Ali Attar

A7U: Distributed Planck Bundles, Access-Relative Purity, and the Matter-Wave Visibility Bridge

When a pure object is only pure for a closed access cut The completed distributed bundle closes one source budget: \[ \boxed{Q_w^{\mathrm{vis}}+Q_w^{\mathrm{hid}}=2\pi.} \] Version: 4.1 Concept DOI: 10.5281/zenodo.20097247 Author: Ali Attar, ORCID 0009-0008-9931-2691 Website: qua...

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...

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 Entropy and Second-Law Reference Theorem: Completed Records, Access Loss, and the A2-A3 Source-Volume Ledger

A Two-Coordinate Second Law with a Separate Source-Volume Ledger This paper separates two statements often compressed into one word. Completed physical records do not disappear from the source history, while a laboratory channel can lose access to distinctions that remain present...

The Stefan–Boltzmann Constant as a Photon-Throughput Theorem of Artian Geometry and Phase Topology

Where the blackbody coefficient gets each of its factors The photon mode measure is fixed by two transverse rails, the isotropic direction sphere, and three phase-closure cycles: \[ \frac{dN}{V} =2\,\frac{4\pi k^2dk}{(2\pi)^3} =\frac{\omega^2d\omega}{\pi^2c^3}. \] The source meas...

Boltzmann Weighting from Finite Completed-Event Reservoirs: The Completed-Record–Multiplicity Bridge, Signed Finite-Bath Corrections, and a Seven-Face Thermal Consistency Ledger

When a finite reservoir becomes a Gibbs weight For a closed system coupled to a finite reservoir, the exact subsystem law is \[ p_a= \frac{g_a\,\Omega_R(E_{\rm tot}-E_a)} {\sum_b g_b\,\Omega_R(E_{\rm tot}-E_b)}. \] The familiar Boltzmann factor is the tangent limit of this finite...

Artian Inertial Mass Operator and Three-Readout Spectral Equivalence Theorem

When does the coefficient in Newton's second law become a finite spectrum rather than an inserted input? The paper constructs a positive finite source operator from funded completed-event classes. For a finite region \(\mathcal R\), \[ \widehat B_{\mathcal R} = \sum_{p\in\mathfra...

Artian's Casimir Boundary-Access Framework: Gauge-Invariant Plate Projectors, the Standard Coefficient, Three-2pi Non-Equivalence, and a Conditional Finite-Address Test

How two conducting plates reshape the photon spectrum without retuning the photon The ideal parallel-plate Casimir coefficient is familiar. The sharper question is what mathematical operation a conducting boundary performs on the physical photon space. This paper constructs that...

Maxwell Dynamics from the Monadic Real-J Address Dial: A QTT Axiom-to-Field Theorem with Source-Derived Photon Stiffness

From a compact internal dial to Maxwell's equations and a frozen photon stiffness The paper asks a precise foundations question: once a local compact phase dial, finite per-address capacity, and local Lorentz readout are fixed, how much of electrodynamics remains free? The result...

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_...

Artian Action-Rotor Reference Framework: Hamilton's Stationary-Action Recovery, the Real-J Path Sum, and the Capacity/Canonical Action Ledger

One Phase Turn, Three Different Ledgers Version: 3.0 Concept DOI: 10.5281/zenodo.20098143 Author: Ali Attar Website: quantumtraction.org Main book: Quantum Traction Theory: Main Book v10.01 A unit quantum phase can be written entirely with a real two-component rotor, \[ R_J(\thet...

The Born Rule from Finite Address-Capacity Counting: A Conditional QTT Representation and Uniqueness Theorem

Why does quantum probability use the square rather than another power? This paper separates that question into a source theorem and two explicit laboratory bridges. For a finite address block, every nonnegative, regular, orthogonally additive capacity that is invariant under real...

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? Let the source state be a square-summable family of real-(J) amplitudes, \[ \mathcal H_{\rm src} = \ell^2(\mathcal W)\widehat\otimes\mathcal H_{{\rm lab},\mathbb R}, \] and let one...

QTT HVP Prospective Blind-Run Lock and Fail-Closed Verdict Executor

Can an HVP topology be predicted before the row's central value is opened? The original QTT HVP blind lock froze an eight-component vector-source ledger, an access quantum, and the finite topology class \(n_d\in\{0,2,3,4,8\}\) before true central values were available. Version 2....