2021ApJ...909...21H


Query : 2021ApJ...909...21H

2021ApJ...909...21H - Astrophys. J., 909, 21-21 (2021/March-1)

Reconstructing masses of merging neutron stars from stellar r-process abundance signatures.

HOLMBECK E.M., FREBEL A., McLAUGHLIN G.C., SURMAN R., FERNANDEZ R., METZGER B.D., MUMPOWER M.R. and SPROUSE T.M.

Abstract (from CDS):

Neutron star mergers (NSMs) are promising astrophysical sites for the rapid neutron-capture ("r") process, but can their integrated yields explain the majority of heavy-element material in the Galaxy? One method to address this question implements a forward approach that propagates NSM rates and yields along with stellar formation rates and compares those results with observed chemical abundances of r-process-rich, metal-poor stars. In this work, we take the inverse approach by utilizing r-process-element abundance ratios of metal-poor stars as input to reconstruct the properties-especially the masses-of their neutron star (NS) binary progenitors. This novel analysis provides an independent avenue for studying the population of the original NS binary systems that merged and produced the r-process material now incorporated in Galactic metal-poor halo stars. We use ratios of elements typically associated with the limited-r-process and the actinide region to those in the lanthanide region (i.e., Zr/Dy and Th/Dy) to probe the NS masses of the progenitor merger. We find that NSMs can account for all r-process material in metal-poor stars that display r-process signatures, while simultaneously reproducing the present-day distribution of double-NS systems. Notably, with our model assumptions and the studied stellar sample, we postulate that the most r-process enhanced stars (the r-II stars) on their own would require progenitor NSMs of asymmetric systems that are distinctly different from present ones in the Galaxy. We also explore variations to the model and find that the predicted degree of asymmetry is most sensitive to the electron fraction of the remnant disk wind.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Nuclear astrophysics - Nucleosynthesis - R-process - Neutron stars - Chemically peculiar stars - Population II stars - Compact binary stars

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 BPS CS 29497-0004 Pe* 00 28 06.9155612016 -26 03 04.269055032   14.76 14.07 13.583 13.116 ~ 64 0
2 BPS CS 22953-0003 Pe* 01 02 15.8723379360 -61 43 45.836012208   14.43 13.75 13.339 12.886 KIIvw 78 0
3 HD 6268 Pe* 01 03 18.1716378504 -27 52 49.953768852   9.725 9.046 8.601   F/Gw 166 0
4 BD-16 251 RG* 01 29 31.1311443552 -16 00 45.495314460 12.527 12.427 11.642 11.189 10.713 CEMP 318 0
5 [KCB2015] Reti 4 RG* 03 35 23.8544722128 -54 04 07.586442660           ~ 29 0
6 NAME Reticulum II G 03 35 42.1 -54 02 57           ~ 375 0
7 BD-07 2674 Pe* 08 58 05.8480558056 -08 09 17.382965652   11.18 10.26     CEMP 11 0
8 TYC 3814-1598-1 Pe* 09 54 42.7718004504 +52 46 41.559838968   11.19 10.10     ~ 32 0
9 HE 1219-0312 Pe* 12 21 34.1430245160 -03 28 39.636260184     15.940   15.043 ~ 50 0
10 HD 108317 Pe* 12 26 36.8319587208 +05 18 09.023783400       7.7   G2IVm-5 182 0
11 HD 108577 Pe* 12 28 16.8614710944 +12 20 41.089853184   10.18 9.6 9.8   KIIvw 84 0
12 HD 110184 SB* 12 40 14.0781612216 +08 31 38.057301300 10.20 9.45 8.27 8.52   KIIvw 153 0
13 BD+10 2495 SB* 12 59 19.9306410576 +09 14 35.634594444   10.44 9.73     G0 82 0
14 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
15 HD 115444 Pe* 13 16 42.4590842616 +36 22 52.692135420   9.77 8.97 8.3 7.88 G9V 252 0
16 BD+08 2856 Pe* 14 23 58.1664038424 +08 01 33.333124908   10.90 10.08     KIIvw 70 0
17 TYC 7814-133-1 Pe* 14 32 53.3360210280 -41 25 49.477241028   11.76 11.08     ~ 15 0
18 2MASS J15095862+6716200 RB? 15 09 58.6103318448 +67 16 20.032584024   18.53 17.006   15.614 ~ 41 0
19 BPS CS 30306-0132 Pe* 15 14 18.9191634456 +07 27 02.680959780   13.62 12.73 12.421 11.948 ~ 43 0
20 TYC 6189-285-1 Pe* 15 38 30.8456260680 -18 04 24.290986440   11.725 10.864 10.58 10.529 CEMP 25 0
21 BD+17 3248 HB* 17 28 14.4690179544 +17 30 35.847574776   10.02 9.34     KIIvw 239 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 TYC 7440-1195-1 Pe* 20 05 06.6848152872 -30 57 44.589302460   12.478 11.246     ~ 14 0
24 UCAC2 31779418 Pe* 20 38 43.1848979784 -00 23 32.761814352   13.726 12.731 12.51 11.57 CEMP 34 0
25 BD-15 5781 Pe* 20 45 34.5446785080 -14 31 15.154963788   11.57 10.83     KIIvw 56 0
26 BPS CS 22892-0052 Pe* 22 17 01.6558764360 -16 39 27.051026544   14.03 13.20 13.06 12.19 KIIvw 472 0
27 BPS CS 29491-0069 Pe* 22 31 02.1859040712 -32 38 36.526573572   13.72 13.1 12.654 12.175 ~ 43 0
28 HE 2252-4225 Pe* 22 54 58.5673558608 -42 09 19.386504792     14.878   13.855 ~ 30 0
29 HD 221170 Pe* 23 29 28.8087143040 +30 25 57.849303180 9.43 8.74 7.66     CEMP-r 306 0
30 HE 2327-5642 Pe* 23 30 37.0896973176 -56 26 14.385030648   14.590 13.881 13.425 12.948 ~ 51 0
31 BPS CS 30315-0029 Pe* 23 34 26.6960486448 -26 42 14.003379828   14.56 13.64 13.092 12.518 ~ 32 0
32 NAME Tuc III G 23 56.6 -59 36           ~ 229 0
33 GRB 190425 GWE ~ ~           ~ 438 0

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