2009ApJ...698.1963R


Query : 2009ApJ...698.1963R

2009ApJ...698.1963R - Astrophys. J., 698, 1963-1980 (2009/June-3)

The end of nucleosynthesis: production of lead and thorium in the early galaxy.

ROEDERER I.U., KRATZ K.-L., FREBEL A., CHRISTLIEB N., PFEIFFER B., COWAN J.J. and SNEDEN C.

Abstract (from CDS):

We examine the Pb and Th abundances in 27 metal-poor stars (-3.1< [Fe/H] ←1.4) whose very heavy metal (Z > 56) enrichment was produced only by the rapid (r-) nucleosynthesis process. New abundances are derived from Hubble Space Telescope/Space Telescope Imaging Spectrograph, Keck/High Resolution Echelle Spectrograph, and Very Large Telescope/UV-Visual Echelle Spectrograph spectra and combined with other measurements from the literature to form a more complete picture of nucleosynthesis of the heaviest elements produced in the r-process. In all cases, the abundance ratios among the rare earth elements and the third r-process peak elements considered (La, Eu, Er, Hf, and Ir) are constant and equivalent to the scaled solar system r-process abundance distribution. We compare the stellar observations with r-process calculations within the classical "waiting-point" approximation. In these computations a superposition of 15 weighted neutron-density components in the range 23 ≤log nn≤ 30 is fit to the r-process abundance peaks to successfully reproduce both the stable solar system isotopic distribution and the stable heavy element abundance pattern between Ba and U in low-metallicity stars. Under these astrophysical conditions, which are typical of the "main" r-process, we find very good agreement between the stellar Pb r-process abundances and those predicted by our model. For stars with anomalously high Th/Eu ratios (the so-called actinide boost), our observations demonstrate that any nucleosynthetic deviations from the main r-process affect–at most–only the elements beyond the third r-process peak, namely Pb, Th, and U. Our theoretical calculations also indicate that possible r-process abundance "losses" by nuclear fission are negligible for isotopes along the r-process path between Pb and the long-lived radioactive isotopes of Th and U.

Abstract Copyright:

Journal keyword(s): Galaxy: halo - nuclear reactions, nucleosynthesis, abundances - stars: abundances - stars: Population II

