330314376 × 10−7, numerically the conventional two-sided five-sigma tail. This is a design threshold, not a reported discovery. Successful equivalence requires every probability coordinate to meet a five-percentage-point tolerance. Design-stage preregistration. This deposit fixes the test today. Independent apparatus qualification, a public or verifiably escrowed Stage B capsule and new validation observations remain required. The canonical branch is shared with matched microscopic QM; a finite-slot comparison tests only the independently selected physical models. The package includes the protocol, frozen design, count analyzer, synthetic verification, deliberately incomplete laboratory templates and exact checksums. Companion: QTT Physical Contact Selection and Predictive Transfer Theorem. Source dependencies: Completed-Event Transport and Quantum Coherence; QTT Main Book. Independent experimental context: Hou et al., Nature Physics (2024). Browse the corpus. The main PDF is the preview; the ZIP contains the full reconstruction package.A preregistered one- and two-excitation trapped-ion benchmark \[\boxed{p_\eta(\mathbf y\mid u)=\operatorname{Tr}[\mathcal I_{y_m,\eta}^{u_m}\circ\cdots\circ\mathcal I_{y_1,\eta}^{u_1}(\rho_\eta)].}\] One interaction, selected before the data, must predict several observations. This prospective trapped-ion protocol fixes one- and two-excitation time scans, relative-phase scans and an even-curvature null control. It uses 18 contexts, 62 complete raw-count coordinates and 900,000 initiated validation attempts. The same independently constructed contact supplies the time-transfer predictions \[p_{10\to01}=\sin^2\Theta,\qquad p_{11\to11}=\cos^2(F\Theta).\] Preparation, detector response, physical insertion class and uncertainty are frozen in a separately timestamped laboratory capsule before acquisition. No validation-fitted exchange frequency, capacity, phase origin or contrast is allowed. Failed attempts and null outcomes remain in the count denominators. A sensitivity gate prevents an unresponsive detector from passing. The finite-sample analysis has separate rejection, equivalence, inconclusive and ineligible decisions. Its total conditional false-rejection budget is 5.7330314376 × 10−7, numerically the conventional two-sided five-sigma tail. This is a design threshold, not a reported discovery. Successful equivalence requires every probability coordinate to meet a five-percentage-point tolerance. Design-stage preregistration. This deposit fixes the test today. Independent apparatus qualification, a public or verifiably escrowed Stage B capsule and new validation observations remain required. The canonical branch is shared with matched microscopic QM; a finite-slot comparison tests only the independently selected physical models. The package includes the protocol, frozen design, count analyzer, synthetic verification, deliberately incomplete laboratory templates and exact checksums. Companion: QTT Physical Contact Selection and Predictive Transfer Theorem. Source dependencies: Completed-Event Transport and Quantum Coherence; QTT Main Book. Independent experimental context: Hou et al., Nature Physics (2024). Browse the corpus. The main PDF is the preview; the ZIP contains the full reconstruction package.

