2014
DOI: 10.1016/j.jqsrt.2014.09.002
|View full text |Cite
|
Sign up to set email alerts
|

A collisional radiative model for low-pressure hydrogen–caesium plasmas and its application to an RF source for negative hydrogen ions

Abstract: a b s t r a c tA collisional radiative (CR) model for caesium in low-temperature, low-pressure hydrogen-caesium plasmas is introduced. This model includes the caesium ground state, 14 excited states, the singly charged caesium ion and the negative hydrogen ion. The reaction probabilities needed as an input are based on literature data, using some scaling and extrapolations. Additionally, new cross sections for electron collision ionization and threebody recombination have been calculated.The relevance of mutua… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
6
0

Year Published

2015
2015
2024
2024

Publication Types

Select...
7
2

Relationship

2
7

Authors

Journals

citations
Cited by 12 publications
(10 citation statements)
references
References 66 publications
0
6
0
Order By: Relevance
“…In addition to the excitation caused by collisions with electrons, the Cs excited states are populated by the mutual neutralization of Cs + and H − , especially when 𝑛 𝐻 − reaches values similar or greater than 𝑛 𝑒 [13]. The importance of this channel is well documented, but including it requires assumptions on both 𝑛 𝐻 − and 𝑛 Cs + .…”
Section: Spidermentioning
confidence: 99%
“…In addition to the excitation caused by collisions with electrons, the Cs excited states are populated by the mutual neutralization of Cs + and H − , especially when 𝑛 𝐻 − reaches values similar or greater than 𝑛 𝑒 [13]. The importance of this channel is well documented, but including it requires assumptions on both 𝑛 𝐻 − and 𝑛 Cs + .…”
Section: Spidermentioning
confidence: 99%
“…The caesium emission is correlated to plasma parameters like the caesium density, the electron density and the electron temperature. For quantitative statements absolutely calibrated measurements as well as the application of an appropriate population model are necessary [21]. During each of the four pulses a continuous slope of the Cs emission is seen, with two phases of slightly increased emission during the two beam blips, correlated with the increased caesium release from the back plate caused by the back streaming ions, i.e.…”
Section: Caesium Conditioning For Long Pulsesmentioning
confidence: 99%
“…For the determination of the neutral Cs density in the ground state close to the convertor surface, a tunable diode laser spectroscopy (TDLAS) at the resonant Cs 852 nm trans ition (6 2 S 1/2 → 6 2 P 3/2 , named Cs-D2) is applied at ELISE, measuring the hyperfine spectrum. The density of Cs 0 in the ground state reflects the total density of neutral Cs, because the densities in the excited states contribute with less than 1% to the total population [13,14]. Significant broadening and dist ortion of the lines result from the Doppler effect as well as from the Zeeman effect; further broadening mech anisms as the pressure or Stark broadening are of no relevance in the ion sources.…”
Section: Introductionmentioning
confidence: 99%