1995A&A...293..457L


Query : 1995A&A...293..457L

1995A&A...293..457L - Astronomy and Astrophysics, volume 293457-462 (1995/1-2)

High-resolution spectroscopy and NLTE calculations of the HeI 10830 A line in magnetic chemically peculiar stars. A search for indirect evidences of hot stellar envelopes.

LEONE F., LANZAFAME A.C. and PASQUINI L.

Abstract (from CDS):

Observations of CIV and SIIV lines in the ultraviolet spectra, X-ray and radio emission for some of the hottest chemically peculiar stars have led to the suggestion that high temperature plasmas are present around them. A possible indirect way to prove the existence of a corona around the CP stars is to observe the HeI 10830A line since, in presence of a X-ray emitting corona, this line should disappear in the spectrum of B-type stars (Mitskevich & Tsymbal 1992A&A...260..303M). Searching for possible differences, we have obtained high resolution HeI 10830A spectra for 7 early type magnetic CP and 8 normal stars. The equivalent width of the HeI 10830A line, always in absorption, increases from A1 to B3 and then decreases. The HeI 10830A line is present in the spectrum of CP stars with the same strength as in normal stars. Comparison with Mitskevich & Tsymbal (1992A&A...260..303M) calculations suggests that no X-ray emitting plasma is present around the observed CP stars. We also present new NLTE calculations for HeI 10830A, analysing the sensitivity of this line to abundance variations. For normal main sequence stars of spectral type A1-B3 our computations are in closer agreement with observations than in previous work. In this spectral range, the line is found to be weakly dependent on the chemical composition.

Abstract Copyright: ∼

Journal keyword(s): line: formation - techniques: spectroscopy - stars: chemically peculiar - stars: corona - stars: early-type

Simbad objects: 19

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Number of rows : 19
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 * gam Peg bC* 00 13 14.1523490172 +15 11 00.954346538 1.75 2.61 2.84 2.94 3.13 B2IV 720 0
2 * alf Scl Ro* 00 58 36.3592644040 -29 21 26.832190995 3.52 4.09 4.27 4.30 4.43 B7IIIp 259 0
3 * eps Cas Be* 01 54 23.7340861680 +63 40 12.360238788 2.61 3.22 3.37 3.40 3.52 B3Vp_sh 207 0
4 HD 36960 * 05 35 02.6823091513 -06 00 07.308349203 3.52 4.50 4.72     B0.5V 283 0
5 HD 37017 SB* 05 35 21.8667428568 -04 29 39.024375324 5.66 6.43 6.56 6.61 6.74 B2/3V 318 0
6 * sig Ori E Y*O 05 38 47.2050040320 -02 35 40.521424812 5.66 6.38 6.46 6.84 7.08 B2IV-Vp_He 486 0
7 * rho Cen Pu* 12 11 39.1197479712 -52 22 06.384420264 3.20 3.81 3.96 4.05 4.21 B3V 136 0
8 V* CU Vir a2* 14 12 15.8055434051 +02 24 33.945178515 4.46 4.90 5.02 5.10 5.23 ApSi 411 0
9 * rho Lup V* 14 37 53.2261607412 -49 25 32.981831985 3.34 3.90 4.05 4.14 4.25 B3/4V 112 0
10 V* V913 Sco Ro* 15 58 34.8665694960 -24 49 53.361727284 4.70 5.34 5.43     B5V 226 0
11 HD 143699 * 16 03 24.1895252119 -38 36 09.141541952 4.18 4.75 4.89 4.96 5.10 B5/7III/IV 154 0
12 HD 146001 * 16 14 53.4294665736 -25 28 37.100440632 5.73 6.09 6.05     B8V 161 0
13 * del Ara PM* 17 31 05.9135939049 -60 41 01.841838888 3.21 3.52 3.62     B8Vn 98 0
14 V* V2393 Oph a2* 18 33 23.3029636152 +08 16 05.698559100 6.05 6.379 6.416     B9III 77 0
15 * sig Sgr ** 18 55 15.92650 -26 17 48.2068 1.06 1.923 2.067     B2.5V 284 1
16 V* V686 CrA a2* 18 56 40.4859327624 -37 20 35.701261512 4.53 5.24 5.38     B3V 214 0
17 * bet01 Sgr Pu* 19 22 38.2992119424 -44 27 32.250184884 3.52 3.91 4.01     B9V 81 0
18 * tet Cap PM* 21 05 56.8284751494 -17 13 58.306214724 4.07 4.06 4.07 4.06 4.08 A1V 94 0
19 * alf Gru PM* 22 08 13.98473 -46 57 39.5078 1.11 1.58 1.71 1.75 1.83 B6V 311 0

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