The Artian Hamiltonian Framework for QTT
- 1Independent Researcher, Colombes, France
Abstract
Reading the Schrödinger Hamiltonian as a laboratory shadow of a real source generator Version: 3.04 Concept DOI: 10.5281/zenodo.20484906 Author: Ali Attar Website: quantumtraction.org Main book anchor: Quantum Traction Theory: Main Book v10.01 Textbook quantum mechanics begins with a Hamiltonian operator acting in laboratory time. This framework asks what that operator is a readout of when the source layer is a finite ledger of completed address events, a real phase rotor, and a capacity ceiling. The source evolution equation is real- J: JΣℏ ∂T|ρΣ⟩ = HΣsrc|ρΣ⟩. After a declared access window represents the real J-dial by the laboratory imaginary unit and selects the lab clock, the familiar equation appears: iℏ ∂tlabψ = HWlabψ. The Hamiltonian constructor order is therefore completed address events ⟶ real J−source module ⟶ HΣsrc ⟶ Access Law ⟶ HWlab. The no-retune condition is ∂ HΣsrcover ∂{observed spectrum, fitted laboratory constants}=0. The paper is a framework for writing QTT sector Hamiltonians: name the completed event set, define the source generator, state the A6/A7 capacity and closure gates, project through access, and then compare with observation.
Related
- Hamiltonian truncation framework for gauge theories on the interval
- Quantum-classical solvation hydrodynamics: a Hamiltonian modeling framework
- Hamiltonian framework for Chiral Gauge Theories on a Disk Boundary
- Stroh--Hamiltonian Framework for Modeling Incompressible Poroelastic Materials
- The Gated Quantum Resonator: a reduced-representation Hamiltonian–network framework for gated driven–dissipative quantum systems
BibTeX
@misc{ali2026artian,
title = {{The Artian Hamiltonian Framework for QTT}},
author = {Attar Ali},
howpublished = {Zenodo (CERN European Organization for Nuclear Research)},
year = {2026},
month = jun,
doi = {10.5281/zenodo.20484906},
url = {https://doi.org/10.5281/zenodo.20484906},
note = {CC BY},
}
RIS
TY - UNPB
TI - The Artian Hamiltonian Framework for QTT
AU - Attar Ali
PY - 2026
DA - 2026/06/25
PB - Zenodo (CERN European Organization for Nuclear Research)
DO - 10.5281/zenodo.20484906
UR - https://doi.org/10.5281/zenodo.20484906
AB - Reading the Schrödinger Hamiltonian as a laboratory shadow of a real source generator Version: 3.04 Concept DOI: 10.5281/zenodo.20484906 Author: Ali Attar Website: quantumtraction.org Main book anchor: Quantum Traction Theory: Main Book v10.01 Textbook quantum mechanics begins with a Hamiltonian operator acting in laboratory time. This framework asks what that operator is a readout of when the source layer is a finite ledger of completed address events, a real phase rotor, and a capacity ceiling. The source evolution equation is real- J: J_Σℏ ∂_T|ρ_Σ⟩ = H_Σ^src|ρ_Σ⟩. After a declared access window represents the real J-dial by the laboratory imaginary unit and selects the lab clock, the familiar equation appears: iℏ ∂_t_labψ = H_W^labψ. The Hamiltonian constructor order is therefore completed address events ⟶ real J−source module ⟶ H_Σ^src ⟶ Access Law ⟶ H_W^lab. The no-retune condition is ∂ H_Σ^srcover ∂{observed spectrum, fitted laboratory constants}=0. The paper is a framework for writing QTT sector Hamiltonians: name the completed event set, define the source generator, state the A6/A7 capacity and closure gates, project through access, and then compare with observation.
ER -