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

Attar Ali

Published Aug 19, 2026• 3 citations
Publisher

Abstract

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

DOI
10.5281/zenodo.22010227

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Two-Configuration Talbot-Lau Feature-Transport Preregistration: A Blind Test of the A7U Completed-Event Migration Law

Attar Ali

Can an integer completed-event fingerprint move between independently calibrated matter-wave configurations exactly as the frozen transport law requires? \[ \boxed{ \begin{gathered} v_B=\Lambda_{AB}v_A,\qquad \Lambda_{AB}=\frac{L_Bd_A^2\mathcal B_A}{L_Ad_B^2\mathcal B_B},\\ N_{\Gamma,n}^{(B)}(\Lambda_{AB}v)=N_{\Gamma,n}^{(A)}(v),\qquad F_n^{(B)}(\Lambda_{AB}v)=F_n^{(A)}(v). \end{gathered}} \] Executable joint-ensemble prediction. The fixed-mass formula is the monochromatic specialization. The physical prediction now integrates the source factor over each calibrated joint mass-velocity node inside the ordinary complex kernel. Both prediction and actual analysis inputs are bound to the full reviewed pre-data manifest. The source law and historical decision thresholds are unchanged. The current reconstruction preserves directory paths and includes regression tests for missing evidence, substituted covariance or tangents, and mass averaging. A design separation of five standard deviations is not an observed five-sigma discovery. Physical activation and observations remain pending. Version: 1.1 State: Source transport theorem closed; Stage-0 test sealed; configuration pair and physical target not activated; observation pending Concept DOI: 10.5281/zenodo.22282943 Author: Ali Attar, ORCID 0009-0008-9931-2691 This is the separate Test B companion to the single-configuration Fourth-Face Talbot-Lau preregistration. Test A remains unchanged. Test B asks a harder question: if a completed-event visibility fingerprint is real, does the entire integer structure move to the new velocity coordinates fixed by a controlled change of source mass, grating separation, or grating period? The registered source branch is n = 1 with kappaA = kappaB = 1. It contains zero target-fitted QTT parameters. Each of fourteen physical target components is built by inserting the frozen A7U factor inside the independently calibrated complex Talbot/environment kernel before taking the modulus. A source-only curve may never substitute for that physical prediction. The experiment must pass two pre-data design gates: \[ R_0\ge5,\qquad R_{\rm move}\ge5. \] The first requires at least five-sigma projected separation from the ordinary null. The second requires at least five-sigma projected separation from a frozen competitor in which the same source-shaped feature stays at the old laboratory velocity coordinates. The configuration pair is selected deterministically from a complete candidate ledger using calibration-only inputs. Arbitrary post-data polynomial nuisances, fitted amplitudes, branch changes, and pair shopping are forbidden. The sealed fork is ordinary null versus transported A7U target versus non-migrating source-shaped competitor. Every activation field defaults false. An unactivated, underpowered, incorrectly mapped, or incompletely calibrated run returns INELIGIBLE_NO_THEORY_VERDICT; once every gate passes, a null remains a real scoped falsifier. A first primary match is only GREEN-TRANSPORT-CANDIDATE. Hard green requires the same frozen result in a sequestered holdout or a preregistered third configuration or species. This test directly adjudicates the A7U completed-event migration law. A stronger interpretation as a measurement of the Access-Law projector weight requires the additional frozen camera identities W†MW = Pa and Cobs = (1 - eta)Cu + eta Ca in both configurations. Without that certificate, the A7U verdict remains valid and the Access-Law eta verdict remains ineligible. The Pedalino sodium-nanoparticle experiment establishes the relevant platform class with more than 7,000 atoms, masses above 170,000 Da, and a three-grating optical Talbot-Lau interferometer. Its public archive does not execute this prospectively frozen two-configuration test. The published quantum and classical contrast curves also share one fitted global factor of 0.78, so that archive cannot identify a constant extra sector by itself. QTT is a speculative new theory. This record publishes a parameter-free prospective discriminator, full schemas, blind audit, adversarial mutation tests, protocol seal, and reconstruction source. It reports no observation and makes no claim of direct metrology of the completed-event four-volume. Scientific anchors: Single-configuration Fourth-Face Talbot-Lau Test A A7U Molecular Visibility Transport A7U source framework Quantum Traction Theory: Main Book Pedalino et al., Nature experiment Public experimental archive QTT Observatory · DOI map

