2014MNRAS.439.2638Y


Query : 2014MNRAS.439.2638Y

2014MNRAS.439.2638Y - Mon. Not. R. Astron. Soc., 439, 2638-2650 (2014/April-2)

Chemical abundances in bright giants of the globular cluster M62 (NGC 6266).

YONG D., ALVES BRITO A., DA COSTA G.S., ALONSO-GARCIA J., KARAKAS A.I., PIGNATARI M., ROEDERER I.U., AOKI W., FISHLOCK C.K., GRUNDAHL F. and NORRIS J.E.

Abstract (from CDS):

With the exception of Terzan 5, all the Galactic globular clusters that possess significant metallicity spreads, such as ω Cen and M22, are preferentially the more luminous clusters with extended horizontal branches. Here we present radial velocities and chemical abundances for seven bright giants in the globular cluster M62, a previously little-studied cluster. With MV = -9.18, M62 is the ninth most luminous Galactic globular cluster and has an extended horizontal branch. Within our sample, we find (i) no evidence for a dispersion in metallicity, [Fe/H], beyond the measurement uncertainties, (ii) star-to-star abundance variations for C, O, Na and Al with the usual correlations between these elements as seen in other globular clusters, and (iii) a global enrichment for the elements Zr, Ba and La at the level [X/Fe] ≃ +0.4dex. For elements heavier than La, the abundance ratios are consistent with the scaled-solar r-process distribution. Below La, the abundances are anomalous when compared to the scaled-solar s-process or r-process distributions. For these elements, the abundance signature in M62 is in agreement with predictions of the s-process from fast-rotating massive stars, although the high [Rb/Y] ratio we measure may be a challenge to this scenario.

Abstract Copyright: © 2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2014)

Journal keyword(s): stars: abundances - Galaxy: abundances - globular clusters: individual: NGC 6266

CDS comments: star d10 is 2MASS J17011703-3008198 , c53 is 2MASS J17011547-3008397 in Simbad.

Simbad objects: 31

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Number of rows : 31
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 NGC 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 4158 0
2 NGC 362 GlC 01 03 14.26 -70 50 55.6     6.58     ~ 1167 0
3 NGC 1851 GlC 05 14 06.76 -40 02 47.6           ~ 1529 0
4 M 79 GlC 05 24 10.59 -24 31 27.3     8.16     ~ 883 0
5 NGC 2419 GlC 07 38 08.51 +38 52 54.9     10.05     ~ 998 0
6 NGC 3201 GlC 10 17 36.82 -46 24 44.9           ~ 1001 0
7 NGC 5139 GlC 13 26 47.28 -47 28 46.1           ~ 3677 0
8 NGC 5824 GlC 15 03 58.612 -33 04 06.70   10.28 9.56     ~ 441 0
9 M 5 GlC 15 18 33.22 +02 04 51.7     5.95     ~ 2095 0
10 M 4 GlC 16 23 35.22 -26 31 32.7           ~ 1978 0
11 Cl* NGC 6266 ALC 124 * 17 01 00.280 -30 07 38.28     14.32     ~ 3 0
12 M 62 GlC 17 01 12.60 -30 06 44.5           ~ 668 0
13 Cl* NGC 6266 ALC 195 * 17 01 12.6323194320 -30 03 40.943202084           ~ 2 0
14 2MASS J17011547-3008397 * 17 01 15.472 -30 08 39.79           ~ 1 0
15 Cl* NGC 6266 ALC 5 * 17 01 16.210 -30 03 31.81     13.25     ~ 3 0
16 2MASS J17011703-3008198 * 17 01 17.0392147224 -30 08 19.843319400           ~ 1 0
17 Cl* NGC 6266 ALC 14 * 17 01 17.290 -30 03 58.69           ~ 2 0
18 Cl* NGC 6266 ALC 7 * 17 01 17.500 -30 03 20.60     13.19     ~ 3 0
19 Cl* NGC 6266 ALC 27 * 17 01 25.190 -30 04 09.85           ~ 2 0
20 ESO 455-11 GlC 17 31 05.20 -29 58 54.0           ~ 208 0
21 Cl Terzan 5 Cl* 17 48 05.00 -24 46 48.0           ~ 948 1
22 * 4 Sgr PM* 17 59 47.5564555824 -23 48 58.012965864   4.698 4.724     A0 95 0
23 NGC 6522 GlC 18 03 34.08 -30 02 02.3           ~ 569 0
24 NGC 6558 GlC 18 10 17.6 -31 45 50           ~ 265 0
25 HD 170642 * 18 32 21.3310764544 -39 42 14.402758830   5.233 5.155     A3V 41 0
26 M 22 GlC 18 36 23.94 -23 54 17.1           ~ 1459 0
27 M 54 GlC 18 55 03.33 -30 28 47.5           ~ 1164 0
28 NGC 6752 GlC 19 10 52.11 -59 59 04.4           ~ 2121 0
29 * b Aql PM* 19 24 58.1999714302 +11 56 39.888480530 6.35 5.93   4.7   G7IVHdel1 522 0
30 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0
31 M 2 GlC 21 33 27.02 -00 49 23.7     6.25     ~ 1114 1

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