2020
DOI: 10.3390/data5030073
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Forty Years of the Applications of Stark Broadening Data Determined with the Modified Semiempirical Method

Abstract: The aim of this paper is to analyze the various uses of Stark broadening data for non-hydrogenic lines emitted from plasma, obtained with the modified semiempirical method formulated 40 years ago (1980), which are continuously implemented in the STARK-B database. In such a way one can identify research fields where they are applied and better see the needs of users in order to better plan future work. This is done by analysis of citations of the modified semiempirical method and the corresponding data in inter… Show more

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Cited by 19 publications
(7 citation statements)
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References 153 publications
(169 reference statements)
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“…Here are presented results of calculations of Stark full widths at half intensity maximum (FWHM) of spectral lines of ionized palladium (Pd II), by using the modified semiempirical method [25,32]. Atomic energy levels of ionized palladium, needed for present calculations, have been taken from [33,34].…”
Section: Resultsmentioning
confidence: 99%
“…Here are presented results of calculations of Stark full widths at half intensity maximum (FWHM) of spectral lines of ionized palladium (Pd II), by using the modified semiempirical method [25,32]. Atomic energy levels of ionized palladium, needed for present calculations, have been taken from [33,34].…”
Section: Resultsmentioning
confidence: 99%
“…Of course, these data may be of interest for laboratory plasma diagnostics and for investigations of laser produced plasma and lasers. A detailed analysis of the usage of published Stark broadening data was published in [19,20].…”
Section: Discussionmentioning
confidence: 99%
“…Among the line broadening mechanisms, the Stark broadening ★ Email: haelabidi@uqu.edu.sa -resulting from the action of electric field of particles surrounding an emitter-is the most important. There are two origins of this importance: firstly, because Stark broadening occurs for various physical conditions of plasma, especially for astrophysical plasmas: from clouds of interstellar molecular hydrogen, with temperatures around 30 K and electron densities 𝑁 𝑒 = 1−5 cm −3 (conditions that cannot be obtained in laboratory plasmas) to white dwarf atmospheres and hot stars of A and B types with temperature about 10 5 K and density 𝑁 𝑒 = 10 17 cm −3 (Dimitrijević 2020). The reader can find in Dimitrijević (2003) a set of extremely different plasma conditions for which Stark broadening cannot be neglected.…”
Section: Introductionmentioning
confidence: 99%