•Sep 3, 2026•1 citation

A7U Molecular Visibility Transport: Closed Source Floor, Access Transport, and Existing-Data Consistency Rows

Attar Ali

A matter-wave visibility floor becomes physics only when a frozen source certificate produces a surviving experimental shape. The paper inserts the A7U source factor into the ordinary Talbot-Lau transport rather than replacing environmental decoherence: \[ B_n^{\rm QTT}(v) = B_n^{\rm QM/env}(v)F_n^{\rm A7U}(v), \qquad F_n^{\rm A7U}(v)=\left|1-\frac{2}{N_{\Gamma,n}^{\rm TL}(v)}\right|. \] Version 10.1 executes this factor inside the public Pedalino complex first-harmonic mass/velocity kernel. The ordinary public kernel gives chi-square 44.539 for 31 nominal degrees of freedom; the saturated A7U branch gives 70.439 under the same diagonal-error treatment and the same one-contrast profiling rule. The nominal branch is therefore a reproducible stressed diagnostic. Version 10.1 also closes the projector-harmonic type boundary. The A7U factor above is a source-conditioned harmonic transport coefficient. The Access-Law quantity eta = Tr(rho M) is the state weight of a bounded central projector. Their exact bridge is the sector-resolved Fourier camera \[ C_n^{\rm obs}=(1-\eta)C_{n,u}+\eta C_{n,a}. \] A single visibility does not identify eta generically. The simple rule Vobs/Vu = 1 - eta is exact only after a physical intertwiner, equal DC throughput, zero aligned-sector analyzed harmonic, independent ordinary camera, and full covariance are certified before the target row is opened. The public Pedalino archive does not contain those objects, so it remains a camera diagnostic and carries no Access-Law eta verdict. That result is not a sigma exclusion. The fixed curves are nonnested, and the public archive does not contain the full observation covariance or the target-blind physical calibration tangent packet required by the separately sealed Fourth-Face activation theorem. The lawful status is: Nominal public branch: stressed diagnostic.Theory verdict: ineligible.Blind A7U observation: pending. The release also closes the multi-operating-point rank-lift theorem. With a target-blind ordinary tangent matrix \(U_{\rm phys}\), full covariance \(\Sigma\), and frozen A7U shape \(g\), define \[ P_{\rm cal} = I-U_{\rm phys} \left(U_{\rm phys}^{T}\Sigma^{-1}U_{\rm phys}\right)^{+} U_{\rm phys}^{T}\Sigma^{-1}. \] The A7U shape is identifiable exactly when \[ P_{\rm cal}g\ne0 \quad\Longleftrightarrow\quad g\notin{\rm col}(U_{\rm phys}). \] This converts the present ambiguity into a finite experimental requirement: predeclare multiple operating points, freeze the physical calibration tangent space and full covariance before target-data access, and require calibrated sensitivity of at least five. Missing activation objects block favorable and adverse verdicts equally; a packet that passes before unblinding cannot be withdrawn after a qualified null. Concept DOI: 10.5281/zenodo.20796924 Fourth-Face test: 10.5281/zenodo.22010227 Main book: 10.5281/zenodo.17527179 Website: quantumtraction.org

•Jun 22, 2026•3 citations

Artian Absolute-Clock Two-Test Preregistration: Matter-Wave Sagnac and Faraday Polarization-Coherence Tests

Attar Ali

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: \[ R_d^{\rm obs} =\frac{1}{C_dN_d^{\rm ord}} \sqrt{\frac{|D_{\tau T}^{(d)}D_{T\tau}^{(d)}|} {|D_{\tau\tau}^{(d)}D_{TT}^{(d)}|}}. \] After physical activation, the frozen fork is \[ \boxed{ R_d^{\rm standard}=1, \qquad R_d^{\rm QTT}=\cos\!\left(\frac{\pi}{8}\right) =0.9238795325112867\ldots }. \] 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, \[ H_{\rm rot}^{\rm std} =H_0-\Omega\cdot(L+F+\ell_F) +H_{\rm RR}+H_Z+H_{\rm Stark}+H_{\rm trap} +H_{\rm bs}+H_{\rm pol}+\cdots, \] with the rotation-induced hyperfine row \[ \boxed{ H_{\rm RH}=-\Omega\cdot F, \qquad \delta\omega_{\rm RH}=-\Omega_{\parallel}\Delta m_F. } \] 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.

