2008ApJ...675.1223M


Query : 2008ApJ...675.1223M

2008ApJ...675.1223M - Astrophys. J., 675, 1223-1232 (2008/March-2)

Abundance anomalies in horizontal branch stars and atomic diffusion.

MICHAUD G., RICHER J. and RICHARD O.

Abstract (from CDS):

Using stellar evolution models in which atomic diffusion was included self-consistently throughout the evolution of a Population II 0.8 M☉ star (Y=0.2352, Z=0.0001, α=0.3) from the zero-age main sequence to the end of the core expansion phase on the horizonatal branch (HB), surface-abundance composition is calculated and compared to observations of HB stars in the globular cluster M15. The effect of turbulence is characterized by the outer mass it mixes. It is shown that the overabundances of Fe by a factor of 50-100 observed by Behr in the seven stars of that cluster with Teff>11,000 K require an outer mixed mass of about 10–7 M*. The abundance anomalies of Al, Si, S, Ca, Ti, Cr, and Ni, but not of Mg, are also reasonably well reproduced without any additional adjustment. This constitutes a convincing confirmation of the role of atomic diffusion driven by radiative accelerations in HB stars.

Abstract Copyright: ∼

Journal keyword(s): Diffusion - Galaxy: Globular Clusters: General - Galaxy: Globular Clusters: Individual: Messier Number: M15 - Stars: Abundances - Stars: Horizontal-Branch

CDS comments: Stars BNNN are Cl* NGC 7078 BBFP NNN

Simbad objects: 9

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Number of rows : 9
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 M 79 GlC 05 24 10.59 -24 31 27.3     8.16     ~ 883 0
2 NGC 2808 GlC 09 12 03.10 -64 51 48.6           ~ 1540 0
3 M 13 GlC 16 41 41.634 +36 27 40.75     5.8     ~ 2291 0
4 NGC 6752 GlC 19 10 52.11 -59 59 04.4           ~ 2121 0
5 NGC 7078 1080 * 21 29 56.502 +12 10 39.85   16.77 16.79     ~ 8 0
6 NGC 7078 637 * 21 29 57.266 +12 10 24.16   16.56 16.56     ~ 9 0
7 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0
8 NGC 7078 119 * ~ ~   16.78 16.80     ~ 8 0
9 NGC 7078 276 * ~ ~   16.67 16.68     ~ 9 0

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