2012ApJ...761..161S


Query : 2012ApJ...761..161S

2012ApJ...761..161S - Astrophys. J., 761, 161 (2012/December-3)

Identifying contributions to the stellar halo from accreted, kicked-out, and in situ populations.

SHEFFIELD A.A., MAJEWSKI S.R., JOHNSTON K.V., CUNHA K., SMITH V.V., CHEUNG A.M., HAMPTON C.M., DAVID T.J., WAGNER-KAISER R., JOHNSON M.C., KAPLAN E., MILLER J. and PATTERSON R.J.

Abstract (from CDS):

We present a medium-resolution spectroscopic survey of late-type giant stars at mid-Galactic latitudes of (30° <|b| < 60°), designed to probe the properties of this population to distances of ∼9 kpc. Because M giants are generally metal-rich and we have limited contamination from thin disk stars by the latitude selection, most of the stars in the survey are expected to be members of the thick disk ( < [Fe/H] > ∼ -0.6) with some contribution from the metal-rich component of the nearby halo. Here we report first results for 1799 stars. The distribution of radial velocity (RV) as a function of l for these stars shows (1) the expected thick disk population and (2) local metal-rich halo stars moving at high speeds relative to the disk, which in some cases form distinct sequences in RV-l space. High-resolution echelle spectra taken for 34 of these "RV outliers" reveal the following patterns across the [Ti/Fe]-[Fe/H] plane: 17 of the stars have abundances reminiscent of the populations present in dwarf satellites of the Milky Way, 8 have abundances coincident with those of the Galactic disk and a more metal-rich halo, and 9 of the stars fall on the locus defined by the majority of stars in the halo. The chemical abundance trends of the RV outliers suggest that this sample consists predominantly of stars accreted from infalling dwarf galaxies. A smaller fraction of stars in the RV outlier sample may have been formed in the inner Galaxy and subsequently kicked to higher eccentricity orbits, but the sample is not large enough to distinguish conclusively between this interpretation and the alternative that these stars represent the tail of the velocity distribution of the thick disk. Our data do not rule out the possibility that a minority of the sample could have formed from gas in situ on their current orbits. These results are consistent with scenarios where the stellar halo, at least as probed by M giants, arises from multiple formation mechanisms; however, when taken at face value, our results for metal-rich halo giants suggest a much higher proportion to be accreted than found by Carollo et al. and more like the fraction suggested in the analysis by Nissen & Schuster and Schuster et al. We conclude that M giants with large RVs can provide particularly fruitful samples to mine for accreted structures and that some of the velocity sequences may indeed correspond to real physical associations resulting from recent accretion events.

Abstract Copyright:

Journal keyword(s): Galaxy: disk - Galaxy: evolution - Galaxy: formation - Galaxy: halo - Galaxy: kinematics and dynamics - solar neighborhood - stars: abundances

