2007ApJ...660..516T


Query : 2007ApJ...660..516T

2007ApJ...660..516T - Astrophys. J., 660, 516-540 (2007/May-1)

Supernova nucleosynthesis in population III 13-50 m☉ stars and abundance patterns of extremely metal-poor stars.

TOMINAGA N., UMEDA H. and NOMOTO K.

Abstract (from CDS):

We perform hydrodynamic and nucleosynthesis calculations of core-collapse supernovae (SNe) and hypernovae (HNe) of Population (Pop) III stars. We provide new yields for the main-sequence mass of MMS=13-50 M☉ and the explosion energy of E=1-40x1051 ergs to apply to chemical evolution studies. Our HN yields based on the mixing-fallback model of explosions reproduce the observed abundance patterns of extremely metal-poor (EMP) stars (-4<[Fe/H]←3), while those of very metal-poor (VMP) stars (-3<[Fe/H]←2) are reproduced by the normal SN yields integrated over the Salpeter initial mass function. Moreover, the observed trends of abundance ratios [X/Fe] against [Fe/H] with small dispersions for the EMP stars can be reproduced as a sequence resulting from the various combination of MMS and E. This is because we adopt the empirical relation that a larger amount of Fe is ejected by more massive HNe. Our results imply that the observed trends with small dispersions do not necessarily mean the rapid homogeneous mixing in the early Galactic halo at [Fe/H]←3 but can be reproduced by the ``inhomogeneous'' chemical evolution model. In addition, we examine how the modifications of the distributions of the electron mole fraction Ye and the density in the presupernova models improve the agreement with observations. In this connection, we discuss possible contributions of nucleosynthesis in the neutrino-driven wind and the accretion disk.

Abstract Copyright: ∼

Journal keyword(s): Galaxy: Halo - Nuclear Reactions, Nucleosynthesis, Abundances - Stars: Abundances - Stars: Population II - Stars: Supernovae: General

Simbad objects: 25

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Number of rows : 25
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 HD 2796 Pe* 00 31 16.9147531152 -16 47 40.790991624 9.58 9.28 8.50 8.14 8.67 Fw 203 0
2 CD-38 245 Pe* 00 46 36.1954514592 -37 39 33.555030480   12.733 11.929 13.39 10.996 KIIvw 233 0
3 HE 0107-5240 Pe* 01 09 29.1555567432 -52 24 34.202039148   15.89 15.07 15.10 14.283 CEMP-no 250 0
4 SN 2002ap SN* 01 36 23.85 +15 45 13.2   13.11 14.54     SNIc-BL 587 1
5 HE 0239-1340 Pe* 02 41 42.3721546152 -13 28 10.603797240   14.73 13.97 13.566 13.080 CEMP-no 64 0
6 2MASS J03142084-1035112 Pe* 03 14 20.8495451808 -10 35 11.277788028   13.54 12.73 12.204 11.693 KIIvw 73 0
7 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
8 SN 1997D SN* 04 11 01.00 -56 29 56.0       16.3   SNIIpec 184 1
9 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
10 SN 1997ef SN* 07 57 02.87 +49 33 41.3     16.5     SNIc-BL 281 1
11 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
12 SN 1993J SN* 09 55 24.77476 +69 01 13.7026   10.8 12.0     SNIIb 1507 1
13 SN 2005bf SN* 10 23 56.99 -03 11 29.3     18.0     SNIb 225 1
14 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
15 SN 2004aw SN* 11 57 50.24 +25 15 55.1   18.06       SNIc 209 1
16 SN 1999br SN* 13 00 41.80 +02 29 45.8     17.5     SNIIPp 171 1
17 SN 1994I SN* 13 29 54.072 +47 11 30.50     12.9     SNIc 645 1
18 HE 1327-2326 Pe* 13 30 05.9394958608 -23 41 49.699340844 13.761 14.01 13.55 13.50 12.803 CEMP-no 258 0
19 BD+17 3248 HB* 17 28 14.4690179544 +17 30 35.847574776   10.02 9.34     KIIvw 239 0
20 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
21 UCAC2 7177623 Pe* 19 42 26.8926894816 -56 58 34.059037980   14.27 13.63     ~ 57 0
22 HD 186478 SB* 19 45 14.1409752672 -17 29 27.071239056   10.116 9.302 8.527 7.961 K2III 166 0
23 BPS CS 22885-0096 Pe* 20 20 51.1730095656 -39 53 30.234972840   14.02 13.33     CEMP-no 96 0
24 BPS CS 29498-0043 Pe* 21 03 52.1197651440 -29 42 50.344181712   14.8 13.72 13.013 12.406 CEMP-no 100 0
25 2MASS J23485776-2939228 Pe* 23 48 57.7540034928 -29 39 22.824085392 14.759   14.3   13.512 ~ 38 0

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