2023A&A...677A.119D


Query : 2023A&A...677A.119D

2023A&A...677A.119D - Astronomy and Astrophysics, volume 677A119 (2023/9-1)

Angular momentum and lithium transport from main sequence to sub-giant and red giant low-mass stars.

DUMONT T.

Abstract (from CDS):

Context. Asteroseismology provides a unique opportunity to probe the interiors of evolved stars and constrain their internal rotation. The correct reproduction of the core rotation evolution has not yet been achieved, although it is key to understanding the internal processes involved in low-mass stars.
Aims. We explore the efficiency required to reproduce the general behaviour of the transport of angular momentum along the evolution in view of asteroseismic constraints from giant low-mass stars. We analyse the consequences and predictions for lithium and beryllium surface abundances from the main sequence to red giant phase.
Methods. We computed a series of models, which included atomic diffusion, rotation-induced mixing, magnetic braking, and additional processes tailored for main sequence low-mass stars. We extended these models to more evolved phases and investigated an updated angular momentum transport by including a time-dependent extra viscosity related to the azimuthal magneto-rotational instability. We compared our predictions to the asteroseismic measurements of the core and surface rotation of a sample of sub-giant and red giant stars. We compared the model predictions for the lithium and beryllium surface evolution with the available observations.
Results. We confirm that a time-dependent additional viscosity νadd(t) is required to reproduce the general behaviour of the core rotation rate along successive stellar evolutionary phases given the dependence on the differential rotation and the mass. We show that it results in stronger lithium and beryllium depletions for low-mass stars over evolution. We confirm that predicted lithium abundances at the red giant bump by classical models, commonly used as references, cannot reproduce the lithium depletion along the main sequence and evolved phases of stellar evolution. We show that the observed amount of lithium of stars less massive than 1 M⊙ leads to a discrepancy between model predictions and observations at the red giant bump.
Conclusions. We show that a semi-parametric model can reproduce the rotational behaviour along the first phases of evolution well, with the exception of the sharp transition observed during the sub-giant phase. This suggests that two distinct transport processes may be involved. The processes required to transport chemicals during the main sequence phase and angular momentum until the red giant phase impact the lithium depletion all along the evolutionary duration. A good prediction of the lithium abundance at young phases places strong constraints on the predicted one at more evolved phases. It also highlights discrepancies between models and observations for the lowest mass stars and impacts the threshold that defines lithium-rich giant stars, showing that classical models tend to overestimate this threshold.

Abstract Copyright: © The Authors 2023

Journal keyword(s): stars: abundances - stars: rotation - stars: evolution - stars: interiors - stars: low-mass - open clusters and associations: general

Simbad objects: 13

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Number of rows : 13
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 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
2 HD 49178 PM* 06 48 53.8179652461 +37 30 18.436463504   8.76 8.07     G0 58 0
3 NGC 2420 OpC 07 38 24.6 +21 34 26   9.0 8.3     ~ 523 0
4 NGC 2682 OpC 08 51 23.5 +11 48 54           ~ 2528 0
5 2MASS J18441281+4332024 RG* 18 44 12.8095920264 +43 32 02.367065760   10.756 9.676 9.465   K1IV 45 0
6 TYC 3541-1117-1 RG* 18 59 09.8407415520 +46 17 05.703253368   11.99 10.99     ~ 31 0
7 TYC 3124-433-1 * 19 04 54.5382998976 +40 55 39.842672340   12.59 11.36     K0III 30 0
8 2MASS J19055103+3930412 RG* 19 05 51.0323748192 +39 30 41.141047572           K2 38 0
9 BD+41 3315 PM* 19 20 29.3442099120 +41 17 28.510142676   9.92 9.38     F9IV-V 55 0
10 TYC 3555-1403-1 * 19 20 52.7286151344 +51 28 18.186868416   10.68 9.78     K0III-IV 46 0
11 HD 182736 PM* 19 24 03.3792608280 +44 56 00.738992328   7.82 7.01     G8IV 88 0
12 BD+44 3244 * 19 46 17.8465825824 +44 49 39.614328156   10.24 9.51     G5IV-V 53 0
13 HD 190319 PM* 20 02 33.3210896856 +44 31 58.994152536   10.63 9.91     G2.5V 46 0

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