2013MNRAS.431.1625C


Query : 2013MNRAS.431.1625C

2013MNRAS.431.1625C - Mon. Not. R. Astron. Soc., 431, 1625-1637 (2013/May-2)

The explosion energy of early stellar populations: the Fe-peak element ratios in low-metallicity damped Lyα systems.

COOKE R., PETTINI M., JORGENSON R.A., MURPHY M.T., RUDIE G.C. and STEIDEL C.C.

Abstract (from CDS):

The relative abundances of the Fe-peak elements (Ti-Zn) at the lowest metallicities are intimately linked to the physics of core-collapse supernova explosions. With a sample of 25 very metal poor damped Lyα systems (DLAs), we investigate the trends of the Fe-peak element ratios with metallicity. For nine of the 25 DLAs, a direct measurement (or useful upper limit) of one or more of the Ti, Cr, Co, Ni, Zn/Fe abundance ratios could be determined from detected absorption lines. For the remaining systems (without detections), we devised a new form of spectral stacking to estimate the typical Fe-peak element ratios of the DLA population in this metallicity regime. We compare these data to analogous measurements in metal-poor stars of the Galactic halo and to detailed calculations of explosive nucleosynthesis in metal-free stars. We conclude that most of the DLAs in our sample were enriched by stars that released an energy of ≲ 1.2x1051 erg when they exploded as core-collapse supernovae. Finally, we discuss the exciting prospect of measuring Fe-peak element ratios in DLAs with Fe/H < 1/1000 of solar when 30-m class telescopes become available. Only then will we be able to pin down the energy that was released by the supernovae of the first stars.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): supernovae: general - galaxies: abundances - galaxies: evolution - quasars: absorption lines

Simbad objects: 24

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Number of rows : 24
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 QSO J0003-2603 QSO 00 03 22.9531962024 -26 03 18.304471908   18 17.53     ~ 293 0
2 QSO J0035-0918 QSO 00 35 01.8852012984 -09 18 17.640206928   19.32 19.12     ~ 60 0
3 QSO B0112-30 QSO 01 15 04.8742901280 -30 25 14.952952308           ~ 50 1
4 QSO J0140-0839 QSO 01 40 49.1830961952 -08 39 42.462483840   19.62 18.57     ~ 57 0
5 QSO J0255+0048 QSO 02 55 18.5784341184 +00 48 47.540744316   21.15 20.00     ~ 84 0
6 QSO J0831+3358 QSO 08 31 02.5681902336 +33 58 03.088763328   19.20 19.00     ~ 44 0
7 QSO B0913+0715 QSO 09 16 13.9618240848 +07 02 24.497778588     17.1     ~ 109 0
8 QSO J1001+0343 QSO 10 01 51.4511281416 +03 43 01.496091612   19.59 19.29     ~ 43 0
9 QSO J1037+0139 QSO 10 37 24.4046481840 +01 39 33.974678340   19.88 19.51     ~ 30 0
10 QSO B1108-07 QSO 11 11 13.600 -08 04 02.00     18.10     ~ 85 0
11 QSO J1112+1333 QSO 11 11 51.6094494408 +13 32 35.858687640   17.30 17.08     ~ 37 0
12 QSO J1337+3152 QSO 13 37 24.6964232832 +31 52 54.575696928   19.40 19.01     ~ 58 1
13 QSO B1337+11 QSO 13 40 02.5419344664 +11 06 30.181521168     18.7     ~ 120 0
14 QSO J1358+6522 QSO 13 58 42.9160217208 +65 22 36.664532364   19.53 19.06     ~ 59 0
15 QSO J1419+5923 QSO 14 19 06.3130746264 +59 23 12.312356640   18.19 18.00     ~ 49 0
16 QSO J1419+0829 QSO 14 19 50.5527303624 +08 29 48.295169592   19.39 19.07     ~ 51 0
17 QSO J1558-0031 QSO 15 58 10.1642192448 -00 31 20.035621812   18.07 17.80     ~ 62 0
18 QSO J1558+4053 QSO 15 58 14.5121953872 +40 53 37.014549288   19.09 18.92     ~ 45 0
19 QSO B1946+770 QSO 19 44 54.8532392016 +77 05 52.673448048     15.8     ~ 156 0
20 QSO B2059-360 QSO 21 02 44.6068720464 -35 53 07.081042308   19.18 18.62     ~ 58 0
21 QSO J2155+1358 QSO 21 55 02.0017063296 +13 58 25.712205816     18.00     ~ 50 0
22 LBQS 2206-1958A QSO 22 08 52.0729138920 -19 43 59.866776948   17.49 17.33     ~ 223 0
23 QSO B2348-0108 QSO 23 50 57.8771296800 -00 52 09.886281492   19.23 18.77 18.7   ~ 152 0
24 QSO B2348-147 BLL 23 51 29.8153792680 -14 27 56.840819544     16.9     ~ 81 1

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