2010A&A...522A..10C


Query : 2010A&A...522A..10C

2010A&A...522A..10C - Astronomy and Astrophysics, volume 522, A10-10 (2010/11-1)

Thermohaline instability and rotation-induced mixing. I. Low- and intermediate-mass solar metallicity stars up to the end of the AGB.

CHARBONNEL C. and LAGARDE N.

Abstract (from CDS):

Numerous spectroscopic observations provide compelling evidence for non-canonical processes that modify the surface abundances of low- and intermediate-mass stars beyond the predictions of standard stellar theory. We study the effects of thermohaline instability and rotation-induced mixing in the 1-4M range at solar metallicity. We present evolutionary models by considering both thermohaline and rotation-induced mixing in stellar interior. We discuss the effects of these processes on the chemical properties of stars from the zero age main sequence up to the end of the second dredge-up on the early-AGB for intermediate-mass stars and up to the AGB tip for low-mass stars. Model predictions are compared to observational data for lithium, 12C/13C, [N/C], [Na/Fe], 16O/17O, and 16O/18O in Galactic open clusters and in field stars with well-defined evolutionary status, as well as in planetary nebulae. Thermohaline mixing simultaneously accounts for the observed behaviour of 12C/13C, [N/C], and lithium in low-mass stars that are more luminous than the RGB bump, and its efficiency is increasing with decreasing initial stellar mass. On the TP-AGB, thermohaline mixing leads to lithium production, although the 7Li yields remain negative. Although the 3He stellar yields are much reduced thanks to this process, we find that solar-metallicity, low-mass stars remain net 3He producers. Rotation-induced mixing is found to change the stellar structure so that in the mass range between ∼1.5 and 2.2M the thermohaline instability occurs earlier on the red giant branch than in non-rotating models. Finally rotation accounts for the observed star-to-star abundance variations at a given evolutionary status, and is necessary to explain the features of CN-processed material in intermediate-mass stars. Overall, the present models account for the observational constraints very well over the whole mass range presently investigated.

Abstract Copyright:

Journal keyword(s): instabilities - stars: abundances - stars: interiors - stars: rotation - stars: evolution - hydrodynamics

Errata: + corrigendum vol. 570, p. C2 (2014)

Simbad objects: 24

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Number of rows : 24
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 NAME Sculptor Dwarf Galaxy G 01 00 09.4 -33 42 32   9.79 8.6 8.81   ~ 1358 4
2 NGC 752 OpC 01 56 53.5 +37 47 38           ~ 642 0
3 NGC 1817 OpC 05 12 33.4 +16 41 46           ~ 180 0
4 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17428 0
5 NGC 1883 OpC 05 25 55.2 +46 29 35     12.0     ~ 48 0
6 NGC 2141 OpC 06 02 56.2 +10 27 04           ~ 145 0
7 NGC 2158 OpC 06 07 26.9 +24 05 56           ~ 294 0
8 NGC 2360 OpC 07 17 46.3 -15 37 52           ~ 194 0
9 PN M 1-17 PN 07 40 22.1724359520 -11 32 29.783641164           ~ 100 0
10 NGC 2447 OpC 07 44 33.8 -23 51 11           ~ 149 1
11 NGC 2682 OpC 08 51 23.0 +11 48 50           ~ 2342 0
12 NGC 3532 OpC 11 05 40.1 -58 42 25           ~ 350 0
13 IC 2714 OpC 11 17 29.5 -62 43 08     8.2     ~ 97 0
14 NGC 3680 OpC 11 25 34.1 -43 14 24   8.40 7.6     ~ 319 0
15 NGC 5822 OpC 15 04 12.2 -54 21 58           ~ 208 0
16 NGC 6134 OpC 16 27 48.7 -49 09 40   7.89 7.2     ~ 152 0
17 NGC 6281 OpC 17 04 43.0 -37 56 53           ~ 137 0
18 IC 4651 OpC 17 24 50.9 -49 55 01           ~ 350 0
19 NGC 6633 OpC 18 27 22.8 +06 36 54           ~ 385 0
20 IC 4756 OpC 18 38 35.8 +05 26 06           ~ 241 0
21 NGC 6781 PN 19 18 28.085 +06 32 19.29     11.8     ~ 261 0
22 V* V441 Cyg S* 20 27 08.1147520512 +36 33 06.503128128   12.04 9.80 7.58   S4,6 49 0
23 NGC 6939 OpC 20 31 40.1 +60 39 11           ~ 159 0
24 NGC 7142 OpC 21 45 09.6 +65 46 55   10.36 9.3     ~ 143 0

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