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

Attar Ali

Published Jul 29, 2026• 2 citations

Abstract

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.

DOI: 10.5281/zenodo.21674815

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Sep 26, 20261 citation

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

Attar Ali

Published Jul 29, 2026• 2 citations

Publisher

Abstract

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.

DOI: 10.5281/zenodo.21674815

Related papers

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

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A geometric phase can verify a loop without being mistaken for the clock effect under test. This paper isolates a clean experimental question in geometric quantum mechanics: can the same completed holonomy be read through two physically distinct terminal-reference architectures without confusing ordinary carrier geometry, calibration, or passive propagation with a new clock projection? For an adiabatic spin- $\tfrac12$ loop, the ordinary Berry carrier is $\gamma_{\rm geo}=-\frac{\Omega}{2}.$ That relation is retained as a shared geometry check. It is not assigned a direct $\cos(\pi/8)$ deficit. The paper shows why the raw ratio $\frac{\widehat\gamma_{\rm geo}}{-\Omega/2}$ has the target $1$ for both ordinary quantum mechanics and the registered QTT A1 readout statement. 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The resulting protocol is prospective and falsifiable: a qualified result compatible with one fixed target while excluding the other has a predeclared meaning; any topology, transfer, carrier, covariance, target-contamination, or power failure is ineligible for a theory verdict. The recommended first implementation is a polarized-neutron spin-echo or interferometric platform with a static helical magnetic-field loop. Its spin- $\tfrac12$ carrier, field-defined solid angle, and winding reversal provide an independently auditable geometry layer while the terminal-reference switch is tested separately. The fixed separation $1-\cos\!\left(\frac{\pi}{8}\right) =0.0761204674887133\ldots$ requires $\sigma(R_{\rm geo,clk})\leq0.0152241$ for a bare five-standard- deviation distinction; the laboratory design target is $0.005$ . Status: PASS_GEOMETRIC_CARRIER_HAS_INDEPENDENT_LOOP_GEOMETRY PASS_SAME_PLATFORM_BERRY_REFERENCE_SWITCH_IS_BOOK_NATIVE ARCHIVE_INELIGIBLE_NO_CROSSED_REFERENCE_HISTORIES PROSPECTIVE_TEST_READY Concept DOI: 10.5281/zenodo.21673340 Main book anchor: Quantum Traction Theory: Main Book v10.01, especially PDF pp. 159--172 and 889--892. Website: quantumtraction.org | Two Universes: time | Lexicon | Observatory | Corpus Tree Included files: PDF paper, Version 1.0 Complete reconstruction ZIP with LaTeX source, laboratory certificates, archival audit, synthetic cancellation fixture, verification scripts, render audit, and SHA-256 manifest Version 1.1: operation qualification and retained observations The numerical targets, ratio orientation, decision regions and historical seals are unchanged. A 22.5-degree or 45-degree component is no longer excluded by its angle alone: its physical transfer must be independently established. Common-operation cancellation and signal-preserving calibration are proved; both hypotheses must remain identifiable. Every acquired record is retained. After authorized unblinding, QTT-like, ordinary-like and unexpected outcomes are reported, including observations that do not qualify for a theory verdict. This is a prospective amendment, not a retrospective resealing of data. Clock, ruler and signal-recovery qualification. Both registered predictions are constructed at the raw detector with explicit proper-time, coordinate-time, worldline, ruler and synchronization conventions. Each relativistic effect is counted once. Independently calibrated corrections carry their uncertainties through the common comparison; the tested rows cannot train a normalization that forces either answer. Blind recovery is required separately for both alternatives at every predeclared operating setting. The inherited targets and decision rules remain fixed. The included design study makes sensitivity explicit: for the Two-Test Gram classifier, a total ratio uncertainty of 0.0013 gives approximately 88.9% QTT-branch and 94.1% ordinary-branch power under the stated ideal model. These are conditional detection probabilities, not probabilities that a theory is true, and each instrument retains its own classifier. The complete apparatus packet must be sealed before acquisition and target access; historical campaign rules remain preserved. Reconstruction entry point. Start with current/CURRENT_RELATIVISTIC_EXECUTION.md in the ZIP. The shared execution contract refers once to the development filename CURRENT_EXECUTION_RC.md; that reference means CURRENT_RELATIVISTIC_EXECUTION.md in this release. The packaged README names the correct file. This navigation correction does not change the deposited files, scientific requirements or historical seals.A geometric phase can verify a loop without being mistaken for the clock effect under test. This paper isolates a clean experimental question in geometric quantum mechanics: can the same completed holonomy be read through two physically distinct terminal-reference architectures without confusing ordinary carrier geometry, calibration, or passive propagation with a new clock projection? For an adiabatic spin-$\tfrac12$ loop, the ordinary Berry carrier is $\gamma_{\rm geo}=-\frac{\Omega}{2}.