•Jul 15, 2026•8 citations

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.

•Aug 14, 2026•0 citations

Artian Monitored-Recurrence Reference-Switch Laboratory Protocol: A Preregistered, Activation-Gated A1 Test with First-Detection Resonances

Attar Ali

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, \[ y_{dj} = \log\!\left( \frac{\widehat x^{*}_{dLj}} {\widehat x^{*}_{dAj}} \right), \qquad \widehat\Delta = \frac{\mathbf 1^{\mathsf T}\Sigma_y^{-1}\mathbf y} {\mathbf 1^{\mathsf T}\Sigma_y^{-1}\mathbf 1}, \qquad \widehat R_{\rm MRRS}=e^{\widehat\Delta}. \] The two frozen point hypotheses are \[ H_0: \quad \Delta_0=0, \qquad R_0=1, \] \[ H_{A1}: \quad \Delta_{A1}=\log\!\cos\!\left(\frac{\pi}{8}\right) =-0.0791735919101875\ldots, \qquad R_{A1}=\cos\!\left(\frac{\pi}{8}\right) =0.9238795325112867\ldots . \] 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: \[ G_{\rm PT} = \prod_{i=1}^{15}P_i. \] 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 \(T^{\star}\) terminal. If any gate fails, the registered result is \[ G_{\rm PT}=0 \quad\Longrightarrow\quad \texttt{TARGET\_NOT\_ACTIVATED}. \] 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 \[ {\rm SE}(\widehat\Delta)\le 0.006. \] A registered point must also exclude the other by at least five standard deviations. A fresh 400+400 finite-horizon synthetic campaign gives \[ u_{\Delta}^{\rm synth}=0.0010808000, \qquad \frac{|\Delta_{A1}-\Delta_0|}{u_{\Delta}^{\rm synth}} =73.25. \] 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

•Jul 30, 2026•2 citations

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

Attar Ali

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.

