Attar Ali

Artian Constitutive Mechanics

A QTT Source-Work Framework for Stiffness, Oscillation, Damping and Noise Artian Constitutive Mechanics, version 1.0, joins restoring force, mechanical response and equilibrium fluctuations through one independently selected QTT source-work packet. \[ \boxed{\begin{gathered} \mat...

Artian's Source-Work and Ion-Escape Framework

Why a heating spectrum cannot determine an ion's escape history A trapped ion can heat slowly near the bottom of its well and still disappear quickly. What must a physical theory specify to predict both observations with one construction? This framework joins source work, finite...

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 2.03 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...

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}...

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

When does a physical device contain two genuinely different clock terminals? This framework gives a carrier-independent constructor for a source terminal and a laboratory-written terminal. A four-history experiment becomes eligible only when a completed source event, continuous p...

Artian A1 Earth-Flyby Handshake Preregistration: A Prospective Dual-Link Test of the QTT Two-Clock Map

One spacecraft can carry two physically different radio handshakes. Their difference is a new, geometry-locked clock test. Historical Earth-flyby residuals cannot decide this test because they contain only one physical radio-clock history. This preregistration instead requires tw...

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

A geometric phase can verify a loop without being mistaken for the clock effect under test. This paper isolates a clean experimental question in geometric quantum mechanics: can the same completed holonomy be read through two physically distinct terminal-reference architectures w...

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

When does a physical device contain two genuinely different clock terminals? This framework gives a carrier-independent constructor for a source terminal and a laboratory-written terminal. A four-history experiment becomes eligible only when a completed source event, continuous p...

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

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...

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

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-co...

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 2.03 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...

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

A geometric phase can verify a loop without being mistaken for the clock effect under test. This paper isolates a clean experimental question in geometric quantum mechanics: can the same completed holonomy be read through two physically distinct terminal-reference architectures w...

Artian's A6 Hard Coherence-Capacity Wall: A Source-Admissibility Postulate and Non-Stacking Theorems

A sharp upper bound on jointly coherent mass, rather than a collapse lifetime Can a jointly coherent mass keep growing without a physical ceiling? This paper states the global A6 hard-wall postulate in Artian geometry and gives it an explicit mathematical form. \[\boxed{\begin{al...

Artian's A6 Hard Coherence-Capacity Wall: A Source-Admissibility Postulate and Non-Stacking Theorems

A sharp upper bound on jointly coherent mass, rather than a collapse lifetime Can a jointly coherent mass keep growing without a physical ceiling? This paper states the global A6 hard-wall postulate in Artian geometry and gives it an explicit mathematical form. \[\boxed{\begin{al...

Artian Rotor-to-Wavefunction Projection Theorem: A Conditional QTT Recovery of the Schrödinger Equation, the A6 Bounded-Generator Gate, and the Macroscopic-Ceiling No-Go

What must be supplied before the Schrödinger equation can be recovered from a finite address model? A finite address ledger can reproduce Schrödinger evolution through an exact source-to-wavefunction projection. The result identifies the readout, the generator domain, and the clo...

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...

Artian's Completed-Event Bell Reconstruction: Real Source Geometry, Access, and Durable Records

From a finite event record to Bell correlations and their loss under recording A pair is prepared together, read at two separated instruments, and allowed to leave a material record. This paper builds the correlation law from a real source geometry in Artian's Quantum Traction Th...

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}}=&\ \...

Complex Structure and Composition from Finite Real Source Histories: An Artian Frame-Cycle Construction

How a finite real cycle acquires a complex structure and a rule for composition Quantum theory uses a common imaginary unit when individual systems become a composite. This framework constructs that compatibility from finite real source histories. On the complete contrast sector...