2014A&A...565A.100M


Query : 2014A&A...565A.100M

2014A&A...565A.100M - Astronomy and Astrophysics, volume 565A, 100-100 (2014/5-1)

Hot horizontal branch stars in NGC 288 - effects of diffusion and stratification on their atmospheric parameters.

MOEHLER S., DREIZLER S., LEBLANC F., KHALACK V., MICHAUD G., RICHER J., SWEIGART A.V. and GRUNDAHL F.

Abstract (from CDS):

NGC288 is a globular cluster with a well-developed blue horizontal branch (HB) covering the u-jump that indicates the onset of diffusion. It is therefore well suited to study the effects of diffusion in blue HB stars. We compare observed abundances with predictions from stellar evolution models calculated with diffusion and from stratified atmospheric models. We verify the effect of using stratified model spectra to derive atmospheric parameters. In addition, we investigate the nature of the overluminous blue HB stars around the u-jump. We defined a new photometric index sz from uvby measurements that is gravity-sensitive between 8000K and 12000K. Using medium-resolution spectra and Stroemgren photometry, we determined atmospheric parameters (Teff, logg) and abundances for the blue HB stars. We used both homogeneous and stratified model spectra for our spectroscopic analyses. The atmospheric parameters and masses of the hot HB stars in NGC288 show a behaviour seen also in other clusters for temperatures between 9000K and 14000K. Outside this temperature range, however, they instead follow the results found for such stars in ωCen. The abundances derived from our observations are for most elements (except He and P) within the abundance range expected from evolutionary models that include the effects of atomic diffusion and assume a surface mixed mass of 10–7M. The abundances predicted by stratified model atmospheres are generally significantly more extreme than observed, except for Mg. When effective temperatures, surface gravities, and masses are determined with stratified model spectra, the hotter stars agree better with canonical evolutionary predictions. Our results show definite promise towards solving the long-standing problem of surface gravity and mass discrepancies for hot HB stars, but much work is still needed to arrive at a self-consistent solution.

Abstract Copyright:

Journal keyword(s): stars: horizontal-branch - stars: atmospheres - techniques: spectroscopic - globular clusters: individual: NGC 288

VizieR on-line data: <Available at CDS (J/A+A/565/A100): table1.dat n288abu.dat>

Nomenclature: Table 1: [MDL2014] NNN N=68 among (Nos 52-357).

Errata: erratum vol. 605, art. C4 (2017)