$ That relation is retained as a shared geometry check. It is not assigned a direct $\cos(\pi/8)$ deficit. The paper shows why the raw ratio $\frac{\widehat\gamma_{\rm geo}}{-\Omega/2}$ has the target $1$ for both ordinary quantum mechanics and the registered QTT A1 readout statement. The proposed discriminating object is instead a sealed four-history, first-phasor amplitude ratio: \[ \boxed{ R_{\rm geo,clk} = \frac{1}{\mathcal N_{\times}^{\rm ord}} \sqrt{ \frac{D_{\tau T}D_{T\tau}} {D_{\tau\tau}D_{TT}} }, \qquad D_{ab}=\sqrt{\left|Z_{ab}(+\Omega)Z_{ab}(-\Omega)\right|}. } \] Here $Z_{ab}$ is the fitted first complex fringe phasor and $\mathcal N_{\times}^{\rm ord}$ is a target-blind, independently certified ordinary cross-history map. The frozen alternatives are \[ H_{\rm ordinary}:R_{\rm geo,clk}=1, \qquad H_{\rm QTT\text{-}A1}:R_{\rm geo,clk}=\cos\!\left(\frac{\pi}{8}\right). \] The paper audits the historical neutron-spin and optical-fiber geometric-phase records. They establish useful holonomy carriers but do not contain the physical crossed $T/\tau$ terminal histories, target-blind transfer map, raw four phasors, or joint covariance needed for this statistic. No archival QTT confirmation is claimed. The resulting protocol is prospective and falsifiable: a qualified result compatible with one fixed target while excluding the other has a predeclared meaning; any topology, transfer, carrier, covariance, target-contamination, or power failure is ineligible for a theory verdict. The recommended first implementation is a polarized-neutron spin-echo or interferometric platform with a static helical magnetic-field loop. Its spin-$\tfrac12$ carrier, field-defined solid angle, and winding reversal provide an independently auditable geometry layer while the terminal-reference switch is tested separately. The fixed separation \[ 1-\cos\!\left(\frac{\pi}{8}\right) =0.0761204674887133\ldots \] requires $\sigma(R_{\rm geo,clk})\leq0.0152241$ for a bare five-standard- deviation distinction; the laboratory design target is $0.005$. Status: PASS_GEOMETRIC_CARRIER_HAS_INDEPENDENT_LOOP_GEOMETRY PASS_SAME_PLATFORM_BERRY_REFERENCE_SWITCH_IS_BOOK_NATIVE ARCHIVE_INELIGIBLE_NO_CROSSED_REFERENCE_HISTORIES PROSPECTIVE_TEST_READY Concept DOI: 10.5281/zenodo.21673340 Main book anchor: Quantum Traction Theory: Main Book v10.01, especially PDF pp. 159--172 and 889--892. Website: quantumtraction.org | Two Universes: time | Lexicon | Observatory | Corpus Tree Included files: PDF paper, Version 1.0 Complete reconstruction ZIP with LaTeX source, laboratory certificates, archival audit, synthetic cancellation fixture, verification scripts, render audit, and SHA-256 manifest Version 1.1: operation qualification and retained observations The numerical targets, ratio orientation, decision regions and historical seals are unchanged. A 22.5-degree or 45-degree component is no longer excluded by its angle alone: its physical transfer must be independently established. Common-operation cancellation and signal-preserving calibration are proved; both hypotheses must remain identifiable. Every acquired record is retained. After authorized unblinding, QTT-like, ordinary-like and unexpected outcomes are reported, including observations that do not qualify for a theory verdict. This is a prospective amendment, not a retrospective resealing of data. Clock, ruler and signal-recovery qualification. Both registered predictions are constructed at the raw detector with explicit proper-time, coordinate-time, worldline, ruler and synchronization conventions. Each relativistic effect is counted once. Independently calibrated corrections carry their uncertainties through the common comparison; the tested rows cannot train a normalization that forces either answer. Blind recovery is required separately for both alternatives at every predeclared operating setting. The inherited targets and decision rules remain fixed. The included design study makes sensitivity explicit: for the Two-Test Gram classifier, a total ratio uncertainty of 0.0013 gives approximately 88.9% QTT-branch and 94.1% ordinary-branch power under the stated ideal model. These are conditional detection probabilities, not probabilities that a theory is true, and each instrument retains its own classifier. The complete apparatus packet must be sealed before acquisition and target access; historical campaign rules remain preserved. Reconstruction entry point. Start with current/CURRENT_RELATIVISTIC_EXECUTION.md in the ZIP. The shared execution contract refers once to the development filename CURRENT_EXECUTION_RC.md; that reference means CURRENT_RELATIVISTIC_EXECUTION.md in this release. The packaged README names the correct file. This navigation correction does not change the deposited files, scientific requirements or historical seals.