Sep 26, 20261 citation

Can one physical access gate control both extractable work and a closed phase-space commutator without retuning? This record seals a prospective circuit-QED test of the QTT Access Intertwiner. Its paper-native master equation is [ \boxed{ \begin{aligned} w_j&:=\frac{\Delta\mathcal W_j}{\hbar\omega|\alpha|^2}=\eta_j,\ \mathcal R_{jk}^{\rm QTT} &=(1-\eta_j)+\eta_j e^{J\phi_k},\ \mathcal R_{jk}^{\rm QM}&=1,\ \frac{\partial(\eta_j,\phi_k)} {\partial\mathcal R_{jk}^{\rm target}}&=0. \end{aligned}} ] A bosonic microwave mode is prepared in the symmetric ensemble (|+\alpha\rangle) or (|-\alpha\rangle). The preparation bit is written into an authenticated physical register. A randomized hardware route either makes that record available during the terminal window or keeps it unavailable until afterward. The work branch is a physical qualification. If the bit is available, a conditional displacement returns the mode to vacuum and the normalized gross energy drop is (w_j=\eta_j). Standard information thermodynamics and QTT both expect that row; it is not counted as QTT-exclusive evidence. The second branch is the discriminator. Four calibrated displacements form a closed phase-space group commutator. Ordinary canonical quantum mechanics predicts the same normalized geometric phase for every idle access setting. QTT predicts the exact complex surface ((1-\eta)+\eta e^{J\phi}) from the same independently constructed central effect. Frozen design: five access settings: (0,1/4,1/2,3/4,1); four primary loop areas: (\pi/4,\pi/2,3\pi/4,\pi); positive and negative loop orientations; zero target-fitted QTT coefficients; one global complex-vector comparison under one frozen covariance; late-route, dummy-bit, matched-load, erasure, reversal, zero-area, state-transport, and complete-record controls. A theory verdict is legal only after an experiment-specific activation certificate freezes the physical effect, its complete terminal alphabet, the ordinary circuit model, all calibration quantities and covariances, crosstalk bounds, the work/loop route identity, and at least 90 percent power at a global one-sided five-sigma threshold before target data are opened. Status: STAGE-0 SEALED / PHYSICAL ACTIVATION PENDING / OBSERVATION PENDING. This is a test of a speculative new theory. No observation is claimed. Reader anchors: Observation as Access Artian Hamiltonian Framework QTT Main Book QTT Observatory QTT Derivation Atlas QTT Lexicon The PDF is the default preview. The reconstruction ZIP contains the LaTeX and Markdown sources, immutable protocol seal, frozen prediction surface, activation templates, data schemas, blind classifier, three adversarial reviews, scientific and render audits, verification receipt, and SHA-256 manifest.

\mathcal R_i(\omega)=|0\rangle\!\langle0|_i\otimes\operatorname{Tr}_i\omega,

Q_{\rm del}=2F_{\rm avg}(\mathcal N_{\rm del},\operatorname{id})-1, \qquad \boxed{F_e^{\rm del}=\frac{1+3Q_{\rm del}}4.}

Target-only and every smaller halo subwindow remain optimized counterfactuals. A physical reset, sham reset, hidden-record injection, boundary ladder, and complete terminal record are required before the recovery layer qualifies. Test B: does the memory verifier intertwine with an independent timing projector?

\boxed{W^\dagger M_eW=P_{\rm align}}, \qquad \eta_T=\operatorname{Tr}(\rho P_{\rm align}),

\mathcal U_T^\star =\inf 2\sqrt{\det\Sigma_{T\Omega}}.

On the certified canonical branch, the sealed QTT target is

\boxed{ \eta_T=F_e^{\rm del}, \qquad \mathcal U_T^\star=1-F_e^{\rm del}. }

No complement coefficient is fitted. Five fidelity corridors, a radius/depth ladder, one-third untouched holdouts, topology twins, full covariance, global five-sigma decisions, at least 95% planned power, and transfer to a second record technology are frozen before data. The external computation is a feasibility anchor, not the timing target An, Cao, and Cui report carrier-deletion recovery in a local kicked-Ising memory. Their result qualifies the plausibility of Test A. Their reported

Q=0.516

is explicitly forbidden from constructing Test B. The public source archive lacks the exact arrays and scripts, so exact replication remains pending. Five terminal outcomes INELIGIBLE_NO_THEORY_VERDICT REGISTERED_QTT_CONSEQUENCE_FALSIFIED QTT_CANDIDATE QUALIFIED_OTHER_OR_CROSS_CHANNEL_ANOMALY AMBIGUOUS_OR_UNDERPOWERED Any failed eligibility gate terminates without a theory verdict. A positive result requires the full multirung shape, not one selected point. An off-target anomaly is preserved rather than discarded or used as a post-hoc rescue. Immutable protocol seal eb0640b25c1d0bde56cacc7f25d9ce4304594833e4aa937ed50293a1faafc849 This is a separate sealed extension. It changes no target, threshold, classifier, protocol hash, or file in the parent test under concept DOI 10.5281/zenodo.21902885. Public anchors Completed-record fan-out and timing-access framework Observation as Access Quantum Traction Theory: Main Book External finite-window recovery paper The PDF is the default preview. The reconstruction archive contains the sealed JSON, classifier, eighteen-gate and raw-terminal templates, Stage-0 handoff, verifier, external audit, adversarial review, metadata, and checksums.

