Artian's Physical Contact Transfer Test

Attar Ali

Published Sep 26, 2026• 1 citation

Abstract

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.

DOI: 10.5281/zenodo.22981950

Related papers

QTT Physical Contact Selection and Predictive Transfer Theorem

Attar Ali

From independently qualified work to one interaction and several observations \[\boxed{L\ker B=\{0\}.}\] When does a device's independently specified work already determine its interaction? In a finite affine constructor, the answer is exact: every unresolved calibration direction must disappear from the observable interaction. The paper proves necessity and sufficiency, constructs a dual certificate, and counts the additional linear probes needed when selection fails. The QTT source-to-contact construction connects geometry, supported work, mode participation and the actual electrode waveform to a single coupling. That same coupling predicts one-excitation transfer, two-excitation redistribution, phase response and parity controls. A finite future-memory theorem identifies what must remain in the retained packet so that later operations cannot reveal something the model discarded. For independently specified insertion magnitudes, the cross-occupation prediction is \[P_{11}=\cos^2(F\Theta),\qquad F^2=f_{2,a}^2+f_{2,b}^2.\] For symmetric-slot modes, the corresponding frequency ratio obeys \[\boxed{\left(\frac{\Omega_2}{2\Omega_1}\right)^2=1-\frac{1}{2K_a}-\frac{1}{2K_b}.}\] Version 2.0 adds complete feasible-set selection, a harmonic three-dimensional drive, unequal-capacity transfer, and the full preparation-to-detector calculation. A cross-Kerr counterexample shows why a perfect one-excitation calibration alone cannot settle the two-excitation prediction. The package contains the manuscript, proofs, executable checks, synthetic examples and a reproducible audit of the public Hou trapped-ion tables. The selection and transfer results are proved within their stated finite classes. The canonical realization shares laboratory probabilities with matched microscopic quantum mechanics; finite-slot discrimination requires independently qualified physical capacities and instruments. The archive is a retrospective eligibility audit. The separate prospective test commits the measurement design before a laboratory supplies its physical capsule. Companion: Artian's Physical Contact Transfer Test. 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, 20266 citations

QTT Reference-Memory Composition Test: A Preregistered Shared, Fresh and Echo Benchmark

Attar Ali

Six frozen interference predictions, independent calibration and a count-preserving memory test \[\mathbf g_*=(1,c_*,2c_*^2-1,c_*^2,1,c_*^2),\qquad c_*=\cos\frac{\pi}{8}.\] Can a retained reference recover interference that two fresh references cannot? This prospective protocol freezes the signed coherence for six histories: null, single, shared forward, fresh forward, shared echo and fresh echo. The forward and echo memory contrasts are respectively minus and plus $\sin^2(\pi/8)=0.1464466094\ldots$. The paper derives the complete reference-partition map, specifies 24 history/phase settings, preserves every raw attempt including loss, and separates source coefficients from independent apparatus calibration. It fixes a disjoint training sample, 2.4 million validation attempts, simultaneous finite-sample rejection and equivalence criteria, and held-out scores against explicitly declared comparators. A second, independently timestamped laboratory capsule is required before validation data are acquired. What the test establishes. A qualified joint pass validates this QTT optical construction and its reference-memory pattern in the specified apparatus. The matched controlled-unitary quantum-mechanical model predicts the same pattern with the same calibration and no additional fitted parameters. Therefore this benchmark does not distinguish QTT from matched QM or independently establish an absolute clock. Any predictive advantage over a fitted memory-free reduction or history-specific harmonic fit is reported separately. Design-stage preregistration. The deposit includes the full paper, frozen machine-readable predictions, analysis code, independent algebra and mutation checks, synthetic operating checks, and exact reconstruction checksums. No new laboratory result is reported. The earlier 95.76% injected-template retention motivates count-preserving processing; it is neither a natural-signal detection nor an experimental correction factor. QTT source dependency: Balanced-Rail Optical Intertwining Theorem. The necessary mathematics is reproduced here. Related physical reference qualification: Physical-Terminal Reference Framework. The current PDF is the default preview; the ZIP contains the complete reconstruction package.

