Electron-impact excitation of the 
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Marinković, B P; Tosic, Sanja; Šević, D.; McEachran, R P; Blanco, F.; Garcı́a, Gustavo; Brunger, M. J.

doi:10.1103/physreva.104.022808

Cited by 3 publications

(4 citation statements)

References 57 publications

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“…This oscillatory behaviour appears to be ubiquitous in electron collision processes, for both the elastic and discrete inelastic channels. Some specific examples for electron scattering from metal vapours include zinc [3], bismuth [4], silver [15], sodium [25], magnesium [26] and indium [27]. The oscillatory nature of any differential cross section arises from the interference, both constructive and destructive, between the various partial waves that describe the collisional behaviour [28].…”

Section: Resultsmentioning

confidence: 99%

“…The apparatus employed in the present measurements is a conventional crossed-beam spectrometer, the details of which can be found elsewhere [3,4,15]. Briefly, a nearly monoenergetic beam of electrons intersected a beam of Rb atoms at right angles.…”

Section: Experimental Considerationsmentioning

confidence: 99%

“…The spectroscopic notation for the main features is indicated. The solid black line is a weighted cubic-spline interpolation between the data points as in reference [15], with an uncertainty in that process of ± 0.1 eV.…”

Section: Experimental Considerationsmentioning

confidence: 99%

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Electron-impact excitation of the 5$$\varvec{^2\textbf{S}_{1/2} \rightarrow 5^2\textbf{P}_{1/2}}$$ and 5$$\varvec{^2\textbf{P}_{3/2}}$$ transitions in rubidium by 40 eV electrons: theory and experiment

et al. 2022

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We report on a series of detailed Breit-Pauli and Dirac B-spline R-matrix (DBSR) differential cross section (DCS) calculations for excitation of the $$5\,^2\mathrm{S}_{1/2} \rightarrow 5\,^2\mathrm{P}_{1/2}$$ 5 2 S 1 / 2 → 5 2 P 1 / 2 and $$5\,^2\mathrm{S}_{1/2}\rightarrow 5\,^2\mathrm{P}_{3/2}$$ 5 2 S 1 / 2 → 5 2 P 3 / 2 states in rubidium by 40 eV incident electrons. The early BP computations shown here were carried out with both 5 states and 12 states, while the DBSR models coupled 150 and 325 states, respectively. We also report corresponding results from a limited set of DCS measurements on the unresolved $$5\,^2\mathrm{P}_{1/2,3/2}$$ 5 2 P 1 / 2 , 3 / 2 states, with the experimental data being restricted to the scattered electron angular range 2–$$10^\circ $$ 10 ∘ . Typically, good agreement is found between our calculated and measured DCS for excitation of the unresolved $$5\,^2\mathrm{P}_{1/2,3/2}$$ 5 2 P 1 / 2 , 3 / 2 states, with best accord being found between the DBSR predictions and the measured data. The present theoretical and experimental results are also compared with predictions from earlier 40 eV calculations using the nonrelativistic Distorted-Wave Born Approximation and a Relativistic Distorted-Wave model. Graphic abstract

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Section: Resultsmentioning

confidence: 99%

Section: Experimental Considerationsmentioning

confidence: 99%

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Electron-impact excitation of the 5$$\varvec{^2\textbf{S}_{1/2} \rightarrow 5^2\textbf{P}_{1/2}}$$ and 5$$\varvec{^2\textbf{P}_{3/2}}$$ transitions in rubidium by 40 eV electrons: theory and experiment

et al. 2022

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“…We have recently described our standard nonrelativistic OP approach in our studies of the electron-beryllium, 42 electron-magnesium, 43 electron-zinc, 44 electron-indium, 59 and electron-silver 60 scattering systems. The generic details of this atomic OP method were given in those papers, so only the key points of this method are summarized below.…”

Section: Atomic Op Modelmentioning

confidence: 99%

Cross Sections for Electron Scattering from Cadmium: Theory and Experiment

Marinković

McEachran

Fursa³

et al. 2023

Journal of Physical and Chemical Reference Data

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Results from the application of optical potential, relativistic optical potential, relativistic convergent close-coupling, and binary encounter Bethe models to electron scattering from gas-phase cadmium are presented. In particular, integral cross sections for elastic scattering, summed discrete electronic-state excitation, and ionization scattering processes are reported over an extended incident electron-energy range. Total cross sections are constructed by taking their sum. Measurements are presented for elastic scattering and for excitation to the 51P1 state. The theoretical and experimental results are compared to previous calculations and measurements. Recommended electron cross-section datasets are constructed over an incident electron energy range of 0.01–10 000 eV.

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Elastic and inelastic scattering of low-energy electrons from gas-phase $$\hbox {C}_{\mathbf {60}}$$: elastic scattering angular distributions and coexisting solid-state features revisited

2021

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Electron-impact excitation of the (4d105s)S1/22→

Abstract: Electron-impact excitation of the (4d 10 5s) 2 S1/2 → (4d 9 5s 2 ) 2 D3/2 and (4d 10 5s) 2 S1/2 → (4d 10 6s) 2 S1/2 transitions in silver: Experiment and theory

Cited by 3 publications

References 57 publications

Electron-impact excitation of the 5$$\varvec{^2\textbf{S}_{1/2} \rightarrow 5^2\textbf{P}_{1/2}}$$ and 5$$\varvec{^2\textbf{P}_{3/2}}$$ transitions in rubidium by 40 eV electrons: theory and experiment

Electron-impact excitation of the 5$$\varvec{^2\textbf{S}_{1/2} \rightarrow 5^2\textbf{P}_{1/2}}$$ and 5$$\varvec{^2\textbf{P}_{3/2}}$$ transitions in rubidium by 40 eV electrons: theory and experiment

Cross Sections for Electron Scattering from Cadmium: Theory and Experiment

Elastic and inelastic scattering of low-energy electrons from gas-phase $$\hbox {C}_{\mathbf {60}}$$: elastic scattering angular distributions and coexisting solid-state features revisited

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