\tfrac12

loop, the ordinary Berry carrier is

\gamma_{\rm geo}=-\frac{\Omega}{2}.

That relation is retained as a shared geometry check. It is not assigned a direct

\cos(\pi/8)

deficit. The paper shows why the raw ratio

\frac{\widehat\gamma_{\rm geo}}{-\Omega/2}

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:

\boxed{ R_{\rm geo,clk} = \frac{1}{\mathcal N_{\times}^{\rm ord}} \sqrt{ \frac{D_{\tau T}D_{T\tau}} {D_{\tau\tau}D_{TT}} }, \qquad D_{ab}=\sqrt{\left|Z_{ab}(+\Omega)Z_{ab}(-\Omega)\right|}. }

Here

Z_{ab}

is the fitted first complex fringe phasor and

\mathcal N_{\times}^{\rm ord}

is a target-blind, independently certified ordinary cross-history map. The frozen alternatives are

H_{\rm ordinary}:R_{\rm geo,clk}=1, \qquad H_{\rm QTT\text{-}A1}:R_{\rm geo,clk}=\cos\!\left(\frac{\pi}{8}\right).

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/\tau

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-

\tfrac12

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\!\left(\frac{\pi}{8}\right) =0.0761204674887133\ldots

requires

\sigma(R_{\rm geo,clk})\leq0.0152241

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.

\Delta\phi_{\rm clock}=\omega_0\Delta\tau.

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,

\tau\tau,\qquad \tau T,\qquad T\tau,\qquad TT.

For each history and reversed proper-time geometry, the laboratory fits the first complex clock-coherence phasor and forms

D_{ab}=\sqrt{|Z_{ab}^{+}Z_{ab}^{-}|}.

The registered reference-switch statistic is

\boxed{ R_{\rm qc,clk}= \frac{1}{\mathcal N_{\times}^{\rm ord}} \sqrt{\frac{D_{\tau T}D_{T\tau}} {D_{\tau\tau}D_{TT}}}.}

After a target-blind ordinary cross-history map, the fixed prospective fork is

\boxed{ H_{\rm ordinary}:R_{\rm qc,clk}=1, \qquad H_{\rm QTT-A1}:R_{\rm qc,clk}=\cos\!\left(\frac{\pi}{8}\right).}

The alternatives differ by 7.6120467%. A bare five-standard-deviation separation requires

\sigma(R_{\rm qc,clk})\leq0.0152241,

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

\tau

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.

\eta_T = F_{\rm joint}^{2} = F^2\!\left( \rho_{RME}^{\rm meas}, \rho_{RME}^{\rm ideal} \right),

and the registered timing-access frontier is

\mathcal U_T^{\star} = \left|(1-\eta_T)\,\Upsilon_{\rm tr}+b_N\right|.

The canonical branch, reachable only after every physical and statistical certificate passes, is

\boxed{ \mathcal U_T^{\star}=1-F_{\rm joint}^{2} }.

The causal firewall is explicit:

\boxed{ R\nrightarrow C, \qquad M\nrightarrow C, \qquad E_{\rm mcm}\nrightarrow C }.