Jul 29, 20262 citations

Artian's Physical Terminal Reference Framework: A Carrier-Independent T-star/Tau Constructor Theorem for Activation-Gated Tests of QTT Axiom A1

Attar Ali

When do two clock labels become two physical experiments? An A1 reference-switch test is meaningful only if the two terminal labels are implemented by different physical write histories. This paper gives a carrier-independent answer. It represents the apparatus as a complete quantum instrument, reconstructs the laboratory write graph, and asks which physical event last wrote the durable record that survives to closure. Ontological reading. The primitive relevant to this theorem is the completed event: one finite source process closes and leaves a physical ledger record before a laboratory clock assigns its readout label. The candidate (T^\star) terminal carries a durable memory of that completion; the $\tau$ terminal is defined or overwritten by a laboratory reference. The experiment therefore does not compare two names for time. It compares two physical histories of what last wrote the terminal record. The candidate source terminal is defined without using the desired result: $\boxed{ \mathfrak T_{T^\star}: C_E=1,\quad \Xi_L\le\epsilon_L,\quad \Xi_S\ge\eta_S,\quad M_S\ \text{continuous},\quad N_{\rm rec}=0,\quad N_{\rm proj}=1 }$ Here (C_E) certifies a completed source event, (Xi_L) bounds laboratory write susceptibility, (Xi_S) proves that the surviving record still depends on the source memory, (N_{\rm rec}=0) forbids a later reference overwrite, and (N_{\rm proj}=1) permits one final basis-selecting readout. Ordinary free evolution does not pass this constructor. Fifteen predeclared gates compute one activation bit: $\boxed{ G_{\rm PT}=\prod_{j=1}^{15}P_j }$ $\boxed{ G_{\rm PT}=1 \Longrightarrow \begin{cases} R_{\rm clk}^{\rm ordinary}=1,\\[1mm] R_{\rm clk}^{\rm QTT-A1} =\cos^q\!\left(\frac{\pi}{8}\right), \end{cases} \qquad G_{\rm PT}=0 \Longrightarrow \texttt{INELIGIBLE\_NO\_THEORY\_VERDICT} }$ The detector degree (q) is derived and frozen before target data. A four-history experiment then tests the crossing character ((0,1,1,0)), with the geometric-mean estimator $\boxed{ R_{\rm clk} = \sqrt{ \frac{|D_{\tau T^\star}D_{T^\star\tau}|} {|D_{\tau\tau}D_{T^\star T^\star}|} } \frac{1}{C_K N_\times^{\rm ordinary}} }$ The framework proves that software relabelling, passive data reduction, a dark interval, and zero laboratory-write rank by themselves cannot create a second clock terminal. It also makes any apparatus containing a programmed (22.5^\circ), (45^\circ), CHSH-standard, or target-equivalent overlap ineligible before unblinding. The theorem is the shared activation layer for matter-wave Sagnac, Faraday, Berry/holonomy, delocalized quantum-clock, monitored-recurrence, photon-storage, and related reference-switch tests. Platform qualification and empirical A1 judgment remain separate downstream tasks. Concept DOI: 10.5281/zenodo.21739215 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org · Lexicon · Derivation Atlas · ObservatoryWhen do two clock labels become two physical experiments? An A1 reference-switch test is meaningful only if the two terminal labels are implemented by different physical write histories. This paper gives a carrier-independent answer. It represents the apparatus as a complete quantum instrument, reconstructs the laboratory write graph, and asks which physical event last wrote the durable record that survives to closure. Ontological reading. The primitive relevant to this theorem is the completed event: one finite source process closes and leaves a physical ledger record before a laboratory clock assigns its readout label. The candidate (T^\star) terminal carries a durable memory of that completion; the $\tau$ terminal is defined or overwritten by a laboratory reference. The experiment therefore does not compare two names for time. It compares two physical histories of what last wrote the terminal record. The candidate source terminal is defined without using the desired result: \[ \boxed{ \mathfrak T_{T^\star}: C_E=1,\quad \Xi_L\le\epsilon_L,\quad \Xi_S\ge\eta_S,\quad M_S\ \text{continuous},\quad N_{\rm rec}=0,\quad N_{\rm proj}=1 } \] Here (C_E) certifies a completed source event, (Xi_L) bounds laboratory write susceptibility, (Xi_S) proves that the surviving record still depends on the source memory, (N_{\rm rec}=0) forbids a later reference overwrite, and (N_{\rm proj}=1) permits one final basis-selecting readout. Ordinary free evolution does not pass this constructor. Fifteen predeclared gates compute one activation bit: \[ \boxed{ G_{\rm PT}=\prod_{j=1}^{15}P_j } \] \[ \boxed{ G_{\rm PT}=1 \Longrightarrow \begin{cases} R_{\rm clk}^{\rm ordinary}=1,\\[1mm] R_{\rm clk}^{\rm QTT-A1} =\cos^q\!\left(\frac{\pi}{8}\right), \end{cases} \qquad G_{\rm PT}=0 \Longrightarrow \texttt{INELIGIBLE\_NO\_THEORY\_VERDICT} } \] The detector degree (q) is derived and frozen before target data. A four-history experiment then tests the crossing character ((0,1,1,0)), with the geometric-mean estimator \[ \boxed{ R_{\rm clk} = \sqrt{ \frac{|D_{\tau T^\star}D_{T^\star\tau}|} {|D_{\tau\tau}D_{T^\star T^\star}|} } \frac{1}{C_K N_\times^{\rm ordinary}} } \] The framework proves that software relabelling, passive data reduction, a dark interval, and zero laboratory-write rank by themselves cannot create a second clock terminal. It also makes any apparatus containing a programmed (22.5^\circ), (45^\circ), CHSH-standard, or target-equivalent overlap ineligible before unblinding. The theorem is the shared activation layer for matter-wave Sagnac, Faraday, Berry/holonomy, delocalized quantum-clock, monitored-recurrence, photon-storage, and related reference-switch tests. Platform qualification and empirical A1 judgment remain separate downstream tasks. Concept DOI: 10.5281/zenodo.21739215 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org · Lexicon · Derivation Atlas · Observatory

