Attar Ali

Observation as Access: A Quantum Traction Theory Dissolution of the Measurement Problem

When does a laboratory record belong to the source, and when does it belong to the measurement camera? Source, physical access operation, and laboratory camera. The paper-native master equation keeps the source, the physical access operation, and the laboratory camera in their pr...

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

Can a finite Talbot chamber produce a nonconstant visibility shape after the ordinary interferometer kernel is frozen? \[ \boxed{ \begin{aligned} H_0:&\ \mathbf y_\perp=0,\\ H_{\mathrm{A7U}}:&\ \mathbf y_\perp=P_{\mathrm{prof}}\mathbf g^{\mathrm{phys}},\\ g_r^{\mathrm{phys}}=&\ \...

A7U Molecular Visibility Transport: From Certified Source Gap to Talbot-Lau Matter-Wave Shape and Row-Packet Execution

A matter-wave visibility floor becomes physics only when a frozen source certificate produces a surviving experimental shape. The paper inserts the A7U source factor into the ordinary Talbot-Lau transport rather than replacing environmental decoherence: \[ B_n^{\rm QTT}(v) = B_n^...

Observation as Access: A Quantum Traction Theory Dissolution of the Measurement Problem

When does a laboratory record belong to the source, and when does it belong to the measurement camera? Master equation: source, physical access operation, and laboratory camera. This paper treats observation as a finite access operation rather than an observer-dependent event: \[...

The Artian Keystone Audit

Which QTT numbers are pure, anchored, keystone-dependent, or structural? The Keystone Audit classifies every headline result before judging its numerical landing. Its paper-native master split remains \[ \boxed{ \mathcal R = \mathcal R_{\rm U}\sqcup \mathcal R_{\rm A}\sqcup \math...

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

A sealed timing test can only be judged after the physical reference operator is independently admitted. This preregistration separates ordinary coherent recovery from its independent timing test. The sealed object contains the observable, projector pair, camera, covariance, poin...

The Folman Phase Spine and the Operator-Complete pi/8 Reference-Switch Test

A passive coordinate seam is a negative control, not a physical reference switch. This paper develops a four-channel Gram-ratio test for an A1 reference switch. Its registered fork is simple: \[ H_{\rm std}:R_{\rm Gram}=1, \qquad H_{\rm QTT-A1}:R_{\rm Gram}=\cos\!\left(\frac{\pi}...

No-Go Theorem and Conditional Uniqueness for the Universal Endpoint Gain in Quantum Traction Theory: Tier-K Preregistration v1.0

Does a finite-capacity source law force the gravitational endpoint to be read at full gain? \[ \boxed{ \mathrm{A2+A5\!\text{-}\!X+A6+A7}\not\Rightarrow\chi_g=1, \qquad G_{\rm end}=\chi_gG_A,\quad 0\leq\chi_g\leq1, \qquad \mathrm{EFA\!\text{-}\!G1}\Longleftrightarrow\chi_g=1. } \]...

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

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 origi...

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

A Hardware-Ready Route to an Unprogrammed Record-to-Clock Test Dynamic circuits can already write mid-circuit outcomes, condition later operations, and erase coherent markers. This preregistered extension removes the control path that would make the result trivial: a physical rec...

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

When Does a Quantum Record Become a Timing Observable? This framework separates a reversible marker, an accessible memory, and a completed physical record. It then asks a sharper question: after the complete record packet is reconstructed, can the same independently measured reco...

Artian's Time Framework: The Arrow of Time, Quantized Now, Time Drift, Time Tilt, and the w-Address of Reality-Space-Time

What does a clock measure when history, endurance, and created volume are different ledgers? Version: 5.2 Concept DOI: 10.5281/zenodo.20761499 Author: Ali Attar Website: quantumtraction.org Main book: Quantum Traction Theory, concept DOI 10.5281/zenodo.17527179 This framework sep...

Artian's Entropy and Second-Law Reference Theorem: Completed-Record Persistence, Record-State Recurrence Separation, Typed Capacity Geometry, Anchored Modular Charge, Clausius Production, Surface Entropy, and Page-Capacity Consequences

Two entropy coordinates, one finite Second-Law cone This release separates the cumulative record written by completed source events from information lost through an observer's access map. The combined law is \[ \Sigma_{\rm QTT}[T_1,T_2] =k_B\big[N_{\rm rec}(T_2)-N_{\rm rec}(T_1)\...

Artian's HVP Source-Access Reference Framework

Which HVP object is the source, which one is the apparatus, and which one is only statistics? A resolved hadronic-vacuum-polarization test passes through several mathematically different layers before it becomes a laboratory verdict. This framework now types that full chain: \[ \...

Artian A2 Endurance and the Einstein-Field Infrared Theorem

From finite endurance currents to Einstein-field dynamics This paper asks a sharply typed question: when a finite completed-address ledger is read through an infrared metric camera, which field equation is forced, and which source receipts must be supplied before its coefficient...

Artian's Entropy and Second-Law Reference Theorem: Completed-Event Ledger Growth, Anchored Modular Charge, Clausius Production, Surface Entropy, and Page-Capacity Consequences

Where irreversibility enters a finite quantum record The local and global statements usually grouped under "the Second Law" are different mathematical objects. This paper keeps them separate and then shows how they combine. At one address, the anchored modular charge is \[ Q_w=2\...

Artian Fluid Mechanics: Navier-Stokes from Exact Finite-Address Conservation

From finite transport packets to the Navier-Stokes equation This paper asks what a fluid equation becomes when the continuum is not the source object. The primitive state is a finite graph of completed address events. Material is counted in Artian-mass units, \[ B_w=\frac{M_w}{m_...

Boltzmann Weighting from Finite Completed-Event Reservoirs: A Conditional QTT Reconstruction of the Canonical Distribution, the Role of k_B, and a Seven-Face Thermal Consistency Ledger

When does finite counting become the canonical Boltzmann law? This paper separates the microscopic support, the probability premise, the reservoir approximation, and the laboratory units map. A finite completed-event reservoir gives the exact subsystem marginal \[ p_a= \frac{g_a\...

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

A sealed phase-root test for two time-reference classes Version 2.02 of this preregistration asks one narrow experimental question: after the same monitored quantum system has passed through two physically qualified reference classes, does the location of a first-detection recurr...

Experimental Verdict Governance for Quantum Traction Theory

When does an experimental null actually count against a theory? An experimental verdict is meaningful only when the intended physical object was built, ordinary alternatives were controlled, the covariance and power were adequate, and the analysis was frozen before the target was...