QTT Record-Fan-Out Timing-Envelope Blind Test Preregistration

Attar Ali

Published Aug 12, 2026• 1 citation

Abstract

A sealed timing test can only be judged after the physical reference operator is independently admitted. This preregistration separates ordinary coherent recovery from its independent timing test. The sealed object contains the observable, projector pair, camera, covariance, point hypotheses, and kill rule: \[ \mathfrak T=(O,P,C,D,q,\Sigma,H_0,H_{\rm QTT},K). \] Version 1.2 adds the upstream R0 representation gate. Before any of the numerical decision gates are evaluated, the candidate timing effect must be a bounded, idempotent, central physical projector on a declared direct sum and must remain unchanged under passive coordinate-seam relabeling. \[ G_{\rm eligible}=0 \quad\Longrightarrow\quad \texttt{INELIGIBLE\_NO\_THEORY\_VERDICT}. \] The historical hypotheses, ratio orientation, thresholds, terminal labels, and original protocol hash remain intact. A coordinate artifact is neither evidence for nor falsification of QTT; it is a failed representation preflight.

DOI: 10.5281/zenodo.21902885

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

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Artian's Completed-Record Fan-Out and Timing-Access Reference Framework

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A timing signature is not physics until its reference operator survives a representation audit. \[ \boxed{ \mathcal C_V^\star=F_R^2, \qquad \mathcal U_T^\star=1-F_R^2, \qquad \mathcal C_V^\star+\mathcal U_T^\star=1 } \] This framework separates three objects that must not be merged: a completed historical event, the record support still accessible to a laboratory, and a separately calibrated timing observable. Standard quantum theory closes the optimized coherent-recovery envelope. QTT adds a distinct, falsifiable timing complement only after a physical intertwining certificate proves that the laboratory record operator and the central timing projector are the same physical object in two representations. A public 11,009-trace test of explanatory burden Version 1.4 executes the complete usable public archive associated with Gosling et al., Probing the memory of a superconducting qubit environment. Every trace is split chronologically into training, a discarded guard interval, and held-out testing. The ordinary one-TLS Solomon camera learns two rates per trace, while the memoryless comparator learns one. \[ \boxed{ \operatorname{median}\!\left( \frac{\mathrm{RMSE}_{0}-\mathrm{RMSE}_{\rm TLS}} {\mathrm{RMSE}_{0}} \right)=0.36015, \qquad P(\mathrm{TLS\ wins})=\frac{10{,}169}{11{,}009}=0.92370 } \] The fitted TLS camera is therefore a successful held-out effective model. Its resolved trajectory is not a parameter-free derivation: the values of $\Gamma_q$ and $\Gamma_{qt}$ are learned from each target-bearing trace's training segment. Version 1.4 makes that distinction machine-auditable through the target-fit burden vector \[ \boxed{ \mathbf B_M=(N_c,N_d,N_w,N_n,N_u,N_h), \qquad \mathbf B_M\ne\mathbf0 \Longrightarrow \text{the fitted output is not derived parameter-free.} } \] The QTT result A public QTT source statement from 12 November 2025, before the Gosling preprint, already required complete reset to erase distributed record support beyond the visible carrier. That statement contains no Gosling-fitted rate, hidden-mode count, target window, or trajectory coefficient. The resulting comparative verdict is \[ \boxed{ \texttt{QTT-ZERO-FIT-SOURCE-EXPLANATORY-VICTORY} \;/\; \texttt{TRAJECTORY-VERDICT-OPEN}. } \] This is a scientific victory at the source/ontology layer, not a claim that QTT has already predicted the same resolved qubit trajectory. The stronger same-observable verdict remains locked because the public archive does not independently provide the residual record fidelity $F_{\rm res}$, leakage diagnostic $D$, timing complement $\mathcal U_T$, or physical intertwiner $W$. The paper prints the exact next experiment that would close or falsify that bridge. Reproducibility 11,009 row-level held-out results are included. The 840 traces favoring or tying the memoryless camera are retained. No false significance is assigned to correlated sweep windows. All three official archive objects pass their published MD5 checks. The release verifier passes 30/30 scientific and provenance checks. Three adversarial reviews cover observable equality, leakage and selection, chronology, and claim scope. Version: 1.4 Concept DOI: 10.5281/zenodo.21902886 Author: Ali Attar Website: quantumtraction.org Reader anchors Completed-record timing blind test Dynamic-circuit record-timing extension Observation as Access Quantum Traction Theory: Main Book Gosling public data archive The PDF is the default preview. The reconstruction archive contains the LaTeX source, row-level CSV, public-data integrity receipt, chronology certificate, fit-burden certificate, analysis scripts, exact source checks, adversarial and render audits, metadata, and checksum manifest.