Sep 14, 20260 citations

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

Attar Ali

Jul 29, 20262 citations

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

Attar Ali

Jul 15, 20268 citations

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

Attar Ali

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

Sep 3, 20261 citation

Completed-Event Transport: A Reproducible Record-Deletion Benchmark on Trapped-Ion Data

Attar Ali

Testing how retained measurement records determine prediction performance \[\boxed{p(y,r\mid C)=\frac12\langle y|E_r(C)|y\rangle,\qquad \mathcal R_S-\mathcal R_R=\mathbb E[(q_R-q_S)^2]\ge0.}\] How much predictive information survives when earlier detector records are hidden? This two-platform empirical paper connects qualified completed-event transport to explicit joint probabilities, fixed information-deletion rules and measured prediction performance. In the superconducting recurrence archive, retaining four earlier measurements raises fifth-outcome prediction accuracy from 73.2183% to 82.2774%, across all 495 settings and 19.8 million archived trials. The gain over the latest reading alone is 2.4895 percentage points. No outcome probabilities, noise rates, gate angles or contrast normalizations are fitted. All seven record selections, unsupported histories and adverse settings are retained, and confidence calibration is evaluated separately from accuracy. The complete trapped-ion benchmark is preserved: 32,000 tree records from 6,400 hardware shots, five strengths, seven masks and 30 nested comparisons. Its primary calibration p=0.0862 and complementary p=0.0189 are both reported. The two experiments' sampling units and uncertainties are not pooled. The paper is written for scientists new to Quantum Traction Theory. A boxed fourth-face energy-capacity identity explains the proposed source picture; the additional transport, composition and sampling premises needed to construct detector predictions are stated. The archives test the resulting record instruments, not the factor 4 pi or a fundamental length directly. The displayed joint law describes the ion preparation-inference task; a sequential branch law handles recurrence, with the same prediction-loss identity. The matched ordinary quantum instruments have identical probabilities and the same zero outcome-fit burden. These are retrospective, reproducible source-to-record benchmarks, not a claim of experimental separation. A calibration-first follow-up specifies how an independently source-selected apparatus input could add predictive content. The reconstruction ZIP includes editable source, all derived probabilities and scores, checksum-pinned data acquisition, independent score checks and a complete two-platform replay. The PDF is the primary reading copy. Experimental archives: Feng and colleagues and Liu, Tornow, Kessler and Barkai. Source dependencies: Completed-Event Transport, Completed-Event Four-Capacity and Physical Contact Selection. Corpus navigation: DOI Map.

Sep 25, 20260 citations

Artian's Physical Contact Transfer Test

Attar Ali

Published Sep 26, 2026• 1 citation

Publisher

Abstract

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.

