Attar Ali

QTT Completed-Event Transport and Quantum Coherence

Real-dial dynamics, conditional interactions, and optical interference \[G-F^{T}GF=L^{T}ML,\qquad L=0,\quad FJ=JF\quad\Longrightarrow\quad U_F^\dagger U_F=I.\] When does completed-record transport become unitary quantum evolution? A positive counting metric, a fixed coherent enco...

QTT Completed-Event Transport and Quantum Coherence

Real-dial dynamics, conditional interactions, and optical interference \[G-F^{T}GF=L^{T}ML,\qquad L=0,\quad FJ=JF\quad\Longrightarrow\quad U_F^\dagger U_F=I.\] When does completed-record transport become unitary quantum evolution? A positive counting metric, a fixed coherent enco...

QTT Completed-Event Transport and Quantum Coherence

Real-dial dynamics, conditional interactions, and optical interference \[G-F^{T}GF=L^{T}ML,\qquad L=0,\quad FJ=JF\quad\Longrightarrow\quad U_F^\dagger U_F=I.\] When does a completed-record transport become a unitary quantum evolution? This paper constructs the amplitude map from...

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

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_{\G...

Artian's Completed-Event Four-Capacity Theorem

The finite source packet behind the fourth face of the energy-capacity identity Version: 1.0 Concept DOI: 10.5281/zenodo.22131828 Author: Ali Attar Website: quantumtraction.org \[ \boxed{ \Delta V_A^{(4)} =24\left(\frac{\pi}{6}\ell_A^3\right)\ell_A =4\pi\ell_A^4, \qquad E_*=\rho_...

Planck-length metrology without Newton's constant: a zero-fit weak-sector reconstruction and adversarial provenance audit

A weak-sector ruler for the Planck scale, audited from muon decay to SI metres Version: 8.1 Concept DOI: 10.5281/zenodo.21190193 Author: Ali Attar Website: quantumtraction.org \[ \boxed{ \ell_A^{(\gamma H)} =2^{3/4}\hbar c\,q_H\,\mathcal R_H^{\rm EW}\sqrt{G_F}. } \] This restrict...

Artian Source-Only SI Endpoint Bridge Theorem

Reading the Planck-scale endpoint into SI units without a hidden physics row Version: 3.1 Concept DOI: 10.5281/zenodo.20936013 Author: Ali Attar Website: quantumtraction.org \[ \boxed{ \mathfrak B_{\rm SI}^{A5X/A6/A7}: (\ell_A,\hbar,c)\longmapsto \left(\tilde t_A=\frac{\ell_A}{c}...

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: 5.3 Concept DOI: 10.5281/zenodo.20761499 Author: Ali Attar Website: quantumtraction.org \[ \boxed{ \begin{aligned} N_{\rm SQ}^{A2}(N_T)&=BN_T,&N_{\rm pix}^{A2}(N_T)&=24BN_T,\\ N_...

Artian Capacity Endpoint Without G: A Keystone-Style QTT Framework for Non-Gravitational E* Constructors, Anchor-Free Inter-Sector Locks, and the Source-Only SI Boundary

Non-gravitational Artian capacity endpoint constructor Version: 1.1 Concept DOI: 10.5281/zenodo.21182051 Author: Ali Attar Website: quantumtraction.org \[ \boxed{ E_\ast^{(\gamma H)} =\frac{(\sqrt2\,G_F)^{-1/2}} {\sqrt2\,q_H\mathcal R_H^{\rm EW}}, \qquad \ell_A=\frac{\hbar c}{E_\...

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? 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...

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? \[ \boxed{ \mathrm{A2+A5\!\text{-}\!X+A6+A7}\not\Rightarrow\chi_g=1, \qquad G_{\rm end}=\chi_gG_A,\quad 0\leq\chi_g\leq1, \qquad \mathrm{EFA\!\text{-}\!G1}\Longleftrightarrow\chi_g=1. } \]...

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...

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 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}...

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...

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...

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...

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 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)\...