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QTT Record-Fan-Out Timing-Envelope Blind Test Preregistration

Attar Ali

Published Aug 12, 2026• 1 citation

Publisher

Abstract

A sealed timing test can only be judged after the physical reference operator is independently admitted. This preregistration separates ordinary coherent recovery from its independent timing test. The sealed object contains the observable, projector pair, camera, covariance, point hypotheses, and kill rule: [ \mathfrak T=(O,P,C,D,q,\Sigma,H_0,H_{\rm QTT},K). ] Version 1.2 adds the upstream R0 representation gate. Before any of the numerical decision gates are evaluated, the candidate timing effect must be a bounded, idempotent, central physical projector on a declared direct sum and must remain unchanged under passive coordinate-seam relabeling. [ G_{\rm eligible}=0 \quad\Longrightarrow\quad \texttt{INELIGIBLE_NO_THEORY_VERDICT}. ] The historical hypotheses, ratio orientation, thresholds, terminal labels, and original protocol hash remain intact. A coordinate artifact is neither evidence for nor falsification of QTT; it is a failed representation preflight.

DOI: 10.5281/zenodo.21902885

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

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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's Completed-Record Fan-Out and Timing-Access Reference Framework

Attar Ali

A timing signature is not physics until its reference operator survives a representation audit. $\boxed{ \mathcal C_V^\star=F_R^2, \qquad \mathcal U_T^\star=1-F_R^2, \qquad \mathcal C_V^\star+\mathcal U_T^\star=1 }$ This framework separates three objects that must not be merged: a completed historical event, the record support still accessible to a laboratory, and a separately calibrated timing observable. Standard quantum theory closes the optimized coherent-recovery envelope. QTT adds a distinct, falsifiable timing complement only after a physical intertwining certificate proves that the laboratory record operator and the central timing projector are the same physical object in two representations. A public 11,009-trace test of explanatory burden Version 1.4 executes the complete usable public archive associated with Gosling et al., Probing the memory of a superconducting qubit environment. Every trace is split chronologically into training, a discarded guard interval, and held-out testing. The ordinary one-TLS Solomon camera learns two rates per trace, while the memoryless comparator learns one. $\boxed{ \operatorname{median}\!\left( \frac{\mathrm{RMSE}_{0}-\mathrm{RMSE}_{\rm TLS}} {\mathrm{RMSE}_{0}} \right)=0.36015, \qquad P(\mathrm{TLS\ wins})=\frac{10{,}169}{11{,}009}=0.92370 }$ The fitted TLS camera is therefore a successful held-out effective model. Its resolved trajectory is not a parameter-free derivation: the values of $\Gamma_q$ and $\Gamma_{qt}$ are learned from each target-bearing trace's training segment. Version 1.4 makes that distinction machine-auditable through the target-fit burden vector $\boxed{ \mathbf B_M=(N_c,N_d,N_w,N_n,N_u,N_h), \qquad \mathbf B_M\ne\mathbf0 \Longrightarrow \text{the fitted output is not derived parameter-free.} }$ The QTT result A public QTT source statement from 12 November 2025, before the Gosling preprint, already required complete reset to erase distributed record support beyond the visible carrier. That statement contains no Gosling-fitted rate, hidden-mode count, target window, or trajectory coefficient. The resulting comparative verdict is $\boxed{ \texttt{QTT-ZERO-FIT-SOURCE-EXPLANATORY-VICTORY} \;/\; \texttt{TRAJECTORY-VERDICT-OPEN}. }$ This is a scientific victory at the source/ontology layer, not a claim that QTT has already predicted the same resolved qubit trajectory. The stronger same-observable verdict remains locked because the public archive does not independently provide the residual record fidelity $F_{\rm res}$ , leakage diagnostic $D$ , timing complement $\mathcal U_T$ , or physical intertwiner $W$ . The paper prints the exact next experiment that would close or falsify that bridge. Reproducibility 11,009 row-level held-out results are included. The 840 traces favoring or tying the memoryless camera are retained. No false significance is assigned to correlated sweep windows. All three official archive objects pass their published MD5 checks. The release verifier