DOI: 10.5281/zenodo.22981950

Related papers

QTT Physical Contact Selection and Predictive Transfer Theorem

Attar Ali

From independently qualified work to one interaction and several observations $\boxed{L\ker B=\{0\}.}$ When does a device's independently specified work already determine its interaction? In a finite affine constructor, the answer is exact: every unresolved calibration direction must disappear from the observable interaction. The paper proves necessity and sufficiency, constructs a dual certificate, and counts the additional linear probes needed when selection fails. The QTT source-to-contact construction connects geometry, supported work, mode participation and the actual electrode waveform to a single coupling. That same coupling predicts one-excitation transfer, two-excitation redistribution, phase response and parity controls. A finite future-memory theorem identifies what must remain in the retained packet so that later operations cannot reveal something the model discarded. For independently specified insertion magnitudes, the cross-occupation prediction is $P_{11}=\cos^2(F\Theta),\qquad F^2=f_{2,a}^2+f_{2,b}^2.$ For symmetric-slot modes, the corresponding frequency ratio obeys $\boxed{\left(\frac{\Omega_2}{2\Omega_1}\right)^2=1-\frac{1}{2K_a}-\frac{1}{2K_b}.}$ Version 2.0 adds complete feasible-set selection, a harmonic three-dimensional drive, unequal-capacity transfer, and the full preparation-to-detector calculation. A cross-Kerr counterexample shows why a perfect one-excitation calibration alone cannot settle the two-excitation prediction. The package contains the manuscript, proofs, executable checks, synthetic examples and a reproducible audit of the public Hou trapped-ion tables. The selection and transfer results are proved within their stated finite classes. The canonical realization shares laboratory probabilities with matched microscopic quantum mechanics; finite-slot discrimination requires independently qualified physical capacities and instruments. The archive is a retrospective eligibility audit. The separate prospective test commits the measurement design before a laboratory supplies its physical capsule. Companion: Artian's Physical Contact Transfer Test. 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.From independently qualified work to one interaction and several observations \[\boxed{L\ker B=\{0\}.}\] When does a device's independently specified work already determine its interaction? In a finite affine constructor, the answer is exact: every unresolved calibration direction must disappear from the observable interaction. The paper proves necessity and sufficiency, constructs a dual certificate, and counts the additional linear probes needed when selection fails. The QTT source-to-contact construction connects geometry, supported work, mode participation and the actual electrode waveform to a single coupling. That same coupling predicts one-excitation transfer, two-excitation redistribution, phase response and parity controls. A finite future-memory theorem identifies what must remain in the retained packet so that later operations cannot reveal something the model discarded. For independently specified insertion magnitudes, the cross-occupation prediction is \[P_{11}=\cos^2(F\Theta),\qquad F^2=f_{2,a}^2+f_{2,b}^2.\] For symmetric-slot modes, the corresponding frequency ratio obeys \[\boxed{\left(\frac{\Omega_2}{2\Omega_1}\right)^2=1-\frac{1}{2K_a}-\frac{1}{2K_b}.}\] Version 2.0 adds complete feasible-set selection, a harmonic three-dimensional drive, unequal-capacity transfer, and the full preparation-to-detector calculation. A cross-Kerr counterexample shows why a perfect one-excitation calibration alone cannot settle the two-excitation prediction. The package contains the manuscript, proofs, executable checks, synthetic examples and a reproducible audit of the public Hou trapped-ion tables. The selection and transfer results are proved within their stated finite classes. The canonical realization shares laboratory probabilities with matched microscopic quantum mechanics; finite-slot discrimination requires independently qualified physical capacities and instruments. The archive is a retrospective eligibility audit. The separate prospective test commits the measurement design before a laboratory supplies its physical capsule. Companion: Artian's Physical Contact Transfer Test. 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, 20266 citations

QTT Reference-Memory Composition Test: A Preregistered Shared, Fresh and Echo Benchmark