Nomenclature: Table 1: [SMJ2012] JHHMMSSs+DDMMSS N=39

Simbad objects: 51

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Number of rows : 51
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 * alf Tau LP? 04 35 55.23907 +16 30 33.4885 4.32 2.40 0.86 -0.37 -1.31 K5+III 1255 2
2 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17424 0
3 2MASS J08072064+4354179 RG* 08 07 20.6405340888 +43 54 18.027063936   11.90 10.46     M 2 0
4 2MASS J08302442+2838120 RG* 08 30 24.4210286280 +28 38 11.991413688   12.38 10.39     M 3 0
5 2MASS J09034712+4149437 RG* 09 03 47.1368408448 +41 49 43.616635104   11.30 9.95     M 3 0
6 2MASS J09130919+4509162 RG* 09 13 09.1920495648 +45 09 16.277318676   12.81 11.57 11.1   M 3 0
7 2MASS J09185733+1457486 RG* 09 18 57.3293453976 +14 57 48.474262224           M 1 0
8 2MASS J09320380+0555206 RG* 09 32 03.8132900592 +05 55 20.921636136           M 1 0
9 BD+42 2025 RG* 09 35 55.6027579440 +41 40 45.711454656   11.13 9.60     K0 2 0
10 2MASS J09382042+1129503 RG* 09 38 20.4248285496 +11 29 50.441046504           M 1 0
11 IRAS 09475+0838 RG* 09 50 14.7003922344 +08 23 56.450376132   12.55 10.26     M 6 0
12 2MASS J10015928+1145073 RG* 10 01 59.2887655416 +11 45 07.359874524           M 1 0
13 2MASS J10114976+2305036 RG* 10 11 49.7668223424 +23 05 03.676295760   13.61 11.56     M 2 0
14 ASAS J102457+0049.0 V* 10 24 57.1475084544 +00 48 59.576492052     11.24 10.33   M 3 0
15 TYC 5495-1511-1 RG* 10 37 41.4094277832 -12 10 47.838551556   12.521 10.871 10.545 9.146 M 8 0
16 2MASS J10540354-0651241 RG* 10 54 03.5305509432 -06 51 24.204654720           M 1 0
17 2MASS J11010240-0030040 RG* 11 01 02.4004255200 -00 30 04.310365824   12.422 10.868 10.420   M 5 0
18 2MASS J11015898+0840434 RG* 11 01 58.9708176168 +08 40 43.140041616           M 1 0
19 ATO J166.2658-16.6666 RG* 11 05 03.8172543384 -16 39 59.913309132   13.137 11.391     M 8 0
20 ATO J168.9067+00.1334 RG* 11 15 37.6143433608 +00 08 00.548059164   14.24 12.68 12.18   M 12 0
21 FBS 1128-057 LP* 11 31 24.3165434928 -05 58 24.560557248   13.978 12.367     M6/7 10 0
22 2MASS J11365274+0259486 RG* 11 36 52.7510242224 +02 59 48.701313708   12.86 11.04     M 2 0
23 * ome Vir LP* 11 38 27.6074536027 +08 08 03.459408149 8.46 6.93 5.36     M4.5:III 107 0
24 TYC 272-624-1 RG* 11 45 07.1663054928 +01 37 27.234923376   13.07 10.91 10.65   M 12 0
25 * nu. Vir LP* 11 45 51.5595979999 +06 31 45.748996439 7.32 5.54 4.04 2.79 1.78 M1III 259 0
26 TYC 4942-507-1 RG* 12 06 18.2656078776 -03 50 44.964847824   12.651 10.881 10.622   M 7 0
27 * del Vir RG* 12 55 36.2086240844 +03 23 50.888053818 6.76 4.97 3.38 1.86 0.53 M3+III 272 0
28 2MASS J13131756-1642197 RG* 13 13 17.5827425760 -16 42 19.740030588           M 1 0
29 2MASS J13141250-1323517 RG* 13 14 12.5097100152 -13 23 51.557085492   12.67 10.55     M 4 0
30 BD-05 3727 RG* 13 34 56.7490536024 -05 51 57.835323864   12.708 11.146 10.12 9.248 M 8 0
31 ATO J208.8164-05.5637 RG* 13 55 15.9674090544 -05 33 49.571104536           M 6 0
32 2MASS J14045147-0041565 RG* 14 04 51.4683690144 -00 41 56.478795720   13.18 11.43     M 3 0
33 * alf Boo RG* 14 15 39.67207 +19 10 56.6730 2.46 1.18 -0.05 -1.03 -1.68 K1.5IIIFe-0.5 2318 1
34 UCAC4 424-060065 RG* 14 31 30.2184550872 -05 17 30.283861056   13.133 11.650 11.432 10.248 M 9 0
35 ATO J220.5147-16.3971 RG* 14 42 03.5344517544 -16 23 49.559329428   13.404 11.601     M 7 0
36 ROTSE1 J150930.64+252911.8 LP* 15 09 30.6524917824 +25 29 11.874784308           M 4 0
37 2MASS J15180649-1155361 RG* 15 18 06.5000255064 -11 55 36.308690112           M 1 0
38 2MASS J15210207+0823199 RG* 15 21 02.0788589304 +08 23 20.022024012   12.47 11.17     M 2 0
39 2MASS J15302572+3234092 RG* 15 30 25.7188186800 +32 34 09.182383680   12.31 10.51     M 2 0
40 2MASS J15351781+1353308 RG* 15 35 17.8115644368 +13 53 30.867547524   12.26 10.64     M 2 0
41 2MASS J15460438+0615543 RG* 15 46 04.3809747552 +06 15 54.430714440   13.06 11.25     M 2 0
42 2MASS J15464681+2700522 RG* 15 46 46.8181411848 +27 00 52.089110424   12.27 10.74     M 3 0
43 BD+06 3271 RG* 16 40 35.7905857992 +06 02 50.790860664   11.20 9.66     K0 2 0
44 2MASS J17195957+3011455 RG* 17 19 59.5713397296 +30 11 45.557599092   11.71 10.41     M 2 0
45 BD+40 3161 RG* 17 31 34.2820529592 +40 15 42.735642984   10.95 9.33     K5 2 0
46 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 14400 0
47 M 71 GlC 19 53 46.49 +18 46 45.1           ~ 1127 0
48 NAME Pisces Overdensity G 23 19.0 +00 00           ~ 54 0
49 NAME Orphan Stream St* ~ ~           ~ 253 0
50 NAME Monoceros Stream St* ~ ~           ~ 358 1
51 NAME Triangulum-Andromeda Region reg ~ ~           ~ 85 0

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