The Artian Lagrangian Framework: A Finite Action Ledger for Quantum Traction Theory, from Completed Address Events to Laboratory Least Action
- 1Researcher, Colombes, France
Abstract
A finite-event route from Lagrangians to least action Version: 2.1 Concept DOI: 10.5281/zenodo.20657182 Author: Ali Attar Website: quantumtraction.org Main book anchor: Quantum Traction Theory: Main Book v10.01 Ordinary analytical mechanics begins with a smooth action functional. This framework asks what that action is the laboratory shadow of if the source object is finite, counted, and address-based. The starting object is a completed event: ℰ∈𝒞T Longleftrightarrow Qℰbundle=2π, Eℰ t̃A=ℏ, Δ V(4)ℰ=4πℓA4. The source action is then a finite ledger sum over completed modular-capacity events: SQTTsrc[Γ;T0,T1] = ∑ℰ∈𝒞T(Γ;T0,T1) Δ Sℰ, Δ Sℰ=ℒℰsrc Δ Tℰ. The familiar laboratory action appears only after access/coarse-graining: Slab[ϕ] = ∫ d4x √(−g) ℒlab(ϕ,∇ϕ,x). The paper's constructor order is the point: completed events ⟶ SQTTsrc ⟶ Access Law projection ⟶ Slab. Stationary action is recovered as the coherent real- J dial condition of the ledger sum, δ Slab=0, while the no-retune rule for a legal sector term is ∂ℒsrcover ∂{laboratory fit parameters after projection}=0. Read this paper as the Lagrangian grammar for QTT sector derivations: declare the completed event set, print the source Lagrangian, state capacity and closure gates, project through access, and only then compare with observation.
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BibTeX
@misc{ali2026artian,
title = {{The Artian Lagrangian Framework: A Finite Action Ledger for Quantum Traction Theory, from Completed Address Events to Laboratory Least Action}},
author = {Attar Ali},
howpublished = {Zenodo (CERN European Organization for Nuclear Research)},
year = {2026},
month = jun,
doi = {10.5281/zenodo.20657182},
url = {https://doi.org/10.5281/zenodo.20657182},
note = {CC BY},
}
RIS
TY - UNPB
TI - The Artian Lagrangian Framework: A Finite Action Ledger for Quantum Traction Theory, from Completed Address Events to Laboratory Least Action
AU - Attar Ali
PY - 2026
DA - 2026/06/12
PB - Zenodo (CERN European Organization for Nuclear Research)
DO - 10.5281/zenodo.20657182
UR - https://doi.org/10.5281/zenodo.20657182
AB - A finite-event route from Lagrangians to least action Version: 2.1 Concept DOI: 10.5281/zenodo.20657182 Author: Ali Attar Website: quantumtraction.org Main book anchor: Quantum Traction Theory: Main Book v10.01 Ordinary analytical mechanics begins with a smooth action functional. This framework asks what that action is the laboratory shadow of if the source object is finite, counted, and address-based. The starting object is a completed event: ℰ∈𝒞_T Longleftrightarrow Q_ℰ^bundle=2π, E_ℰ t̃_A=ℏ, Δ V^(4)_ℰ=4πℓ_A^4. The source action is then a finite ledger sum over completed modular-capacity events: S_QTT^src[Γ;T_0,T_1] = ∑_ℰ∈𝒞_T(Γ;T_0,T_1) Δ S_ℰ, Δ S_ℰ=ℒ_ℰ^src Δ T_ℰ. The familiar laboratory action appears only after access/coarse-graining: S_lab[ϕ] = ∫ d^4x √(−g) ℒ_lab(ϕ,∇ϕ,x). The paper's constructor order is the point: completed events ⟶ S_QTT^src ⟶ Access Law projection ⟶ S_lab. Stationary action is recovered as the coherent real- J dial condition of the ledger sum, δ S_lab=0, while the no-retune rule for a legal sector term is ∂ℒ^srcover ∂{laboratory fit parameters after projection}=0. Read this paper as the Lagrangian grammar for QTT sector derivations: declare the completed event set, print the source Lagrangian, state capacity and closure gates, project through access, and only then compare with observation.
ER -