Aug 1, 20265 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.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, 20268 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.orgA 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, 20262 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.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 Physical Contact Transfer Test

Attar Ali

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

Sep 26, 20261 citation

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.

\tfrac12

loop, the ordinary Berry carrier is

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

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

\cos(\pi/8)

deficit. The paper shows why the raw ratio

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

has the target

1

for both ordinary quantum mechanics and the registered QTT A1 readout statement. The proposed discriminating object is instead a sealed four-history, first-phasor amplitude ratio:

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

Here

Z_{ab}

is the fitted first complex fringe phasor and

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

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

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

The paper audits the historical neutron-spin and optical-fiber geometric-phase records. They establish useful holonomy carriers but do not contain the physical crossed

T/\tau

terminal histories, target-blind transfer map, raw four phasors, or joint covariance needed for this statistic. No archival QTT confirmation is claimed. The resulting protocol is prospective and falsifiable: a qualified result compatible with one fixed target while excluding the other has a predeclared meaning; any topology, transfer, carrier, covariance, target-contamination, or power failure is ineligible for a theory verdict. The recommended first implementation is a polarized-neutron spin-echo or interferometric platform with a static helical magnetic-field loop. Its spin-

\tfrac12

carrier, field-defined solid angle, and winding reversal provide an independently auditable geometry layer while the terminal-reference switch is tested separately. The fixed separation