passes 30/30 scientific and provenance checks. Three adversarial reviews cover observable equality, leakage and selection, chronology, and claim scope. Version: 1.4 Concept DOI: 10.5281/zenodo.21902886 Author: Ali Attar Website: quantumtraction.org Reader anchors Completed-record timing blind test Dynamic-circuit record-timing extension Observation as Access Quantum Traction Theory: Main Book Gosling public data archive The PDF is the default preview. The reconstruction archive contains the LaTeX source, row-level CSV, public-data integrity receipt, chronology certificate, fit-burden certificate, analysis scripts, exact source checks, adversarial and render audits, metadata, and checksum manifest.A timing signature is not physics until its reference operator survives a representation audit. \[ \boxed{ \mathcal C_V^\star=F_R^2, \qquad \mathcal U_T^\star=1-F_R^2, \qquad \mathcal C_V^\star+\mathcal U_T^\star=1 } \] This framework separates three objects that must not be merged: a completed historical event, the record support still accessible to a laboratory, and a separately calibrated timing observable. Standard quantum theory closes the optimized coherent-recovery envelope. QTT adds a distinct, falsifiable timing complement only after a physical intertwining certificate proves that the laboratory record operator and the central timing projector are the same physical object in two representations. A public 11,009-trace test of explanatory burden Version 1.4 executes the complete usable public archive associated with Gosling et al., Probing the memory of a superconducting qubit environment. Every trace is split chronologically into training, a discarded guard interval, and held-out testing. The ordinary one-TLS Solomon camera learns two rates per trace, while the memoryless comparator learns one. \[ \boxed{ \operatorname{median}\!\left( \frac{\mathrm{RMSE}_{0}-\mathrm{RMSE}_{\rm TLS}} {\mathrm{RMSE}_{0}} \right)=0.36015, \qquad P(\mathrm{TLS\ wins})=\frac{10{,}169}{11{,}009}=0.92370 } \] The fitted TLS camera is therefore a successful held-out effective model. Its resolved trajectory is not a parameter-free derivation: the values of $\Gamma_q$ and $\Gamma_{qt}$ are learned from each target-bearing trace's training segment. Version 1.4 makes that distinction machine-auditable through the target-fit burden vector \[ \boxed{ \mathbf B_M=(N_c,N_d,N_w,N_n,N_u,N_h), \qquad \mathbf B_M\ne\mathbf0 \Longrightarrow \text{the fitted output is not derived parameter-free.} } \] The QTT result A public QTT source statement from 12 November 2025, before the Gosling preprint, already required complete reset to erase distributed record support beyond the visible carrier. That statement contains no Gosling-fitted rate, hidden-mode count, target window, or trajectory coefficient. The resulting comparative verdict is \[ \boxed{ \texttt{QTT-ZERO-FIT-SOURCE-EXPLANATORY-VICTORY} \;/\; \texttt{TRAJECTORY-VERDICT-OPEN}. } \] This is a scientific victory at the source/ontology layer, not a claim that QTT has already predicted the same resolved qubit trajectory. The stronger same-observable verdict remains locked because the public archive does not independently provide the residual record fidelity $F_{\rm res}$, leakage diagnostic $D$, timing complement $\mathcal U_T$, or physical intertwiner $W$. The paper prints the exact next experiment that would close or falsify that bridge. Reproducibility 11,009 row-level held-out results are included. The 840 traces favoring or tying the memoryless camera are retained. No false significance is assigned to correlated sweep windows. All three official archive objects pass their published MD5 checks. The release verifier passes 30/30 scientific and provenance checks. Three adversarial reviews cover observable equality, leakage and selection, chronology, and claim scope. Version: 1.4 Concept DOI: 10.5281/zenodo.21902886 Author: Ali Attar Website: quantumtraction.org Reader anchors Completed-record timing blind test Dynamic-circuit record-timing extension Observation as Access Quantum Traction Theory: Main Book Gosling public data archive The PDF is the default preview. The reconstruction archive contains the LaTeX source, row-level CSV, public-data integrity receipt, chronology certificate, fit-burden certificate, analysis scripts, exact source checks, adversarial and render audits, metadata, and checksum manifest.

