Dust formation and mass loss around intermediate-mass AGB stars with initial metallicity Zini ≤ 10-4 in the early Universe - I. Effect of surface opacity on stellar evolution and the dust-driven wind

被引:9
|
作者
Tashibu, Shohei [1 ,4 ]
Yasuda, Yuki [2 ]
Kozasa, Takashi [1 ,2 ,3 ]
机构
[1] Univ Tokyo, Dept Astron, Bunkyo Ku, 7-3-1 Hongo, Tokyo 1130033, Japan
[2] Hokkaido Univ, Fac Sci, Div Earth & Planetary Sci, Sapporo, Hokkaido 0600810, Japan
[3] Hokkaido Univ, Grad Sch Sci, Dept Cosmosci, Sapporo, Hokkaido 0600810, Japan
[4] Yokohama City Univ, Sch Med, Yokohama, Kanagawa 2360027, Japan
基金
日本学术振兴会;
关键词
stars: abundances; stars: AGB and post-AGB; ISM: abundances; dust; extinction; ASYMPTOTIC GIANT BRANCH; LONG-PERIOD VARIABLES; MOLECULAR OPACITIES; METAL-POOR; CIRCUMSTELLAR ENVELOPES; ASTROPHYSICS MESA; SDSS J1148+5251; FORMING CLOUDS; CARBON DUST; C-STARS;
D O I
10.1093/mnras/stw3160
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Dust formation and the resulting mass loss around asymptotic giant branch (AGB) stars with initial metallicity in the range 0 <= Z(ini) <= 10(-4) and initial mass 2 <= M-ini/M-circle dot <= 5 are explored by hydrodynamical calculations of the dust-driven wind (DDW) along the AGB evolutionary tracks. We employ the MESA code to simulate the evolution of stars, assuming an empirical mass-loss rate in the post-main-sequence phase and considering three types of low-temperature opacity (scaled-solar, CO-enhanced and CNO-enhanced opacity) to elucidate the effect on stellar evolution and the DDW. We find that the treatment of low-temperature opacity strongly affects dust formation and the resulting DDW; in the carbon-rich AGB phase, the maximum. M of M-ini >= 3M(circle dot) stars with the CO-enhanced opacity is at least one order of magnitude smaller than that with the CNO-enhanced opacity. A wide range of stellar parameters being covered, the necessary condition for driving efficient DDW with. M >= 10(-6) M-circle dot yr(-1) is expressed as effective temperature T-eff less than or similar to 3850 K and log(delta L-C/kappa M-R) greater than or similar to 10.43 log T-eff -32.33, with the carbon excess delta(C) defined as epsilon(C) - epsilon(O), the Rosseland mean opacity.R in units of cm(2) g(-1) in the surface layer and the stellar mass (luminosity) M(L) in solar units. The fitting formulae derived for gas and dust mass-loss rates in terms of input stellar parameters could be useful for investigating the dust yield from AGB stars in the early Universe being consistent with stellar evolution calculations.
引用
收藏
页码:1709 / 1732
页数:24
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