2014
DOI: 10.18524/1815-7459.2006.3.112570
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Sensing the Auger Spectra for Solids: New Quantum Approach

Abstract: SENSING THE AUGER SPECTRA FOR SOLIDS: NEW QUANTUM APPROACH S. V. Ambrosov, A. V. Glushkov, L. V. NikolaIt is proposed new approach to sensing Auger spectra of solids and calculation of charac-teristics of Auger decay within S-matrix Gell-Mann and Low formalism. The energies of Auger electron transitions in solids (Na,Si,Ge,Ag) are calculated with account for correlation effects.

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“…In addition, the proportionality coefficient in the equation coincides with the electron impact ionization cross-section σ ϳ of the level ϳ. Of course, two aspects are to be considered when determining the exit probability of Auger electrons from an atom, namely, the radiative transition under neutralization of a hole at the level j and the possibility of a considerable change in the initial hole distribution at the core levels at the Auger decay via the radiative channel jkl associated as a rule with a considerable distinctions in the non-radiative transition probabilities [11,12]. For definiteness sake, let the ionization of L levels in a multi-electron atom be considered.…”
Section: Results and Conclusionmentioning
confidence: 99%
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“…In addition, the proportionality coefficient in the equation coincides with the electron impact ionization cross-section σ ϳ of the level ϳ. Of course, two aspects are to be considered when determining the exit probability of Auger electrons from an atom, namely, the radiative transition under neutralization of a hole at the level j and the possibility of a considerable change in the initial hole distribution at the core levels at the Auger decay via the radiative channel jkl associated as a rule with a considerable distinctions in the non-radiative transition probabilities [11,12]. For definiteness sake, let the ionization of L levels in a multi-electron atom be considered.…”
Section: Results and Conclusionmentioning
confidence: 99%
“…The Auger line intensity is defined by three atomic constants: А jkl = σ ϳ f ϳ a ϳkl where a ϳkl is the non-radiative transition probability; fi is the Korster-Kronig coefficient; σ ϳ , the ionization cross-section defined by the matrix element (1) calculated for wave functions of bound state and continuum one. In table 1 we present the data on Auger electron energy for some solids calculated using the presented approach (column C), the semi-empirical method with using the Larkins' equivalent core approximation [8] (column A), the perturbation theory approach [11,12] as well as experimental data (c.g. [1]).…”
Section: Results and Conclusionmentioning
confidence: 99%
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