Attar Ali

Six frozen interference predictions, independent calibration and a count-preserving memory test $\mathbf g_*=(1,c_*,2c_*^2-1,c_*^2,1,c_*^2),\qquad c_*=\cos\frac{\pi}{8}.$ Can a retained reference recover interference that two fresh references cannot? This prospective protocol freezes the signed coherence for six histories: null, single, shared forward, fresh forward, shared echo and fresh echo. The forward and echo memory contrasts are respectively minus and plus $\sin^2(\pi/8)=0.1464466094\ldots$ . The paper derives the complete reference-partition map, specifies 24 history/phase settings, preserves every raw attempt including loss, and separates source coefficients from independent apparatus calibration. It fixes a disjoint training sample, 2.4 million validation attempts, simultaneous finite-sample rejection and equivalence criteria, and held-out scores against explicitly declared comparators. A second, independently timestamped laboratory capsule is required before validation data are acquired. What the test establishes. A qualified joint pass validates this QTT optical construction and its reference-memory pattern in the specified apparatus. The matched controlled-unitary quantum-mechanical model predicts the same pattern with the same calibration and no additional fitted parameters. Therefore this benchmark does not distinguish QTT from matched QM or independently establish an absolute clock. Any predictive advantage over a fitted memory-free reduction or history-specific harmonic fit is reported separately. Design-stage preregistration. The deposit includes the full paper, frozen machine-readable predictions, analysis code, independent algebra and mutation checks, synthetic operating checks, and exact reconstruction checksums. No new laboratory result is reported. The earlier 95.76% injected-template retention motivates count-preserving processing; it is neither a natural-signal detection nor an experimental correction factor. QTT source dependency: Balanced-Rail Optical Intertwining Theorem. The necessary mathematics is reproduced here. Related physical reference qualification: Physical-Terminal Reference Framework. The current PDF is the default preview; the ZIP contains the complete reconstruction package.Six frozen interference predictions, independent calibration and a count-preserving memory test \[\mathbf g_*=(1,c_*,2c_*^2-1,c_*^2,1,c_*^2),\qquad c_*=\cos\frac{\pi}{8}.\] Can a retained reference recover interference that two fresh references cannot? This prospective protocol freezes the signed coherence for six histories: null, single, shared forward, fresh forward, shared echo and fresh echo. The forward and echo memory contrasts are respectively minus and plus $\sin^2(\pi/8)=0.1464466094\ldots$. The paper derives the complete reference-partition map, specifies 24 history/phase settings, preserves every raw attempt including loss, and separates source coefficients from independent apparatus calibration. It fixes a disjoint training sample, 2.4 million validation attempts, simultaneous finite-sample rejection and equivalence criteria, and held-out scores against explicitly declared comparators. A second, independently timestamped laboratory capsule is required before validation data are acquired. What the test establishes. A qualified joint pass validates this QTT optical construction and its reference-memory pattern in the specified apparatus. The matched controlled-unitary quantum-mechanical model predicts the same pattern with the same calibration and no additional fitted parameters. Therefore this benchmark does not distinguish QTT from matched QM or independently establish an absolute clock. Any predictive advantage over a fitted memory-free reduction or history-specific harmonic fit is reported separately. Design-stage preregistration. The deposit includes the full paper, frozen machine-readable predictions, analysis code, independent algebra and mutation checks, synthetic operating checks, and exact reconstruction checksums. No new laboratory result is reported. The earlier 95.76% injected-template retention motivates count-preserving processing; it is neither a natural-signal detection nor an experimental correction factor. QTT source dependency: Balanced-Rail Optical Intertwining Theorem. The necessary mathematics is reproduced here. Related physical reference qualification: Physical-Terminal Reference Framework. The current PDF is the default preview; the ZIP contains the complete reconstruction package.

Sep 14, 20260 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

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

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

Attar Ali

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

Sep 3, 20261 citation

Completed-Event Transport: A Reproducible Record-Deletion Benchmark on Trapped-Ion Data