Simbad objects: 82

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Number of rows : 82
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 Cl* NGC 288 SAN 26 HB* 00 52 24.3530030064 -26 35 23.685019440   16.50 16.83     ~ 7 0
2 Cl* NGC 288 ALC 137 HB* 00 52 27.4245191808 -26 35 58.933706964   16.16 16.42     ~ 12 0
3 Cl* NGC 288 ALC 130 HB* 00 52 29.9328425112 -26 36 07.522830972   16.0       ~ 3 0
4 Cl* NGC 288 ALC 131 HB? 00 52 32.0812161360 -26 35 46.759025832   15.5 14.51     ~ 6 0
5 [MDL2014] 107 HB* 00 52 32.3995675440 -26 36 30.382640460           ~ 1 0
6 Cl* NGC 288 SAN 10 HB* 00 52 33.1588960392 -26 33 44.743082004   16.0       ~ 3 0
7 Cl* NGC 288 SAN 28 HB* 00 52 35.4637017984 -26 39 11.107720944   15.796 15.684 15.909   ~ 6 0
8 [MDL2014] 74 HB? 00 52 35.4854816136 -26 34 24.944736612           ~ 1 0
9 [MDL2014] 147 HB* 00 52 37.2762783960 -26 36 47.101879044           ~ 1 0
10 Cl* NGC 288 SAN 12 HB? 00 52 37.6628249520 -26 31 13.665909720   16.0       ~ 6 0
11 Cl* NGC 288 SAN 13 HB* 00 52 37.7946053616 -26 39 31.740288840   16.0       ~ 3 0
12 [MDL2014] 89 HB? 00 52 37.8969824751 -26 36 35.517874473           ~ 1 0
13 [MDL2014] 60 HB? 00 52 38.6040714192 -26 37 05.243419272           ~ 1 0
14 [MDL2014] 114 HB* 00 52 38.6970663240 -26 37 49.800881640           ~ 1 0
15 [MDL2014] 100 HB* 00 52 38.6979551208 -26 35 58.740751536           ~ 2 0
16 [MDL2014] 127 HB* 00 52 39.3321241272 -26 34 31.677073572           ~ 1 0
17 [MDL2014] 113 HB* 00 52 39.4977132096 -26 36 45.823487544           ~ 1 0
18 [MDL2014] 183 HB* 00 52 39.9262422504 -26 37 23.956855968           ~ 2 0
19 [MDL2014] 145 HB* 00 52 40.6010212848 -26 32 48.740339184           ~ 1 0
20 [MDL2014] 81 HB? 00 52 40.7880870792 -26 33 47.782971900           ~ 1 0
21 [MDL2014] 79 HB? 00 52 42.7010883672 -26 34 50.354304132           ~ 1 0
22 [MDL2014] 61 HB? 00 52 42.8156592000 -26 36 39.360735504           ~ 1 0
23 Cl* NGC 288 SAN 29 HB* 00 52 42.8471406720 -26 31 06.951688320   16.0       ~ 9 0
24 [MDL2014] 146 HB* 00 52 43.3618454568 -26 37 56.574294024           ~ 3 0
25 [MDL2014] 240 HB* 00 52 43.7087417352 -26 35 01.878776088           ~ 3 0
26 [MDL2014] 243 HB* 00 52 44.02 -26 35 42.2           ~ 1 0
27 [MDL2014] 196 HB* 00 52 44.3044425000 -26 35 53.343327048           ~ 3 0
28 [MDL2014] 187 HB* 00 52 44.7232897176 -26 35 31.542387072           ~ 1 0
29 [MDL2014] 242 HB* 00 52 45.0309553416 -26 37 35.584498056           ~ 3 0
30 NGC 288 GlC 00 52 45.24 -26 34 57.4   10 8.13     ~ 1041 0
31 [MDL2014] 115 HB* 00 52 45.2566451664 -26 37 55.315735212           ~ 1 0
32 [MDL2014] 70 HB? 00 52 45.40 -26 35 21.5           ~ 1 0
33 [MDL2014] 167 HB? 00 52 46.42 -26 34 07.7           ~ 1 0
34 [MDL2014] 169 HB* 00 52 46.5197937000 -26 31 30.829450980           ~ 4 0
35 UCAC4 317-000960 HB? 00 52 46.6519272960 -26 39 03.256965540   15.646 15.542 15.559   ~ 2 0
36 [MDL2014] 231 HB* 00 52 47.0276555376 -26 36 23.130900324           ~ 2 0
37 [MDL2014] 63 HB? 00 52 47.0987317416 -26 35 25.117011816           ~ 1 0
38 [MDL2014] 228 HB* 00 52 47.3798989680 -26 37 52.771759500           ~ 3 0
39 [MDL2014] 55 HB? 00 52 47.4527235840 -26 33 14.246903124           ~ 1 0