•Sep 1, 2026•1 citation
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
Can an integer completed-event fingerprint move between independently calibrated matter-wave configurations exactly as the frozen transport law requires? vB=ΛABvA,ΛAB=LBdA2BALAdB2BB,NΓ,n(B)(ΛABv)=NΓ,n(A)(v),Fn(B)(ΛABv)=Fn(A)(v). \boxed{ \begin{gathered} v_B=\Lambda_{AB}v_A,\qquad \Lambda_{AB}=\frac{L_Bd_A^2\mathcal B_A}{L_Ad_B^2\mathcal B_B},\\ N_{\Gamma,n}^{(B)}(\Lambda_{AB}v)=N_{\Gamma,n}^{(A)}(v),\qquad F_n^{(B)}(\Lambda_{AB}v)=F_n^{(A)}(v). \end{gathered}} vB​=ΛAB​vA​,ΛAB​=LA​dB2​BB​LB​dA2​BA​​,NΓ,n(B)​(ΛAB​v)=NΓ,n(A)​(v),Fn(B)​(ΛAB​v)=Fn(A)​(v).​​ Executable joint-ensemble prediction. The fixed-mass formula is the monochromatic specialization. The physical prediction now integrates the source factor over each calibrated joint mass-velocity node inside the ordinary complex kernel. Both prediction and actual analysis inputs are bound to the full reviewed pre-data manifest. The source law and historical decision thresholds are unchanged. The current reconstruction preserves directory paths and includes regression tests for missing evidence, substituted covariance or tangents, and mass averaging. A design separation of five standard deviations is not an observed five-sigma discovery. Physical activation and observations remain pending. Version: 1.1 State: Source transport theorem closed; Stage-0 test sealed; configuration pair and physical target not activated; observation pending Concept DOI: 10.5281/zenodo.22282943 Author: Ali Attar, ORCID 0009-0008-9931-2691 This is the separate Test B companion to the single-configuration Fourth-Face Talbot-Lau preregistration. Test A remains unchanged. Test B asks a harder question: if a completed-event visibility fingerprint is real, does the entire integer structure move to the new velocity coordinates fixed by a controlled change of source mass, grating separation, or grating period? The registered source branch is n = 1 with kappaA = kappaB = 1. It contains zero target-fitted QTT parameters. Each of fourteen physical target components is built by inserting the frozen A7U factor inside the independently calibrated complex Talbot/environment kernel before taking the modulus. A source-only curve may never substitute for that physical prediction. The experiment must pass two pre-data design gates: R0≥5,Rmove≥5. R_0\ge5,\qquad R_{\rm move}\ge5. R0​≥5,Rmove​≥5. The first requires at least five-sigma projected separation from the ordinary null. The second requires at least five-sigma projected separation from a frozen competitor in which the same source-shaped feature stays at the old laboratory velocity coordinates. The configuration pair is selected deterministically from a complete candidate ledger using calibration-only inputs. Arbitrary post-data polynomial nuisances, fitted amplitudes, branch changes, and pair shopping are forbidden. The sealed fork is ordinary null versus transported A7U target versus non-migrating source-shaped competitor. Every activation field defaults false. An unactivated, underpowered, incorrectly mapped, or incompletely calibrated run returns INELIGIBLE_NO_THEORY_VERDICT; once every gate passes, a null remains a real scoped falsifier. A first primary match is only GREEN-TRANSPORT-CANDIDATE. Hard green requires the same frozen result in a sequestered holdout or a preregistered third configuration or species. This test directly adjudicates the A7U completed-event migration law. A stronger interpretation as a measurement of the Access-Law projector weight requires the additional frozen camera identities W†MW = Pa and Cobs = (1 - eta)Cu + eta Ca in both configurations. Without that certificate, the A7U verdict remains valid and the Access-Law eta verdict remains ineligible. The Pedalino sodium-nanoparticle experiment establishes the relevant platform class with more than 7,000 atoms, masses above 170,000 Da, and a three-grating optical Talbot-Lau interferometer. Its public archive does not execute this prospectively frozen two-configuration test. The published quantum and classical contrast curves also share one