Attar Ali

Testing how retained measurement records determine prediction performance $\boxed{p(y,r\mid C)=\frac12\langle y|E_r(C)|y\rangle,\qquad \mathcal R_S-\mathcal R_R=\mathbb E[(q_R-q_S)^2]\ge0.}$ How much predictive information survives when earlier detector records are hidden? This two-platform empirical paper connects qualified completed-event transport to explicit joint probabilities, fixed information-deletion rules and measured prediction performance. In the superconducting recurrence archive, retaining four earlier measurements raises fifth-outcome prediction accuracy from 73.2183% to 82.2774%, across all 495 settings and 19.8 million archived trials. The gain over the latest reading alone is 2.4895 percentage points. No outcome probabilities, noise rates, gate angles or contrast normalizations are fitted. All seven record selections, unsupported histories and adverse settings are retained, and confidence calibration is evaluated separately from accuracy. The complete trapped-ion benchmark is preserved: 32,000 tree records from 6,400 hardware shots, five strengths, seven masks and 30 nested comparisons. Its primary calibration p=0.0862 and complementary p=0.0189 are both reported. The two experiments' sampling units and uncertainties are not pooled. The paper is written for scientists new to Quantum Traction Theory. A boxed fourth-face energy-capacity identity explains the proposed source picture; the additional transport, composition and sampling premises needed to construct detector predictions are stated. The archives test the resulting record instruments, not the factor 4 pi or a fundamental length directly. The displayed joint law describes the ion preparation-inference task; a sequential branch law handles recurrence, with the same prediction-loss identity. The matched ordinary quantum instruments have identical probabilities and the same zero outcome-fit burden. These are retrospective, reproducible source-to-record benchmarks, not a claim of experimental separation. A calibration-first follow-up specifies how an independently source-selected apparatus input could add predictive content. The reconstruction ZIP includes editable source, all derived probabilities and scores, checksum-pinned data acquisition, independent score checks and a complete two-platform replay. The PDF is the primary reading copy. Experimental archives: Feng and colleagues and Liu, Tornow, Kessler and Barkai. Source dependencies: Completed-Event Transport, Completed-Event Four-Capacity and Physical Contact Selection. Corpus navigation: DOI Map.Testing how retained measurement records determine prediction performance \[\boxed{p(y,r\mid C)=\frac12\langle y|E_r(C)|y\rangle,\qquad \mathcal R_S-\mathcal R_R=\mathbb E[(q_R-q_S)^2]\ge0.}\] How much predictive information survives when earlier detector records are hidden? This two-platform empirical paper connects qualified completed-event transport to explicit joint probabilities, fixed information-deletion rules and measured prediction performance. In the superconducting recurrence archive, retaining four earlier measurements raises fifth-outcome prediction accuracy from 73.2183% to 82.2774%, across all 495 settings and 19.8 million archived trials. The gain over the latest reading alone is 2.4895 percentage points. No outcome probabilities, noise rates, gate angles or contrast normalizations are fitted. All seven record selections, unsupported histories and adverse settings are retained, and confidence calibration is evaluated separately from accuracy. The complete trapped-ion benchmark is preserved: 32,000 tree records from 6,400 hardware shots, five strengths, seven masks and 30 nested comparisons. Its primary calibration p=0.0862 and complementary p=0.0189 are both reported. The two experiments' sampling units and uncertainties are not pooled. The paper is written for scientists new to Quantum Traction Theory. A boxed fourth-face energy-capacity identity explains the proposed source picture; the additional transport, composition and sampling premises needed to construct detector predictions are stated. The archives test the resulting record instruments, not the factor 4 pi or a fundamental length directly. The displayed joint law describes the ion preparation-inference task; a sequential branch law handles recurrence, with the same prediction-loss identity. The matched ordinary quantum instruments have identical probabilities and the same zero outcome-fit burden. These are retrospective, reproducible source-to-record benchmarks, not a claim of experimental separation. A calibration-first follow-up specifies how an independently source-selected apparatus input could add predictive content. The reconstruction ZIP includes editable source, all derived probabilities and scores, checksum-pinned data acquisition, independent score checks and a complete two-platform replay. The PDF is the primary reading copy. Experimental archives: Feng and colleagues and Liu, Tornow, Kessler and Barkai. Source dependencies: Completed-Event Transport, Completed-Event Four-Capacity and Physical Contact Selection. Corpus navigation: DOI Map.

Sep 25, 20260 citations

From independently qualified work to one interaction and several observations

\boxed{L\ker B=\{0\}.}

When does a device's independently specified work already determine its interaction? In a finite affine constructor, the answer is exact: every unresolved calibration direction must disappear from the observable interaction. The paper proves necessity and sufficiency, constructs a dual certificate, and counts the additional linear probes needed when selection fails. The QTT source-to-contact construction connects geometry, supported work, mode participation and the actual electrode waveform to a single coupling. That same coupling predicts one-excitation transfer, two-excitation redistribution, phase response and parity controls. A finite future-memory theorem identifies what must remain in the retained packet so that later operations cannot reveal something the model discarded. For independently specified insertion magnitudes, the cross-occupation prediction is

P_{11}=\cos^2(F\Theta),\qquad F^2=f_{2,a}^2+f_{2,b}^2.

For symmetric-slot modes, the corresponding frequency ratio obeys

\boxed{\left(\frac{\Omega_2}{2\Omega_1}\right)^2=1-\frac{1}{2K_a}-\frac{1}{2K_b}.}

Version 2.0 adds complete feasible-set selection, a harmonic three-dimensional drive, unequal-capacity transfer, and the full preparation-to-detector calculation. A cross-Kerr counterexample shows why a perfect one-excitation calibration alone cannot settle the two-excitation prediction. The package contains the manuscript, proofs, executable checks, synthetic examples and a reproducible audit of the public Hou trapped-ion tables. The selection and transfer results are proved within their stated finite classes. The canonical realization shares laboratory probabilities with matched microscopic quantum mechanics; finite-slot discrimination requires independently qualified physical capacities and instruments. The archive is a retrospective eligibility audit. The separate prospective test commits the measurement design before a laboratory supplies its physical capsule. Companion: Artian's Physical Contact Transfer Test. 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.