Thirty activation gates precede any theory verdict. The starting external dynamic-circuit archive reproduces in 161/161 checks at maximum absolute discrepancy

1.11\times10^{-16}

, but remains standard-quantum qualification only because it lacks the registered independent timing channel. All sixteen deliberate gate mutations force INELIGIBLE_NO_THEORY_VERDICT. The dynamic-circuit ladder counts named laboratory record carriers. It is not the A3 twenty-four-front White-Void family and has no verdict on A2 support, A3 cosmological source volume, or a universal 23 entropy coefficient. Immutable protocol seal: 30324c4b790ac2e7860910535df8a96a2975dd6d6e4e550ba8a2152af18f1968 Verification and status: 28/28 original protocol, classifier, mutation, and power checks passed. 9/9 Version 1.1 target-preservation checks passed. PUBLIC-PREREGISTRATION-SEALED NO-OBSERVATION-YET NO-TARGET-CHANGE-IN-V1.1 Version: 1.1 Concept DOI: 10.5281/zenodo.21904993 Author: Ali Attar Website: quantumtraction.org Reader anchors: Parent blind-test preregistration Source framework Observation as Access QTT Main Book External dynamic-circuit starting platform The Equation on the Tombstone

Can a finite Talbot chamber produce a nonconstant visibility shape after the ordinary interferometer kernel is frozen?

\boxed{ \begin{aligned} H_0:&\ \mathbf y_\perp=0,\\ H_{\mathrm{A7U}}:&\ \mathbf y_\perp=P_{\mathrm{prof}}\mathbf g^{\mathrm{phys}},\\ g_r^{\mathrm{phys}}=&\ \log\left|\frac{\int_{\Delta v_r}W_r(v)B_1^{\mathrm{QM/env}}(v)F_1^{\mathrm{A7U}}(v)\,dv}{\int_{\Delta v_r}W_r(v)B_1^{\mathrm{QM/env}}(v)\,dv}\right|,\\ &\ \frac{\partial\mathbf g^{\mathrm{phys}}}{\partial\mathbf y}=0. \end{aligned}}

Version: 1.2 State: Stage-0 sealed; physical target activation pending; observation pending Concept DOI: 10.5281/zenodo.22010227 Author: Ali Attar, ORCID 0009-0008-9931-2691 Version note: v1.2 is an append-only source-projector-camera scope upgrade. The historical v1.0.1 branch, source equations, seven-bin vector, thresholds, PDF hash, and protocol-seal hash remain preserved. The v1.1 calibration-orthogonality gate also remains unchanged. The new outer wrapper separates the sealed A7U source-harmonic verdict from any stronger interpretation as a measurement of the central Access-Law projector weight. This preregistration asks for a seven-bin, first-harmonic matter-wave shape, not a constant loss of fringe contrast. The source branch is fixed before observation, but the final laboratory prediction is legal only after the ordinary complex Talbot kernel, event weights, operating point, calibration uncertainty object, physics-generated tangent basis, covariance, extraction operator, and the apparatus proof of kappa = 1 are independently frozen. The finite source law is

\Delta_n(v)=\left\|n^2\frac{hL}{d^2mv}\right\|_{\mathbb Z},\qquad N_{\Gamma,n}=\left\lceil\Delta_n^{-1}\right\rceil,\qquad F_n^{\mathrm{A7U}}=\sqrt{1-2\kappa_n\frac{2}{N_{\Gamma,n}}\left(1-\frac{1}{N_{\Gamma,n}}\right)}.

The release seals a high-precision source-only feasibility vector, but proves why that vector cannot be substituted for the physical instrument prediction. Complex Talbot coefficients must be combined inside each velocity-bin integral before taking their modulus. This is the central wrong-falsification firewall: source-only forecast ≠ physical instrument prediction ≠ observation. A central Access-Law interpretation requires the additional prospectively frozen certificate

W^\dagger M W=P_a, \qquad C_n^{\mathrm{obs}}=(1-\eta)C_{n,u}+\eta C_{n,a}, \qquad \frac{\partial(W,M,C_{n,u},C_{n,a})}{\partial\mathbf y}=0.

