Artian Electron Source-Lab Rydberg Theorem

The electron source packet behind Rydberg precision Concept DOI: 10.5281/zenodo.20800371 Author: Ali Attar Website: quantumtraction.org Main book anchor: Quantum Traction Theory: Main Book v10.01 This paper isolates the electron/Rydberg precision spine as a source-access theorem. The source electron is frozen upstream, and atomic/QED rows may audit it but may not redefine it. The source/lab access exponent is \[ \mathcal I_e^{\mathrm{src/lab,QTT}} =\frac{1}{\rho\mathcal R_e^{\mathrm{ctor}}} +\frac{1}{64\mathcal R_e^{\mathrm{ctor}}}, \qquad \mathcal R_e^{\mathrm{ctor}}=256\cdot384\cdot198\cdot97. \] The frozen source electron and Rydberg audit are \[ m_e^{\mathrm{source,QTT}}=0.510998950610811\,\mathrm{MeV}, \qquad R_\infty^{\mathrm{QTT}}=\frac{\alpha_\lambda^2m_e^{\mathrm{source,QTT}}c}{2h} =10\,973\,731.568156838\,\mathrm{m}^{-1}. \] The no-retune rule is \[ \frac{\partial K_\lambda}{\partial O_a^{\mathrm{exp}}} = \frac{\partial\alpha_\lambda}{\partial O_a^{\mathrm{exp}}} = \frac{\partial m_e^{\mathrm{source,QTT}}}{\partial O_a^{\mathrm{exp}}}=0. \] Core labels: Σ-ELECTRON-SOURCE-RYDBERG, Σ-GAMMA-W-CORRIDOR, Σ-QED-NO-RETUNE-SOURCE-PROPAGATION.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-06-26
DOI
https://doi.org/10.5281/zenodo.20933241
Primary Topic
Chemical and Physical Properties of Materials
Type
preprint
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preprint

Artian Electron Source-Lab Rydberg Theorem

Attar Ali
Zenodo (CERN European Organization for Nuclear Research)
Chemical and Physical Properties of Materials
preprint

Artian Electron Source-Lab Rydberg Theorem

Attar Ali
preprint en

Abstract

The electron source packet behind Rydberg precision Concept DOI: 10.5281/zenodo.20800371 Author: Ali Attar Website: quantumtraction.org Main book anchor: Quantum Traction Theory: Main Book v10.01 This paper isolates the electron/Rydberg precision spine as a source-access theorem. The source electron is frozen upstream, and atomic/QED rows may audit it but may not redefine it. The source/lab access exponent is \[ \mathcal I_e^{\mathrm{src/lab,QTT}} =\frac{1}{\rho\mathcal R_e^{\mathrm{ctor}}} +\frac{1}{64\mathcal R_e^{\mathrm{ctor}}}, \qquad \mathcal R_e^{\mathrm{ctor}}=256\cdot384\cdot198\cdot97. \] The frozen source electron and Rydberg audit are \[ m_e^{\mathrm{source,QTT}}=0.510998950610811\,\mathrm{MeV}, \qquad R_\infty^{\mathrm{QTT}}=\frac{\alpha_\lambda^2m_e^{\mathrm{source,QTT}}c}{2h} =10\,973\,731.568156838\,\mathrm{m}^{-1}. \] The no-retune rule is \[ \frac{\partial K_\lambda}{\partial O_a^{\mathrm{exp}}} = \frac{\partial\alpha_\lambda}{\partial O_a^{\mathrm{exp}}} = \frac{\partial m_e^{\mathrm{source,QTT}}}{\partial O_a^{\mathrm{exp}}}=0. \] Core labels: Σ-ELECTRON-SOURCE-RYDBERG, Σ-GAMMA-W-CORRIDOR, Σ-QED-NO-RETUNE-SOURCE-PROPAGATION.

Zenodo (CERN European Organization for Nuclear Research)
Oldham Council (GB)
Chemical and Physical Properties of Materials
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