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

requires

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

for a bare five-standard- deviation distinction; the laboratory design target is

0.005

. Status: PASS_GEOMETRIC_CARRIER_HAS_INDEPENDENT_LOOP_GEOMETRY PASS_SAME_PLATFORM_BERRY_REFERENCE_SWITCH_IS_BOOK_NATIVE ARCHIVE_INELIGIBLE_NO_CROSSED_REFERENCE_HISTORIES PROSPECTIVE_TEST_READY Concept DOI: 10.5281/zenodo.21673340 Main book anchor: Quantum Traction Theory: Main Book v10.01, especially PDF pp. 159--172 and 889--892. Website: quantumtraction.org | Two Universes: time | Lexicon | Observatory | Corpus Tree Included files: PDF paper, Version 1.0 Complete reconstruction ZIP with LaTeX source, laboratory certificates, archival audit, synthetic cancellation fixture, verification scripts, render audit, and SHA-256 manifest Version 1.1: operation qualification and retained observations The numerical targets, ratio orientation, decision regions and historical seals are unchanged. A 22.5-degree or 45-degree component is no longer excluded by its angle alone: its physical transfer must be independently established. Common-operation cancellation and signal-preserving calibration are proved; both hypotheses must remain identifiable. Every acquired record is retained. After authorized unblinding, QTT-like, ordinary-like and unexpected outcomes are reported, including observations that do not qualify for a theory verdict. This is a prospective amendment, not a retrospective resealing of data. Clock, ruler and signal-recovery qualification. Both registered predictions are constructed at the raw detector with explicit proper-time, coordinate-time, worldline, ruler and synchronization conventions. Each relativistic effect is counted once. Independently calibrated corrections carry their uncertainties through the common comparison; the tested rows cannot train a normalization that forces either answer. Blind recovery is required separately for both alternatives at every predeclared operating setting. The inherited targets and decision rules remain fixed. The included design study makes sensitivity explicit: for the Two-Test Gram classifier, a total ratio uncertainty of 0.0013 gives approximately 88.9% QTT-branch and 94.1% ordinary-branch power under the stated ideal model. These are conditional detection probabilities, not probabilities that a theory is true, and each instrument retains its own classifier. The complete apparatus packet must be sealed before acquisition and target access; historical campaign rules remain preserved. Reconstruction entry point. Start with current/CURRENT_RELATIVISTIC_EXECUTION.md in the ZIP. The shared execution contract refers once to the development filename CURRENT_EXECUTION_RC.md; that reference means CURRENT_RELATIVISTIC_EXECUTION.md in this release. The packaged README names the correct file. This navigation correction does not change the deposited files, scientific requirements or historical seals.

\tau

terminal is defined or overwritten by a laboratory reference. The experiment therefore does not compare two names for time. It compares two physical histories of what last wrote the terminal record. The candidate source terminal is defined without using the desired result:

\boxed{ \mathfrak T_{T^\star}: C_E=1,\quad \Xi_L\le\epsilon_L,\quad \Xi_S\ge\eta_S,\quad M_S\ \text{continuous},\quad N_{\rm rec}=0,\quad N_{\rm proj}=1 }

Here (C_E) certifies a completed source event, (Xi_L) bounds laboratory write susceptibility, (Xi_S) proves that the surviving record still depends on the source memory, (N_{\rm rec}=0) forbids a later reference overwrite, and (N_{\rm proj}=1) permits one final basis-selecting readout. Ordinary free evolution does not pass this constructor. Fifteen predeclared gates compute one activation bit:

\boxed{ G_{\rm PT}=\prod_{j=1}^{15}P_j }

\boxed{ G_{\rm PT}=1 \Longrightarrow \begin{cases} R_{\rm clk}^{\rm ordinary}=1,\\[1mm] R_{\rm clk}^{\rm QTT-A1} =\cos^q\!\left(\frac{\pi}{8}\right), \end{cases} \qquad G_{\rm PT}=0 \Longrightarrow \texttt{INELIGIBLE\_NO\_THEORY\_VERDICT} }

The detector degree (q) is derived and frozen before target data. A four-history experiment then tests the crossing character ((0,1,1,0)), with the geometric-mean estimator

\boxed{ R_{\rm clk} = \sqrt{ \frac{|D_{\tau T^\star}D_{T^\star\tau}|} {|D_{\tau\tau}D_{T^\star T^\star}|} } \frac{1}{C_K N_\times^{\rm ordinary}} }

The framework proves that software relabelling, passive data reduction, a dark interval, and zero laboratory-write rank by themselves cannot create a second clock terminal. It also makes any apparatus containing a programmed (22.5^\circ), (45^\circ), CHSH-standard, or target-equivalent overlap ineligible before unblinding. The theorem is the shared activation layer for matter-wave Sagnac, Faraday, Berry/holonomy, delocalized quantum-clock, monitored-recurrence, photon-storage, and related reference-switch tests. Platform qualification and empirical A1 judgment remain separate downstream tasks. Concept DOI: 10.5281/zenodo.21739215 Main book: Quantum Traction Theory: Main Book v10.01 Website: quantumtraction.org · Lexicon · Derivation Atlas · Observatory

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.

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

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

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

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

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

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