Six frozen interference predictions, independent calibration and a count-preserving memory test

\mathbf g_*=(1,c_*,2c_*^2-1,c_*^2,1,c_*^2),\qquad c_*=\cos\frac{\pi}{8}.

Can a retained reference recover interference that two fresh references cannot? This prospective protocol freezes the signed coherence for six histories: null, single, shared forward, fresh forward, shared echo and fresh echo. The forward and echo memory contrasts are respectively minus and plus

\sin^2(\pi/8)=0.1464466094\ldots

. The paper derives the complete reference-partition map, specifies 24 history/phase settings, preserves every raw attempt including loss, and separates source coefficients from independent apparatus calibration. It fixes a disjoint training sample, 2.4 million validation attempts, simultaneous finite-sample rejection and equivalence criteria, and held-out scores against explicitly declared comparators. A second, independently timestamped laboratory capsule is required before validation data are acquired. What the test establishes. A qualified joint pass validates this QTT optical construction and its reference-memory pattern in the specified apparatus. The matched controlled-unitary quantum-mechanical model predicts the same pattern with the same calibration and no additional fitted parameters. Therefore this benchmark does not distinguish QTT from matched QM or independently establish an absolute clock. Any predictive advantage over a fitted memory-free reduction or history-specific harmonic fit is reported separately. Design-stage preregistration. The deposit includes the full paper, frozen machine-readable predictions, analysis code, independent algebra and mutation checks, synthetic operating checks, and exact reconstruction checksums. No new laboratory result is reported. The earlier 95.76% injected-template retention motivates count-preserving processing; it is neither a natural-signal detection nor an experimental correction factor. QTT source dependency: Balanced-Rail Optical Intertwining Theorem. The necessary mathematics is reproduced here. Related physical reference qualification: Physical-Terminal Reference Framework. The current PDF is the default preview; the ZIP contains the complete reconstruction package.

\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.

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.

Can an integer completed-event fingerprint move between independently calibrated matter-wave configurations exactly as the frozen transport law requires?

\boxed{ \begin{gathered} v_B=\Lambda_{AB}v_A,\qquad \Lambda_{AB}=\frac{L_Bd_A^2\mathcal B_A}{L_Ad_B^2\mathcal B_B},\\ N_{\Gamma,n}^{(B)}(\Lambda_{AB}v)=N_{\Gamma,n}^{(A)}(v),\qquad F_n^{(B)}(\Lambda_{AB}v)=F_n^{(A)}(v). \end{gathered}}

Executable joint-ensemble prediction. The fixed-mass formula is the monochromatic specialization. The physical prediction now integrates the source factor over each calibrated joint mass-velocity node inside the ordinary complex kernel. Both prediction and actual analysis inputs are bound to the full reviewed pre-data manifest. The source law and historical decision thresholds are unchanged. The current reconstruction preserves directory paths and includes regression tests for missing evidence, substituted covariance or tangents, and mass averaging. A design separation of five standard deviations is not an observed five-sigma discovery. Physical activation and observations remain pending. Version: 1.1 State: Source transport theorem closed; Stage-0 test sealed; configuration pair and physical target not activated; observation pending Concept DOI: 10.5281/zenodo.22282943 Author: Ali Attar, ORCID 0009-0008-9931-2691 This is the separate Test B companion to the single-configuration Fourth-Face Talbot-Lau preregistration. Test A remains unchanged. Test B asks a harder question: if a completed-event visibility fingerprint is real, does the entire integer structure move to the new velocity coordinates fixed by a controlled change of source mass, grating separation, or grating period? The registered source branch is n = 1 with kappaA = kappaB = 1. It contains zero target-fitted QTT parameters. Each of fourteen physical target components is built by inserting the frozen A7U factor inside the independently calibrated complex Talbot/environment kernel before taking the modulus. A source-only curve may never substitute for that physical prediction. The experiment must pass two pre-data design gates:

R_0\ge5,\qquad R_{\rm move}\ge5.

