2011ApJ...730L..16M


Query : 2011ApJ...730L..16M

2011ApJ...730L..16M - Astrophys. J., 730, L16 (2011/April-1)

Sodium-oxygen anticorrelation among horizontal branch stars in the globular cluster M4.

MARINO A.F., VILLANOVA S., MILONE A.P., PIOTTO G., LIND K., GEISLER D. and STETSON P.B.

Abstract (from CDS):

The horizontal branch (HB) morphology of globular clusters (GCs) is mainly governed by metallicity. The second parameter problem, well known since the 1960s, states that metallicity alone is not enough to describe the observed HB morphology of many GCs. Despite many efforts to resolve this issue, the second parameter phenomenon still remains without a satisfactory explanation. We have analyzed blue-HB, red-HB, and RR-Lyrae stars in the GC M4 and studied their Fe, Na, and O abundances. Our goal is to investigate possible connections between the bimodal HB of M4 and the chemical signatures of the two stellar populations recently discovered among red giants of this cluster. We obtained FLAMES-UVES/GIRAFFE spectra of a sample of 22 stars covering the HB from the red to the blue region. While iron has the same abundance in both the red-HB and blue-HB segments, the red-HB is composed of stars with scaled-solar sodium abundances, while the blue-HB stars are all sodium enhanced and oxygen depleted. The RR-Lyrae are Na-poor, as the red-HB stars, and O-rich. This is what we expect if the blue-HB consists of a second generation of stars formed from the ejecta produced by an earlier stellar population through high-temperature hydrogen-burning processes that include the CNO, NeNa, and MgAl cycles and are therefore expected to be He-rich. According to this scenario, the sodium and oxygen pattern detected in the blue-HB and red-HB segments suggests helium as the second parameter that rules the HB morphology in M4.

Abstract Copyright: ∼

Journal keyword(s): globular clusters: individual: NGC 6121 - stars: abundances - stars: Population II

Nomenclature: Table 1, col(1): [MVM2011] NNNNN N=22 among (Nos 22746-66604).

Simbad objects: 23

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Number of rows : 23
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 6121 464 HB* 16 23 09.6025657296 -26 31 05.434825296   14.36 13.47     ~ 12 0
2 NGC 6121 348 * 16 23 14.4003678144 -26 27 44.127204624   13.96 13.49     ~ 10 0
3 NGC 6121 516 HB* 16 23 17.6158283232 -26 34 05.549915352   14.32 13.40     ~ 9 0
4 2MASS J16232330-2634231 AB* 16 23 23.2885081152 -26 34 23.134104012   14.45 13.49     ~ 9 0
5 Cl* NGC 6121 SAW V7 RR* 16 23 25.9326520704 -26 27 41.992981632 14.56 14.09 13.42 12.94 12.40 ~ 26 0
6 NGC 6121 526 * 16 23 27.7602757776 -26 34 58.505827944   14.04 13.56     ~ 4 0
7 NGC 6121 357 HB* 16 23 28.1465792845 -26 26 08.566699800   14.369 13.252 13.131   ~ 12 0
8 2MASS J16233193-2631314 HB* 16 23 31.9368315072 -26 31 31.517683140   14.344 13.40     ~ 8 0
9 NGC 6121 365 HB* 16 23 32.9362150272 -26 27 50.209798320   14.41 13.41     ~ 11 0
10 NGC 6121 531 HB* 16 23 33.9154651200 -26 35 09.420930492   14.08 13.56     ~ 10 0
11 M 4 GlC 16 23 35.22 -26 31 32.7           ~ 1978 0
12 NGC 6121 16 * 16 23 35.66 -26 28 38.3   13.94 13.42     ~ 8 0
13 NGC 6121 117 * 16 23 35.7324582048 -26 30 47.956749804   13.703 13.329     ~ 5 0
14 NGC 6121 537 * 16 23 37.3139513208 -26 34 09.374819628   14.52 13.52     ~ 9 0
15 NGC 6121 66 * 16 23 38.75184 -26 30 00.0072   14.32 13.31     ~ 10 0
16 Cl* NGC 6121 SAW V25 RR* 16 23 39.3979780920 -26 30 21.395047284 14.07 13.94 13.23 12.74 12.20 ~ 23 0
17 NGC 6121 193 * 16 23 40.23000 -26 32 04.1712   14.56 13.46     ~ 6 0
18 NGC 6121 29 * 16 23 41.3457277874 -26 29 08.841135799   14.33 13.38     ~ 10 0
19 Cl* NGC 6121 ALC 321 * 16 23 44.18 -26 28 24.3   13.63 13.16     ~ 6 0
20 NGC 6121 548 Pe* 16 23 44.3244994584 -26 36 05.347225656   14.37 13.45     ~ 7 0
21 NGC 6121 608 HB* 16 23 48.0272431056 -26 36 43.631538552   14.30 13.37     ~ 10 0
22 NGC 6121 436 HB* 16 23 52.2836637552 -26 30 25.282472184   14.29 13.27     ~ 10 0
23 NGC 6121 450 HB* 16 24 13.6294969320 -26 30 04.609047672   14.19 13.25     ~ 9 0

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