fitted global factor of 0.78, so that archive cannot identify a constant extra sector by itself. QTT is a speculative new theory. This record publishes a parameter-free prospective discriminator, full schemas, blind audit, adversarial mutation tests, protocol seal, and reconstruction source. It reports no observation and makes no claim of direct metrology of the completed-event four-volume. Scientific anchors: Single-configuration Fourth-Face Talbot-Lau Test A 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 matter-wave visibility floor becomes physics only when a frozen source certificate produces a surviving experimental shape. The paper inserts the A7U source factor into the ordinary Talbot-Lau transport rather than replacing environmental decoherence: BnQTT(v)=BnQM/env(v)FnA7U(v),FnA7U(v)=∣1−2NΓ,nTL(v)∣. B_n^{\rm QTT}(v) = B_n^{\rm QM/env}(v)F_n^{\rm A7U}(v), \qquad F_n^{\rm A7U}(v)=\left|1-\frac{2}{N_{\Gamma,n}^{\rm TL}(v)}\right|. BnQTT​(v)=BnQM/env​(v)FnA7U​(v),FnA7U​(v)=​1−NΓ,nTL​(v)2​​. Version 10.1 executes this factor inside the public Pedalino complex first-harmonic mass/velocity kernel. The ordinary public kernel gives chi-square 44.539 for 31 nominal degrees of freedom; the saturated A7U branch gives 70.439 under the same diagonal-error treatment and the same one-contrast profiling rule. The nominal branch is therefore a reproducible stressed diagnostic. Version 10.1 also closes the projector-harmonic type boundary. The A7U factor above is a source-conditioned harmonic transport coefficient. The Access-Law quantity eta = Tr(rho M) is the state weight of a bounded central projector. Their exact bridge is the sector-resolved Fourier camera Cnobs=(1−η)Cn,u+ηCn,a. C_n^{\rm obs}=(1-\eta)C_{n,u}+\eta C_{n,a}. Cnobs​=(1−η)Cn,u​+ηCn,a​. A single visibility does not identify eta generically. The simple rule Vobs/Vu = 1 - eta is exact only after a physical intertwiner, equal DC throughput, zero aligned-sector analyzed harmonic, independent ordinary camera, and full covariance are certified before the target row is opened. The public Pedalino archive does not contain those objects, so it remains a camera diagnostic and carries no Access-Law eta verdict. That result is not a sigma exclusion. The fixed curves are nonnested, and the public archive does not contain the full observation covariance or the target-blind physical calibration tangent packet required by the separately sealed Fourth-Face activation theorem. The lawful status is: Nominal public branch: stressed diagnostic.Theory verdict: ineligible.Blind A7U observation: pending. The release also closes the multi-operating-point rank-lift theorem. With a target-blind ordinary tangent matrix UphysU_{\rm phys}Uphys​, full covariance Σ\SigmaΣ, and frozen A7U shape ggg, define Pcal=I−Uphys(UphysTΣ−1Uphys)+UphysTΣ−1. P_{\rm cal} = I-U_{\rm phys} \left(U_{\rm phys}^{T}\Sigma^{-1}U_{\rm phys}\right)^{+} U_{\rm phys}^{T}\Sigma^{-1}. Pcal​=I−Uphys​(UphysT​Σ−1Uphys​)+UphysT​Σ−1. The A7U shape is identifiable exactly when Pcalg≠0⟺g∉col(Uphys). P_{\rm cal}g\ne0 \quad\Longleftrightarrow\quad g\notin{\rm col}(U_{\rm phys}). Pcal​g=0⟺g∈/col(Uphys​). This converts the present ambiguity into a finite experimental requirement: predeclare multiple operating points, freeze the physical calibration tangent space and full covariance before target-data access, and require calibrated sensitivity of at least five. Missing activation objects block favorable and adverse verdicts equally; a packet that passes before unblinding cannot be withdrawn after a qualified null. Concept DOI: 10.5281/zenodo.20796924 Fourth-Face test: 10.5281/zenodo.22010227 Main book: 10.5281/zenodo.17527179 Website: quantumtraction.org
