2016A&A...588A..37H


Query : 2016A&A...588A..37H

2016A&A...588A..37H - Astronomy and Astrophysics, volume 588A37-37 (2016/4-1)

Abundances of carbon-enhanced metal-poor stars as constraints on their formation.

HANSEN C.J., NORDSTROM B., HANSEN T.T., KENNEDY C.R., PLACCO V.M., BEERS T.C., ANDERSEN J., CESCUTTI G. and CHIAPPINI C.

Abstract (from CDS):

Context. An increasing fraction of carbon-enhanced metal-poor (CEMP) stars is found as their iron abundance, [Fe/H], decreases below [Fe/H]=-2.0. The CEMP-s stars have the highest absolute carbon abundances, [C/H], and are thought to owe their enrichment in carbon and the slow neutron-capture (s-process) elements to mass transfer from a former asymptotic giant branch (AGB) binary companion. The most Fe-poor CEMP stars are normally single, exhibit somewhat lower [C/H] than CEMP-s stars, but show no s-process element enhancement (CEMP-no stars). Abundance determinations of CNO offer clues to their formation sites.
Aims. Our aim is to use the medium-resolution spectrograph X-Shooter/VLT to determine stellar parameters and abundances for C, N, Sr, and Ba in several classes of CEMP stars in order to further classify and constrain the astrophysical formation sites of these stars.
Methods. Atmospheric parameters for our programme stars were estimated from a combination of V-K photometry, model isochrone fits, and estimates from a modified version of the SDSS/SEGUE spectroscopic pipeline. We then used X-Shooter spectra in conjunction with the 1D local thermodynamic equilibrium spectrum synthesis code MOOG, 1D ATLAS9 atmosphere models to derive stellar abundances, and, where possible, isotopic 12C/13C ratios.
Results. Abundances (or limits) of C, N, Sr, and Ba are derived for a sample of 27 faint metal-poor stars for which the X-Shooter spectra have sufficient signal-to-noise ratios (S/N). These moderate resolution, low S/N (∼10-40) spectra prove sufficient to perform limited chemical tagging and enable assignment of these stars into the CEMP subclasses (CEMP-s and CEMP-no). According to the derived abundances, 17 of our sample stars are CEMP-s and 3 are CEMP-no, while the remaining 7 are carbon-normal. For four CEMP stars, the subclassification remains uncertain, and two of them may be pulsating AGB stars.
Conclusions. The derived stellar abundances trace the formation processes and sites of our sample stars. The [C/N] abundance ratio is useful for identifying stars with chemical compositions unaffected by internal mixing, and the [Sr/Ba] abundance ratio allows us to distinguish between CEMP-s stars with AGB progenitors and the CEMP-no stars. Suggested formation sites for the latter include faint supernovae with mixing and fallback and/or primordial, rapidly-rotating, massive stars (spinstars). X-Shooter spectra have thus proved to be valuable tools in the continued search for their origin.

Abstract Copyright: © ESO, 2016

Journal keyword(s): stars: abundances - stars: Population II - stars: carbon - nuclear reactions, nucleosynthesis, abundances - stars: chemically peculiar