The first requires at least five-sigma projected separation from the ordinary null. The second requires at least five-sigma projected separation from a frozen competitor in which the same source-shaped feature stays at the old laboratory velocity coordinates. The configuration pair is selected deterministically from a complete candidate ledger using calibration-only inputs. Arbitrary post-data polynomial nuisances, fitted amplitudes, branch changes, and pair shopping are forbidden. The sealed fork is ordinary null versus transported A7U target versus non-migrating source-shaped competitor. Every activation field defaults false. An unactivated, underpowered, incorrectly mapped, or incompletely calibrated run returns INELIGIBLE_NO_THEORY_VERDICT; once every gate passes, a null remains a real scoped falsifier. A first primary match is only GREEN-TRANSPORT-CANDIDATE. Hard green requires the same frozen result in a sequestered holdout or a preregistered third configuration or species. This test directly adjudicates the A7U completed-event migration law. A stronger interpretation as a measurement of the Access-Law projector weight requires the additional frozen camera identities W†MW = Pa and Cobs = (1 - eta)Cu + eta Ca in both configurations. Without that certificate, the A7U verdict remains valid and the Access-Law eta verdict remains ineligible. The Pedalino sodium-nanoparticle experiment establishes the relevant platform class with more than 7,000 atoms, masses above 170,000 Da, and a three-grating optical Talbot-Lau interferometer. Its public archive does not execute this prospectively frozen two-configuration test. The published quantum and classical contrast curves also share one fitted global factor of 0.78, so that archive cannot identify a constant extra sector by itself. QTT is a speculative new theory. This record publishes a parameter-free prospective discriminator, full schemas, blind audit, adversarial mutation tests, protocol seal, and reconstruction source. It reports no observation and makes no claim of direct metrology of the completed-event four-volume. Scientific anchors: Single-configuration Fourth-Face Talbot-Lau Test A A7U Molecular Visibility Transport A7U source framework Quantum Traction Theory: Main Book Pedalino et al., Nature experiment Public experimental archive QTT Observatory · DOI map

Testing how retained measurement records determine prediction performance

\boxed{p(y,r\mid C)=\frac12\langle y|E_r(C)|y\rangle,\qquad \mathcal R_S-\mathcal R_R=\mathbb E[(q_R-q_S)^2]\ge0.}

How much predictive information survives when earlier detector records are hidden? This two-platform empirical paper connects qualified completed-event transport to explicit joint probabilities, fixed information-deletion rules and measured prediction performance. In the superconducting recurrence archive, retaining four earlier measurements raises fifth-outcome prediction accuracy from 73.2183% to 82.2774%, across all 495 settings and 19.8 million archived trials. The gain over the latest reading alone is 2.4895 percentage points. No outcome probabilities, noise rates, gate angles or contrast normalizations are fitted. All seven record selections, unsupported histories and adverse settings are retained, and confidence calibration is evaluated separately from accuracy. The complete trapped-ion benchmark is preserved: 32,000 tree records from 6,400 hardware shots, five strengths, seven masks and 30 nested comparisons. Its primary calibration p=0.0862 and complementary p=0.0189 are both reported. The two experiments' sampling units and uncertainties are not pooled. The paper is written for scientists new to Quantum Traction Theory. A boxed fourth-face energy-capacity identity explains the proposed source picture; the additional transport, composition and sampling premises needed to construct detector predictions are stated. The archives test the resulting record instruments, not the factor 4 pi or a fundamental length directly. The displayed joint law describes the ion preparation-inference task; a sequential branch law handles recurrence, with the same prediction-loss identity. The matched ordinary quantum instruments have identical probabilities and the same zero outcome-fit burden. These are retrospective, reproducible source-to-record benchmarks, not a claim of experimental separation. A calibration-first follow-up specifies how an independently source-selected apparatus input could add predictive content. The reconstruction ZIP includes editable source, all derived probabilities and scores, checksum-pinned data acquisition, independent score checks and a complete two-platform replay. The PDF is the primary reading copy. Experimental archives: Feng and colleagues and Liu, Tornow, Kessler and Barkai. Source dependencies: Completed-Event Transport, Completed-Event Four-Capacity and Physical Contact Selection. Corpus navigation: DOI Map.