• Aucun résultat trouvé

Stark broadening of Sr I spectral lines ?

N/A
N/A
Protected

Academic year: 2022

Partager "Stark broadening of Sr I spectral lines ?"

Copied!
2
0
0

Texte intégral

(1)

ASTRONOMY & ASTROPHYSICS NOVEMBER I1996, PAGE 529 SUPPLEMENT SERIES

Astron. Astrophys. Suppl. Ser.119, 529-530 (1996)

Stark broadening of Sr I spectral lines ?

M.S. Dimitrijevi´c1 and S. Sahal-Br´echot2

1 Astronomical Observatory, Volgina 7, 11050 Belgrade, Yugoslavia

2 Laboratoire “Astrophysique, Atomes et Mol´ecules”, D´epartement Atomes et Mol´ecules en Astrophysique, Unit´e associ´ee au C.N.R.S. No. 812, Observatoire de Paris-Meudon, 92190 Meudon, France

Received March 13; accepted March 26, 1996

Abstract. — Using a semiclassical approach, we have calculated electron, proton, and ionized heliumimpact line widths and shifts for 33 Sr I multiplets for perturber densities 1013cm3(for stellar plasma research) and 1015 1018 cm3 (for laboratory plasma research) and temperaturesT = 2 50050 000 K.

Key words:lines: profile-atomic data

1. Introduction

Strontium lines are present in solar and stellar spectra.

E.g. Komarov & Basak (1993) have found neutral stron- tium lines in the spectra of Sun and two Praesepe’s stars.

They are also of interest since Sr is one of thermonuclear s - processes product in stars and its overabundance is ob- served in CH and metal deficient barium stars (ˇSleivyt´e

& Bartkeviˇcius 1995). Neutral strontium lines are also of interest for the investigation of laboratory plasmas. Conse- quently, Kato et al. (1984) investigated wavelength shifts of Sr I lines emitted by an inductively coupled plasma and Karabut et al. (1980) dynamics of strontium line shapes during a pulsed discharge. Such lines have been consid- ered theoretically as well by Davis (1972), for research of a laser - generated barium plasma. In order to con- tinue our research of Stark broadening parameters needed for the investigation of astrophysical and laboratory plas- mas and to provide the needed Stark broadening data, we have calculated within the semiclassical-perturbation for- malism (Sahal−Br´echot 1969a,b) electron-, proton-, and ionized helium-impact line widths and shifts for 33 Sr I multiplets. A summary of the formalism is given in Dimitrijevi´c & Sahal-Br´echot (1984).

2. Results and discussion

Energy levels for Sr I lines have been taken from Moore (1971). Oscillator strengths have been calculated by using Send offprint requests to: M.S. Dimitrijevi´c

?Table 1 is only available in electronic form: The material published electronically can be accessed: by ftp at cdsarc.u- strasbg.fr or 130.79.128.5 or on WWW at: http//cdsweb.u- strasbg.fr/abstract.html

the method of Bates & Damgaard (1949) and the tables of Oertel & Shomo (1968). For higher levels, the method described by Van Regemorter et al. (1979) has been used.

We note that Gruzdev (1967) has found that the semiem- pirical and Hartree - Fock calculations of Sr I oscillator strengths agree fairly well with thef values calculated by the method of Coulomb approximation.

In addition to electron-impact full halfwidths and shifts, Stark-broadening parameters due to proton-, and He II- impacts have been calculated. Our results for 33 Sr I multiplets are shown in Table 1 (accesible only in electronic form), for perturber densities 1013 cm−3 (for stellar plasma research) and 1015−1018 cm−3 (for labo- ratory plasma research) and temperatures T = 2 500− 50 000 K. We also specify a parameter c (Dimitrijevi´c

& Sahal−Br´echot 1984), which gives an estimate for the maximum perturber density for which the line may be treated as isolated when it is divided by the correspond- ing full width at half maximum. For each value given in Table 1, the collision volume (V) multiplied by the per- turber density (N) is much less than one and the impact approximation is valid (Sahal−Br´echot 1969a,b). Values forN V >0.5 are not given and values for 0.1< N V ≤0.5 are denoted by an asterisk. When the impact approxima- tion is not valid, the ion broadening contribution may be estimated by using quasistatic approach (Sahal−Br´echot 1991; Griem 1974). In the region between where neither of these two approximations is valid, a unified type theory should be used. For example in Barnard et al. (1974), a simple analytical formulas for such a case are given. The accuracy of the results obtained decreases when broaden- ing by ion interactions becomes important.

(2)

530 M.S. Dimitrijevi´c and S. Sahal-Br´echot: Stark broadening of Sr I spectral lines

Acknowledgements.This work is a part of the project “Physics and dynamics of celestial bodies”, supported by Ministry of Science and Technology of Serbia.

References

Barnard A.J., Cooper J., Smith E.W., 1974, JQSRT 14, 1025 Bates D.R., Damgaard A., 1949, Trans. Roy. Soc. London Ser.

A 242, 101

Davis J., 1972, JQSRT 12, 1351

Dimitrijevi´c M.S., SahalBr´echot S., 1984, JQSRT 31, 301 Griem H.R., 1974, Spectral Line Broadening by Plasmas.

Academic Press, New York

Gruzdev P.F., 1967, Opt. Spektrosk. 22, 169

Karabut E.K., Kravchenko V.F., Mikhalevskii V.S., 1980, Opt.

Spectrosc. 48, 386

Kato K., Fukushima H., Nakajima T., 1984, Spectrochim. Acta B 39, 979

Komarov N.S., Basak N.Yu., 1993, Astron. Zh. 70, 111 Moore C.E., 1971, Atomic Energy Levels II, NSRDS-NBS 35,

Washington

Oertel G.K., Shomo L.P., 1968, ApJS 16, 175 SahalBr´echot S., 1969a, A&A 1, 91

SahalBr´echot S., 1969b, A&A 2, 322 SahalBr´echot S., 1991, A&A 245, 322

ˇSleivyt´e J., Bartkeviˇcius A., 1995, Vilniaus Astron. Obs.

Biuletenis 85, 3

Van Regemorter H., Hoang Binh Dy, Prud’homme M., 1979, J. Phys. B 12, 1073

Références

Documents relatifs

3 and 4, show that intra-shell L-L transition (around 26 nm) are negligible compared to the Al IV lines (at 13.1 and 16 nm, M-L transitions) at about 8 eV electron temperature. At

Abstract: The particular character of the welding arc working in pure argon, which emission spectrum consists of many spectral lines strongly broadened by Stark effect, has allowed

merous measured and calculated Stark widths have been reported for neutral and singly ionized elements but no data are available for gallium and indium.. In this paper

We hereafter denote the lamp of the former type as ST-HCL(see-through hollow cathode lamp) and the latter as U-HCL(U-shaped cathode HCL). The experiment has shown that the shift

The analysis of the spectra needs atomic and line broadening data: for the evaluation of the abundance of Ba V, Ba VI, and Ba VII [4] and of the Se V, Sr IV-VII, Te VI, and I VI

presented in Table 1, together with cor- responding data from Griem (1974) .4 Since in low-density plasmas Stark parameters depend practically linearly on N, it is evident

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des