Aug 12, 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

Experimental Verdict Governance for Quantum Traction Theory

Attar Ali

When does an experimental null actually count against a theory? An experimental verdict is meaningful only when the intended physical object was built, ordinary alternatives were controlled, the covariance and power were adequate, and the analysis was frozen before the target was opened. This paper turns those requirements into an executable governance object for Quantum Traction Theory (QTT). The registered test object is $\boxed{ \mathfrak T=(\mathcal O,\mathcal P,\mathcal C,\mathcal D,q,\Sigma, H_0,H_{\rm QTT},\mathcal K) }$ and its eligibility is the logical product $\boxed{ G_{\rm eligible} =G_{\rm physical}G_{\rm ordinary}G_{\rm covariance} G_{\rm power}G_{\rm chronology}. }$ If any gate is zero, the packet is ineligible and carries no theory verdict. If all gates pass, the executor must retain five distinct possibilities: registered falsification, QTT candidate, qualified other/cross-channel anomaly, underpowered result, or ineligible packet. A reproducible effect outside the primary channel is preserved rather than silently discarded or relabelled. $\boxed{ \text{protect against wrong falsification} \Longleftrightarrow \text{protect against post-result theory immunization}. }$ The paper also defines a scope lattice: failure of a registered access row does not automatically falsify a source theorem or the whole framework unless a prospectively printed dependency theorem proves that propagation. The same discipline prevents a favorable but ineligible result from becoming evidence. The audit applies this standard to the current deposited QTT test families and provides prospective successor specifications for the older A2 tabletop and HVP blind-lock packets without altering their frozen targets, hashes, or historical seals. Stable anchors: Concept DOI: 10.5281/zenodo.21775175 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org Included files: PDF paper, Version 1.0 Reconstruction ZIP containing LaTeX source, validator, audit table, example packet, metadata, render audit, and SHA-256 manifestWhen does an experimental null actually count against a theory? An experimental verdict is meaningful only when the intended physical object was built, ordinary alternatives were controlled, the covariance and power were adequate, and the analysis was frozen before the target was opened. This paper turns those requirements into an executable governance object for Quantum Traction Theory (QTT). The registered test object is \[ \boxed{ \mathfrak T=(\mathcal O,\mathcal P,\mathcal C,\mathcal D,q,\Sigma, H_0,H_{\rm QTT},\mathcal K) } \] and its eligibility is the logical product \[ \boxed{ G_{\rm eligible} =G_{\rm physical}G_{\rm ordinary}G_{\rm covariance} G_{\rm power}G_{\rm chronology}. } \] If any gate is zero, the packet is ineligible and carries no theory verdict. If all gates pass, the executor must retain five distinct possibilities: registered falsification, QTT candidate, qualified other/cross-channel anomaly, underpowered result, or ineligible packet. A reproducible effect outside the primary channel is preserved rather than silently discarded or relabelled. \[ \boxed{ \text{protect against wrong falsification} \Longleftrightarrow \text{protect against post-result theory immunization}. } \] The paper also defines a scope lattice: failure of a registered access row does not automatically falsify a source theorem or the whole framework unless a prospectively printed dependency theorem proves that propagation. The same discipline prevents a favorable but ineligible result from becoming evidence. The audit applies this standard to the current deposited QTT test families and provides prospective successor specifications for the older A2 tabletop and HVP blind-lock packets without altering their frozen targets, hashes, or historical seals. Stable anchors: Concept DOI: 10.5281/zenodo.21775175 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org Included files: PDF paper, Version 1.0 Reconstruction ZIP containing LaTeX source, validator, audit table, example packet, metadata, render audit, and SHA-256 manifest

Aug 3, 20260 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.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, 20261 citation

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

\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.

A timing signature is not physics until its reference operator survives a representation audit.

\boxed{ \mathcal C_V^\star=F_R^2, \qquad \mathcal U_T^\star=1-F_R^2, \qquad \mathcal C_V^\star+\mathcal U_T^\star=1 }

This framework separates three objects that must not be merged: a completed historical event, the record support still accessible to a laboratory, and a separately calibrated timing observable. Standard quantum theory closes the optimized coherent-recovery envelope. QTT adds a distinct, falsifiable timing complement only after a physical intertwining certificate proves that the laboratory record operator and the central timing projector are the same physical object in two representations. A public 11,009-trace test of explanatory burden Version 1.4 executes the complete usable public archive associated with Gosling et al., Probing the memory of a superconducting qubit environment. Every trace is split chronologically into training, a discarded guard interval, and held-out testing. The ordinary one-TLS Solomon camera learns two rates per trace, while the memoryless comparator learns one.