Simbad objects: 33

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Number of rows : 33
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 HE 2358-4640 Pe* 00 00 50.9112333552 -46 23 31.346424996   14.3       CEMP-mp 5 0
2 HE 0058-3449 Pe* 01 01 21.7177096224 -34 33 10.608290676   13.918 13.203 13.126 12.377 CEMP-s 8 0
3 HE 0206-1916 Pe* 02 09 19.6321025088 -19 01 55.451633016   15.133 13.999 13.458 12.987 CEMP-s 22 0
4 BD+44 493 Pe* 02 26 49.7390353632 +44 57 46.523771136   9.63 9.11 9.073   CEMP-no 116 0
5 HE 0241-3512 Pe* 02 43 26.7740293632 -35 00 12.129681528   15.17 14.00 13.305 12.773 CEMP-s 7 0
6 UCAC4 115-002803 Pe* 03 13 00.3747928560 -67 08 39.336144504   15.442 14.753 14.639   CEMP-no 122 0
7 HE 0400-2030 Pe* 04 02 14.8021418088 -20 21 53.533679904   14.921 14.033 13.605 13.164 CEMP-s 20 0
8 HE 0408-1733 Pe* 04 11 06.0266169456 -17 25 39.745266096   13.511 12.335     CEMP-mp 11 0
9 HE 0414-0343 SB* 04 17 16.4631860496 -03 36 31.388697180   12.23 11.04     CEMP-r/s 21 0
10 HE 0430-4901 Pe* 04 31 31.1369700144 -48 54 41.518597500     14.572   13.770 CEMP-s 17 0
11 HE 0430-1609 Pe* 04 32 50.9240264664 -16 03 38.824888860   14.48 13.1 12.527 12.008 CEMP-s 13 0
12 HE 0440-3426 Pe* 04 42 08.1758822400 -34 21 13.869730368   12.88 11.44     CEMP-s 14 0
13 HE 0448-4806 Pe* 04 49 33.0494670384 -48 01 08.312761272   13.45 12.35     CEMP-s 13 0
14 HE 0516-2515 SB* 05 18 09.4817384592 -25 12 24.992694432   15.57 13.90 12.634 11.953 CEMP-no 8 0
15 GLEAM J092419-220140 QSO 09 24 19.92000 -22 01 41.4984       25.850   ~ 90 1
16 QSO J1120+0641 QSO 11 20 01.463 +06 41 23.79           ~ 262 0
17 C* 3289 C* 12 41 02.3989686024 -08 53 06.586709784     12.0   10.389 C 19 0
18 HD 112869 C* 12 59 22.6406750088 +37 49 03.688255308 12.83 10.72 8.91 7.79 6.92 C3,5CH9 92 0
19 HE 1315-2035 Pe* 13 17 57.4877038128 -20 50 52.861703856   17.05 15.70 14.770 14.318 CEMP-s 7 0
20 HE 1418+0150 SB* 14 21 01.1688766320 +01 37 17.834854152   13.7 12.205 11.335 10.936 CEMP-s 15 0
21 HE 1430-0919 Pe* 14 33 12.8284426056 -09 32 52.661125032   15.26 13.80 13.669 13.197 CEMP-s 8 0
22 HE 1431-0245 Pe* 14 33 54.1499119320 -02 58 32.583788724   16.58 15.30   14.223 CEMP-s 7 0
23 BPS CS 30322-0023 Pe* 21 30 32.1818994960 -46 16 24.614480388   13.447 12.167 11.902 10.908 CEMP-s 59 0
24 HE 2138-1616 Pe* 21 41 16.6096540440 -16 02 39.863733396   14.91 13.90     CEMP-mp 5 0
25 HE 2141-1441 Pe* 21 44 25.6762953072 -14 27 32.869448856   14.63 13.50     CEMP-mp 5 0
26 HE 2144-1832 SB* 21 46 54.6639160128 -18 18 15.587038476   12.651 10.97 10.471 9.860 CEMP-s 16 0
27 HE 2153-2323 Pe* 21 56 37.5847822872 -23 09 25.420064616   16.10 14.50   13.403 CEMP-s 9 1
28 2MASS J21584227-2029156 Pe* 21 58 42.2746240680 -20 29 15.746399232   14.1 13.156 12.692 12.225 CEMP-no 12 0
29 2MASS J22380795-5042416 Pe* 22 38 07.9560821352 -50 42 41.505459048   13.8       CEMP-s 8 0
30 2MASS J22533969-4213038 Pe* 22 53 39.7110580176 -42 13 03.821675880   13.2 12.0     CEMP-no 8 0
31 HE 2310-4523 Pe* 23 13 00.0416103048 -45 07 06.565285596   12.120 11.207 10.55   CEMP-mp 24 0
32 2MASS J23215820-5211431 Pe* 23 21 58.1901363600 -52 11 43.204631172   14.3       CEMP-no 13 0
33 HE 2357-2718 Pe* 23 59 58.1284315416 -27 01 37.629391764   14.313 13.078     CEMP-mp 12 0

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