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=1CdNdord∣DτT(d)DTτ(d)∣∣Dττ(d)DTT(d)∣. R_d^{\rm obs} =\frac{1}{C_dN_d^{\rm ord}} \sqrt{\frac{|D_{\tau T}^{(d)}D_{T\tau}^{(d)}|} {|D_{\tau\tau}^{(d)}D_{TT}^{(d)}|}}. Rdobs​=Cd​Ndord​1​∣Dττ(d)​DTT(d)​∣∣DτT(d)​DTτ(d)​∣​​. After physical activation, the frozen fork is Rdstandard=1,RdQTT=cos⁡ ⁣(π8)=0.9238795325112867…. \boxed{ R_d^{\rm standard}=1, \qquad R_d^{\rm QTT}=\cos\!\left(\frac{\pi}{8}\right) =0.9238795325112867\ldots }. 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+⋯ , H_{\rm rot}^{\rm std} =H_0-\Omega\cdot(L+F+\ell_F) +H_{\rm RR}+H_Z+H_{\rm Stark}+H_{\rm trap} +H_{\rm bs}+H_{\rm pol}+\cdots, Hrotstd​=H0​−Ω⋅(L+F+ℓF​)+HRR​+HZ​+HStark​+Htrap​+Hbs​+Hpol​+⋯, with the rotation-induced hyperfine row HRH=−Ω⋅F,δωRH=−Ω∥ΔmF. \boxed{ H_{\rm RH}=-\Omega\cdot F, \qquad \delta\omega_{\rm RH}=-\Omega_{\parallel}\Delta m_F. } 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.
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? Ri(ω)=∣0⟩ ⁣⟨0∣i⊗Tr⁡iω, \mathcal R_i(\omega)=|0\rangle\!\langle0|_i\otimes\operatorname{Tr}_i\omega, Ri​(ω)=∣0⟩⟨0∣i​⊗Tri​ω, Qdel=2Favg(Ndel,id⁡)−1,Fedel=1+3Qdel4. 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.} Qdel​=2Favg​(Ndel​,id)−1,Fedel​=41+3Qdel​​.​ 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? W†MeW=Palign,ηT=Tr⁡(ρPalign), \boxed{W^\dagger M_eW=P_{\rm align}}, \qquad \eta_T=\operatorname{Tr}(\rho P_{\rm align}), W†Me​W=Palign​​,ηT​=Tr(ρPalign​), UT⋆=inf⁡2det⁡ΣTΩ. \mathcal U_T^\star =\inf 2\sqrt{\det\Sigma_{T\Omega}}. UT⋆​=inf2detΣTΩ​​. On the certified canonical branch, the sealed QTT target is ηT=Fedel,UT⋆=1−Fedel. \boxed{ \eta_T=F_e^{\rm del}, \qquad \mathcal U_T^\star=1-F_e^{\rm del}. } ηT​=Fedel​,UT⋆​=1−Fedel​.​ 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=0.516Q=0.516Q=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.
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 ddd and preregistered transition jjj, the laboratory reports one dimensionless root ratio, ydj=log⁡ ⁣(x^dLj∗x^dAj∗),Δ^=1TΣy−1y1TΣy−11,R^MRRS=eΔ^. y_{dj} = \log\!\left( \frac{\widehat x^{*}_{dLj}} {\widehat x^{*}_{dAj}} \right), \qquad \widehat\Delta = \frac{\mathbf 1^{\mathsf T}\Sigma_y^{-1}\mathbf y} {\mathbf 1^{\mathsf T}\Sigma_y^{-1}\mathbf 1}, \qquad \widehat R_{\rm MRRS}=e^{\widehat\Delta}. ydj​=log(xdAj∗​xdLj∗​​),Δ=1TΣy−1​11TΣy−1​y​,RMRRS​=eΔ. The two frozen point hypotheses are H0:Δ0=0,R0=1, H_0: \quad \Delta_0=0, \qquad R_0=1, H0​:Δ0​=0,R0​=1, HA1:ΔA1=log⁡ ⁣cos⁡ ⁣(π8)=−0.0791735919101875…,RA1=cos⁡ ⁣(π8)=0.9238795325112867…. H_{A1}: \quad \Delta_{A1}=\log\!\cos\!\left(\frac{\pi}{8}\right) =-0.0791735919101875\ldots, \qquad R_{A1}=\cos\!\left(\frac{\pi}{8}\right) =0.9238795325112867\ldots . 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. G_{\rm PT} = \prod_{i=1}^{15}P_i. GPT​=∏i=115​Pi​. 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⋆T^{\star}T⋆ terminal. If any gate fails, the registered result is GPT=0⟹TARGET_NOT_ACTIVATED. G_{\rm PT}=0 \quad\Longrightarrow\quad \texttt{TARGET\_NOT\_ACTIVATED}. 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=1024N=1024N=1024, an 81-point primary scan, and 16,384 trajectories per point, role, device, and transition. The estimator is the full finite-NNN 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 0.0250.0250.025 in log space, and the primary design gate is SE(Δ^)≤0.006. {\rm SE}(\widehat\Delta)\le 0.006. 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,∣ΔA1−Δ0∣uΔsynth=73.25. u_{\Delta}^{\rm synth}=0.0010808000, \qquad \frac{|\Delta_{A1}-\Delta_0|}{u_{\Delta}^{\rm synth}} =73.25. 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-NNN 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
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 wj:=ΔWjℏω∣α∣2=ηj,RjkQTT=(1−ηj)+ηjeJϕk,RjkQM=1,∂(ηj,ϕk)∂Rjktarget=0. \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}} wj​RjkQTT​RjkQM​∂Rjktarget​∂(ηj​,ϕk​)​​:=ℏω∣α∣2ΔWj​​=ηj​,=(1−ηj​)+ηj​eJϕk​,=1,=0.​​ A bosonic microwave mode is prepared in the symmetric ensemble ∣+α⟩|+\alpha\rangle∣+α⟩ or ∣−α⟩|-\alpha\rangle∣−α⟩. 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 wj=ηjw_j=\eta_jwj​=ηj​. 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−η)+ηeJϕ(1-\eta)+\eta e^{J\phi}(1−η)+ηeJϕ from the same independently constructed central effect. Frozen design: five access settings: 0,1/4,1/2,3/4,10,1/4,1/2,3/4,10,1/4,1/2,3/4,1; four primary loop areas: π/4,π/2,3π/4,π\pi/4,\pi/2,3\pi/4,\piπ/4,π/2,3π/4,π; 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.