\boxed{ \operatorname{median}\!\left( \frac{\mathrm{RMSE}_{0}-\mathrm{RMSE}_{\rm TLS}} {\mathrm{RMSE}_{0}} \right)=0.36015, \qquad P(\mathrm{TLS\ wins})=\frac{10{,}169}{11{,}009}=0.92370 }

The fitted TLS camera is therefore a successful held-out effective model. Its resolved trajectory is not a parameter-free derivation: the values of

\Gamma_q

and

\Gamma_{qt}

are learned from each target-bearing trace's training segment. Version 1.4 makes that distinction machine-auditable through the target-fit burden vector

\boxed{ \mathbf B_M=(N_c,N_d,N_w,N_n,N_u,N_h), \qquad \mathbf B_M\ne\mathbf0 \Longrightarrow \text{the fitted output is not derived parameter-free.} }

The QTT result A public QTT source statement from 12 November 2025, before the Gosling preprint, already required complete reset to erase distributed record support beyond the visible carrier. That statement contains no Gosling-fitted rate, hidden-mode count, target window, or trajectory coefficient. The resulting comparative verdict is

\boxed{ \texttt{QTT-ZERO-FIT-SOURCE-EXPLANATORY-VICTORY} \;/\; \texttt{TRAJECTORY-VERDICT-OPEN}. }

This is a scientific victory at the source/ontology layer, not a claim that QTT has already predicted the same resolved qubit trajectory. The stronger same-observable verdict remains locked because the public archive does not independently provide the residual record fidelity

F_{\rm res}

, leakage diagnostic

D

, timing complement

\mathcal U_T

, or physical intertwiner

W

. The paper prints the exact next experiment that would close or falsify that bridge. Reproducibility 11,009 row-level held-out results are included. The 840 traces favoring or tying the memoryless camera are retained. No false significance is assigned to correlated sweep windows. All three official archive objects pass their published MD5 checks. The release verifier passes 30/30 scientific and provenance checks. Three adversarial reviews cover observable equality, leakage and selection, chronology, and claim scope. Version: 1.4 Concept DOI: 10.5281/zenodo.21902886 Author: Ali Attar Website: quantumtraction.org Reader anchors Completed-record timing blind test Dynamic-circuit record-timing extension Observation as Access Quantum Traction Theory: Main Book Gosling public data archive The PDF is the default preview. The reconstruction archive contains the LaTeX source, row-level CSV, public-data integrity receipt, chronology certificate, fit-burden certificate, analysis scripts, exact source checks, adversarial and render audits, metadata, and checksum manifest.

\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.

\boxed{ \mathfrak T=(\mathcal O,\mathcal P,\mathcal C,\mathcal D,q,\Sigma, H_0,H_{\rm QTT},\mathcal K) }

and its eligibility is the logical product

\boxed{ G_{\rm eligible} =G_{\rm physical}G_{\rm ordinary}G_{\rm covariance} G_{\rm power}G_{\rm chronology}. }

If any gate is zero, the packet is ineligible and carries no theory verdict. If all gates pass, the executor must retain five distinct possibilities: registered falsification, QTT candidate, qualified other/cross-channel anomaly, underpowered result, or ineligible packet. A reproducible effect outside the primary channel is preserved rather than silently discarded or relabelled.

\boxed{ \text{protect against wrong falsification} \Longleftrightarrow \text{protect against post-result theory immunization}. }

The paper also defines a scope lattice: failure of a registered access row does not automatically falsify a source theorem or the whole framework unless a prospectively printed dependency theorem proves that propagation. The same discipline prevents a favorable but ineligible result from becoming evidence. The audit applies this standard to the current deposited QTT test families and provides prospective successor specifications for the older A2 tabletop and HVP blind-lock packets without altering their frozen targets, hashes, or historical seals. Stable anchors: Concept DOI: 10.5281/zenodo.21775175 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org Included files: PDF paper, Version 1.0 Reconstruction ZIP containing LaTeX source, validator, audit table, example packet, metadata, render audit, and SHA-256 manifest

\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

|-\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.

\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