40 [MDL2014] 179 HB* 00 52 48.1855494408 -26 35 20.014774548           ~ 2 0
41 [MDL2014] 151 HB* 00 52 48.3408210648 -26 32 57.668757144           ~ 1 0
42 [MDL2014] 304 HB* 00 52 48.6170607912 -26 33 17.221805712           ~ 4 0
43 [MDL2014] 176 HB* 00 52 48.7176007008 -26 34 00.771107628           ~ 2 0
44 [MDL2014] 300 HB* 00 52 49.1335673232 -26 35 35.274501600           ~ 2 0
45 [MDL2014] 288 HB* 00 52 49.3204556952 -26 38 19.300943184           ~ 2 0
46 [MDL2014] 275 HB* 00 52 49.4081690544 -26 35 53.899468800           ~ 3 0
47 [MDL2014] 347 HB* 00 52 50.3245024656 -26 38 30.180406236           ~ 3 0
48 [MDL2014] 156 HB* 00 52 50.5476752808 -26 35 12.165004032           ~ 1 0
49 [MDL2014] 142 HB* 00 52 50.5729459656 -26 36 49.952366388           ~ 3 0
50 [MDL2014] 52 HB? 00 52 50.7873388248 -26 38 03.076113336           ~ 1 0
51 [MDL2014] 180 HB* 00 52 50.9339386824 -26 36 09.575439264           ~ 3 0
52 [MDL2014] 102 HB* 00 52 51.4868425320 -26 36 26.196736644           ~ 1 0
53 [MDL2014] 88 HB? 00 52 52.1204925624 -26 34 12.164726820           ~ 1 0
54 [MDL2014] 221 HB* 00 52 52.3303314336 -26 35 13.758126828           ~ 3 0
55 [MDL2014] 86 HB? 00 52 52.5279560304 -26 34 29.820353376           ~ 1 0
56 [MDL2014] 143 HB* 00 52 52.7886755928 -26 34 53.155889364           ~ 1 0
57 [MDL2014] 157 HB* 00 52 53.7721872648 -26 39 08.830376820           ~ 1 0
58 UCAC4 317-000986 HB? 00 52 53.9367896472 -26 38 45.734633772   15.589 15.408 15.673   ~ 3 0
59 [MDL2014] 216 HB* 00 52 54.5889122016 -26 33 20.495987676           ~ 3 0
60 [MDL2014] 154 HB* 00 52 54.9071747352 -26 37 11.920821420           ~ 2 0
61 [MDL2014] 118 HB* 00 52 55.5269298888 -26 35 08.317181688           ~ 1 0
62 UCAC4 318-001165 HB* 00 52 55.5932167824 -26 32 58.837601184   15.48 15.50 15.775   ~ 4 0
63 UCAC4 318-001168 HB* 00 52 56.8598325288 -26 33 44.915591988   15.994 15.880 16.054   ~ 2 0
64 RGO 10703 HB* 00 52 59.3444628792 -26 39 00.542615544   16.42 16.68     ~ 11 0
65 [MDL2014] 292 HB* 00 53 00.0471062136 -26 36 33.081370884           ~ 3 0
66 UCAC4 317-000998 HB* 00 53 01.8641656512 -26 37 53.314177080       15.759   ~ 3 0
67 Cl* NGC 288 SAN 19 HB* 00 53 02.5701549072 -26 35 33.048290256   16.5       ~ 5 0
68 Cl* NGC 288 ALC 24 HB* 00 53 04.1717127552 -26 38 29.951135016   15.922 15.940 15.920   ~ 12 0
69 Cl* NGC 288 SAN 23 HB* 00 53 05.3320448616 -26 32 45.296094264   16.048 15.933 16.182   ~ 7 0
70 M 79 GlC 05 24 10.59 -24 31 27.3     8.16     ~ 817 0
71 NGC 2808 GlC 09 12 03.10 -64 51 48.6           ~ 1419 0
72 M 68 GlC 12 39 27.98 -26 44 38.6     7.96     ~ 997 0
73 NGC 5139 GlC 13 26 47.28 -47 28 46.1           ~ 3426 0
74 M 3 GlC 13 42 11.62 +28 22 38.2     6.39     ~ 2478 0
75 NGC 5986 GlC 15 46 03.00 -37 47 11.1     6.92     ~ 374 0
76 M 80 GlC 16 17 02.41 -22 58 33.9           ~ 715 0
77 M 13 GlC 16 41 41.634 +36 27 40.75     5.8     ~ 2192 0
78 M 92 GlC 17 17 07.39 +43 08 09.4     6.52     ~ 2115 0
79 M 22 GlC 18 36 23.94 -23 54 17.1           ~ 1378 0
80 NGC 6752 GlC 19 10 52.11 -59 59 04.4           ~ 2000 0
81 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3139 0
82 M 2 GlC 21 33 27.02 -00 49 23.7     6.25     ~ 1030 1

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