Simbad objects: 57

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Number of rows : 57
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2025
#notes
1 HE 0024-2523 Pe* 00 27 27.6486469632 -25 06 28.289948508 15.067 15.32 14.91     CEMP-s 68 0
2 BPS CS 29497-0004 Pe* 00 28 06.9155612016 -26 03 04.269055032   14.76 14.07 13.583 13.116 ~ 63 0
3 V* CM Cet LP? 00 33 14.3108581872 -10 43 42.728423844   10.66 9.48 8.84 9.06 G3/5V 106 0
4 CD-24 266 BS* 00 40 47.9313619824 -24 07 34.183333668   12.955 12.656 12.441 12.216 CEMP-s 98 0
5 HD 6268 Pe* 01 03 18.1716378504 -27 52 49.953768852   9.725 9.046 8.601   F/Gw 162 0
6 2MASS J01261795+0607248 Pe* 01 26 17.9451748632 +06 07 24.727884996           CEMP-s 20 0
7 BD-16 251 RG* 01 29 31.1311443552 -16 00 45.495314460 12.527 12.427 11.642 11.189 10.713 CEMP 312 0
8 BPS CS 31079-0028 Pe* 03 01 00.6866893176 +06 16 31.808500140   13.900 13.211 12.713 12.190 ~ 37 0
9 BPS CS 29526-0110 Pe* 03 27 43.6392396600 -23 00 29.924362260   13.71 13.35 13.116 12.834 CEMP-r/s 53 0
10 BD+06 648 Pe* 04 13 13.1126763288 +06 36 01.768985496   10.27 9.09 8.58   K0 116 0
11 V* HP Eri LP* 04 38 55.7330378304 -13 20 48.133934448 10.91 9.72 8.33     G8/K0IIIwF7 138 0
12 HD 74462 RG* 08 48 20.6518818744 +67 26 59.884515744   9.65 8.69 8.25   G5IV 139 0
13 HE 1219-0312 Pe* 12 21 34.1430245160 -03 28 39.636260184     15.940   15.043 ~ 45 0
14 HD 108317 Pe* 12 26 36.8319587208 +05 18 09.023783400       7.7   G2IVm-5 178 0
15 HD 108577 Pe* 12 28 16.8614710944 +12 20 41.089853184   10.18 9.6 9.8   KIIvw 83 0
16 BD+04 2621 Pe* 12 28 44.6433260568 +04 01 26.631027984   10.86 9.90     KIIvw 61 0
17 HD 115444 Pe* 13 16 42.4590842616 +36 22 52.692135420   9.77 8.97 8.3 7.88 G9V 249 0
18 HD 122563 Pe* 14 02 31.8455084952 +09 41 09.944391876 7.47 7.10 6.19 5.37 4.79 G8:III:Fe-5 905 0
19 HD 122956 Pe* 14 05 13.0244442888 -14 51 25.455804480   8.18 7.3 6.88   G6IV/VwF6 166 0
20 BD+01 2916 Pe* 14 21 45.2614710696 +00 46 59.173056516   10.93 9.65     KIIvw 97 0
21 BD+08 2856 Pe* 14 23 58.1664038424 +08 01 33.333124908   10.90 10.08     KIIvw 68 0
22 HD 126587 Pe* 14 27 00.3636631296 -22 14 38.992940592   9.88 9.60 8.75   CEMP-no 141 0
23 HD 128279 Pe* 14 36 48.5108525999 -29 06 46.612858494 8.64 8.63 8.00     Gw 210 0
24 BD+30 2611 Pe* 15 06 53.8282684752 +30 00 36.941373756 11.50 10.37 9.13     G8III 149 0
25 Z 318-18 G 15 09 08.0 +67 13 21   13.60 10.6     ~ 1433 0
26 2MASS J15095862+6716200 RB? 15 09 58.6103318448 +67 16 20.032584024   18.53 17.006   15.614 ~ 41 0
27 BPS CS 30306-0132 Pe* 15 14 18.9191634456 +07 27 02.680959780   13.62 12.73 12.421 11.948 ~ 39 0
28 M 5 GlC 15 18 33.22 +02 04 51.7     5.95     ~ 2070 0
29 NGC 5904 860 RG* 15 18 44.4962016312 +02 02 05.423756928   14.4600 13.2300   12.0046 ~ 37 0
30 NGC 5904 865 RG* 15 18 44.9526006144 +02 02 03.568247448   13.8900 12.2000   10.6289 ~ 42 0
31 HE 1523-0901 Pe* 15 26 01.0697532504 -09 11 38.885639784   12.37 11.50 10.476 9.863 CEMP 91 0
32 HD 141531 PM* 15 49 16.4993243976 +09 36 42.408069804   10.31 9.08 8.720   M1V 74 0
33 NGC 6205 70 RG* 16 41 23.5306872480 +36 30 17.265922560   13.71 12.12     ~ 93 0
34 M 13 GlC 16 41 41.634 +36 27 40.75     5.8     ~ 2268 0
35 NGC 6205 598 RG* 16 41 41.9443189176 +36 26 51.715259736   13.64 12.00     ~ 57 0
36 2MASS J16414255+3626563 RG* 16 41 42.5493186408 +36 26 56.173428780   13.42 11.94     ~ 38 0
37 NGC 6205 973 RG* 16 41 50.9158586208 +36 28 54.352362612   13.65 11.91     ~ 73 0
38 NGC 6341 7018 RG* 17 16 37.4894075472 +43 06 15.600437640   13.47 12.18     ~ 77 0
39 M 92 GlC 17 17 07.39 +43 08 09.4     6.52     ~ 2206 0
40 BD+17 3248 HB* 17 28 14.4690179544 +17 30 35.847574776   10.02 9.34     KIIvw 235 0
41 HD 175305 RG* 18 47 06.4416868934 +74 43 31.451436187 8.07 7.93 7.18 6.52 6.03 G5III 234 0
42 HD 186478 SB* 19 45 14.1409752672 -17 29 27.071239056   10.116 9.302 8.527 7.961 K2III 163 0
43 HD 187861 SB* 19 56 26.9442832128 -65 22 08.014212084   10.42 9.18     CEMP-rs 67 0
44 BD-18 5550 Pe* 19 58 49.7371417608 -18 12 11.140126164 10.18 10.03 9.35 9.04 8.74 CEMP-no 182 0
45 HD 204543 * 21 29 28.2126852216 -03 30 55.353564216   9.17 8.30 7.99   F6/8(V) 142 0
46 NGC 7078 341 RG* 21 29 54.9258244080 +12 13 22.484816292   13.72 12.54   11.22 ~ 60 0
47 NGC 7078 462 RG* 21 29 56.6627934840 +12 09 46.341312228   14.45 12.90     ~ 40 0
48 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3249 0
49 NGC 7078 583 RG* 21 29 58.5643129152 +12 09 21.382732260   14.26 12.83     ~ 34 0
50 HD 206739 PM* 21 44 23.9461069656 -11 46 22.843385220   9.45 8.60 8.14   G5V 82 0
51 HD 235766 PM* 22 14 47.1706275528 +50 47 15.413299080   10.03 9.01     G5 13 0
52 BPS CS 22892-0052 Pe* 22 17 01.6558764360 -16 39 27.051026544   14.03 13.20 13.06 12.19 KIIvw 464 0
53 BPS CS 29491-0069 Pe* 22 31 02.1859040712 -32 38 36.526573572   13.72 13.1 12.654 12.175 ~ 39 0
54 HD 214925 LP? 22 41 59.4323837856 -20 47 03.709481964   10.77 9.30     (F) 38 0
55 HD 216143 Pe* 22 50 31.0883724288 -06 54 49.554279360   8.78 7.81 7.44   G2/3(IV)(we) 149 0
56 HD 220838 * 23 27 16.4821789104 -26 58 58.175202936   10.50 9.39     G6/8(III)w 64 0
57 HD 221170 Pe* 23 29 28.8087143040 +30 25 57.849303180 9.43 8.74 7.66     CEMP-r 301 0

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