SPECTROSCOPIC DIAGNOSIS IN ELECTRONIC TEMPERATURE OF PHOTOIONISE PLASMAS
<p>In this work, we are interested in the diagnostics in electronic temperature of a plasma purely photoionized, based on the intensity ration of lines emitted by ions helium-like, which have an atomic number <em>Z </em>relatively small. We considered the three lines corresponding...
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doaj-093194c8129e4f958c5d1ba5d5e78f642020-11-24T23:46:35ZengEl Oued UniversityJournal of Fundamental and Applied Sciences1112-98672015-08-011211210.4314/jfas.v1i2.1148SPECTROSCOPIC DIAGNOSIS IN ELECTRONIC TEMPERATURE OF PHOTOIONISE PLASMASA. K. Ferouani0M. K. Inal1Université Abou Bekr Belkaïd Tlemcen, Faculté des Sciences, B.P 119 Tlemcen 13 000Université Abou Bekr Belkaïd Tlemcen, Faculté des Sciences, B.P 119 Tlemcen 13 000<p>In this work, we are interested in the diagnostics in electronic temperature of a plasma purely photoionized, based on the intensity ration of lines emitted by ions helium-like, which have an atomic number <em>Z </em>relatively small. We considered the three lines corresponding to the transitions starting from the excited levels 1s<em>2l</em> towards the fundamental level 1s<sup>2 1</sup>S<sub>0</sub>, like appropriate lines. More precisely, the line of resonance w<em> </em>due to the transition 1s2p <sup>1</sup>P<sub>1</sub> --- 1s<sup>2</sup> <sup>1 </sup>S<sub>0</sub>, the line of intercombinaison (x,y) 1s2p <sup>3 </sup>P<sub>2,1 </sub>--- 1s<sup>2</sup> <sup>1 </sup>S<sub>0</sub> as well as prohibited line z<em> </em>due to the transition 1s<sup>2</sup> <sup>3 </sup>S<sub>1</sub> --- 1s2 <sup>1 </sup>S<sub>0</sub>. These lines appear clearly in the spectra of astrophysical plasmas. As helium-like ion, we chose two, the oxygen O<sup>6+</sup> (Z=8) and neon Ne<sup>8+ </sup>(Z=10). We carried out calculations of the ration of lines intensity G=(z+x+y)/w<em> </em>of O<sup>6+</sup> and Ne<sup>8+ </sup>according to the electronic temperature in the range going from 10<sup>5</sup> to 10<sup>7</sup> K. We will see that, like it was shown by Gabriel and Jordan in 1969 [1], this intensity ration can be very sensitive to the temperature electronic and practically independent of the electronic density. Consequently, the ration G<em> </em>can be used to determine in a reliable way the electronic temperature of plasma observed [2].<em></em></p>http://jfas.info/index.php/jfas/article/view/194Strongly charged ions, lines emission, radiative and dielectronic recombination. |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
A. K. Ferouani M. K. Inal |
spellingShingle |
A. K. Ferouani M. K. Inal SPECTROSCOPIC DIAGNOSIS IN ELECTRONIC TEMPERATURE OF PHOTOIONISE PLASMAS Journal of Fundamental and Applied Sciences Strongly charged ions, lines emission, radiative and dielectronic recombination. |
author_facet |
A. K. Ferouani M. K. Inal |
author_sort |
A. K. Ferouani |
title |
SPECTROSCOPIC DIAGNOSIS IN ELECTRONIC TEMPERATURE OF PHOTOIONISE PLASMAS |
title_short |
SPECTROSCOPIC DIAGNOSIS IN ELECTRONIC TEMPERATURE OF PHOTOIONISE PLASMAS |
title_full |
SPECTROSCOPIC DIAGNOSIS IN ELECTRONIC TEMPERATURE OF PHOTOIONISE PLASMAS |
title_fullStr |
SPECTROSCOPIC DIAGNOSIS IN ELECTRONIC TEMPERATURE OF PHOTOIONISE PLASMAS |
title_full_unstemmed |
SPECTROSCOPIC DIAGNOSIS IN ELECTRONIC TEMPERATURE OF PHOTOIONISE PLASMAS |
title_sort |
spectroscopic diagnosis in electronic temperature of photoionise plasmas |
publisher |
El Oued University |
series |
Journal of Fundamental and Applied Sciences |
issn |
1112-9867 |
publishDate |
2015-08-01 |
description |
<p>In this work, we are interested in the diagnostics in electronic temperature of a plasma purely photoionized, based on the intensity ration of lines emitted by ions helium-like, which have an atomic number <em>Z </em>relatively small. We considered the three lines corresponding to the transitions starting from the excited levels 1s<em>2l</em> towards the fundamental level 1s<sup>2 1</sup>S<sub>0</sub>, like appropriate lines. More precisely, the line of resonance w<em> </em>due to the transition 1s2p <sup>1</sup>P<sub>1</sub> --- 1s<sup>2</sup> <sup>1 </sup>S<sub>0</sub>, the line of intercombinaison (x,y) 1s2p <sup>3 </sup>P<sub>2,1 </sub>--- 1s<sup>2</sup> <sup>1 </sup>S<sub>0</sub> as well as prohibited line z<em> </em>due to the transition 1s<sup>2</sup> <sup>3 </sup>S<sub>1</sub> --- 1s2 <sup>1 </sup>S<sub>0</sub>. These lines appear clearly in the spectra of astrophysical plasmas. As helium-like ion, we chose two, the oxygen O<sup>6+</sup> (Z=8) and neon Ne<sup>8+ </sup>(Z=10). We carried out calculations of the ration of lines intensity G=(z+x+y)/w<em> </em>of O<sup>6+</sup> and Ne<sup>8+ </sup>according to the electronic temperature in the range going from 10<sup>5</sup> to 10<sup>7</sup> K. We will see that, like it was shown by Gabriel and Jordan in 1969 [1], this intensity ration can be very sensitive to the temperature electronic and practically independent of the electronic density. Consequently, the ration G<em> </em>can be used to determine in a reliable way the electronic temperature of plasma observed [2].<em></em></p> |
topic |
Strongly charged ions, lines emission, radiative and dielectronic recombination. |
url |
http://jfas.info/index.php/jfas/article/view/194 |
work_keys_str_mv |
AT akferouani spectroscopicdiagnosisinelectronictemperatureofphotoioniseplasmas AT mkinal spectroscopicdiagnosisinelectronictemperatureofphotoioniseplasmas |
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1725493146547126272 |