Without it, the test still adjudicates the activated A7U Talbot-Lau branch, but the lawful projector label is INELIGIBLE_NO_ACCESS_LAW_ETA_VERDICT. This prevents both wrong falsification and false promotion without weakening the sealed test. The calibration-orthogonality gate is

U_{\mathrm{phys}}=[\mathbf 1,\partial_{\theta_1}\log|\bar B_1^0|,\ldots],\qquad R_{\mathrm{sens}}^{\mathrm{cal}}= \sqrt{(P_{\mathrm{phys}}\mathbf g^{\mathrm{phys}})^T (P_{\mathrm{phys}}\Sigma P_{\mathrm{phys}}^T)^+ (P_{\mathrm{phys}}\mathbf g^{\mathrm{phys}})}\ge5.

If the apparatus or data packet does not pass every activation gate, the deterministic result is TARGET-NOT-ACTIVATED or INELIGIBLE_NO_THEORY_VERDICT. The source-only forecast is 96.51% linear in velocity, so a generic constant-only nuisance model is not sufficient; the activated mass, phase, velocity-width, grating, and separation derivatives must be projected explicitly. These pre-data gates cannot be altered after a null. A qualified null therefore remains a real scoped falsifier. The public Pedalino sodium-nanoparticle archive establishes that the high-mass Talbot-Lau platform is real and experimentally mature, but it does not contain the complete velocity-resolved visibility, covariance, ordinary-kernel, and path-provenance packet required for a retrospective execution. Its published ordinary theory curves share a fitted global contrast factor of 0.78, so a constant additional suppression is not separately identifiable. This is therefore a prospective sealed test, not an observation claim. Stable scientific anchors: A7U Molecular Visibility Transport A7U source framework Quantum Traction Theory: Main Book Pedalino et al., Nature experiment Public experimental archive QTT Observatory · DOI map

A preregistered one- and two-excitation trapped-ion benchmark

\boxed{p_\eta(\mathbf y\mid u)=\operatorname{Tr}[\mathcal I_{y_m,\eta}^{u_m}\circ\cdots\circ\mathcal I_{y_1,\eta}^{u_1}(\rho_\eta)].}

One interaction, selected before the data, must predict several observations. This prospective trapped-ion protocol fixes one- and two-excitation time scans, relative-phase scans and an even-curvature null control. It uses 18 contexts, 62 complete raw-count coordinates and 900,000 initiated validation attempts. The same independently constructed contact supplies the time-transfer predictions

p_{10\to01}=\sin^2\Theta,\qquad p_{11\to11}=\cos^2(F\Theta).

Preparation, detector response, physical insertion class and uncertainty are frozen in a separately timestamped laboratory capsule before acquisition. No validation-fitted exchange frequency, capacity, phase origin or contrast is allowed. Failed attempts and null outcomes remain in the count denominators. A sensitivity gate prevents an unresponsive detector from passing. The finite-sample analysis has separate rejection, equivalence, inconclusive and ineligible decisions. Its total conditional false-rejection budget is 5.7330314376 × 10−7, numerically the conventional two-sided five-sigma tail. This is a design threshold, not a reported discovery. Successful equivalence requires every probability coordinate to meet a five-percentage-point tolerance. Design-stage preregistration. This deposit fixes the test today. Independent apparatus qualification, a public or verifiably escrowed Stage B capsule and new validation observations remain required. The canonical branch is shared with matched microscopic QM; a finite-slot comparison tests only the independently selected physical models. The package includes the protocol, frozen design, count analyzer, synthetic verification, deliberately incomplete laboratory templates and exact checksums. Companion: QTT Physical Contact Selection and Predictive Transfer Theorem. Source dependencies: Completed-Event Transport and Quantum Coherence; QTT Main Book. Independent experimental context: Hou et al., Nature Physics (2024). Browse the corpus. The main PDF is the preview; the ZIP contains the full reconstruction package.