2022ApJ...935...27P


Query : 2022ApJ...935...27P

2022ApJ...935...27P - Astrophys. J., 935, 27 (2022/August-2)

Constraining Nucleosynthesis in Neutrino-driven Winds: Observations, Simulations, and Nuclear Physics.

PSALTIS A., ARCONES A., MONTES F., MOHR P., HANSEN C.J., JACOBI M. and SCHATZ H.

Abstract (from CDS):

A promising astrophysical site to produce the lighter heavy elements of the first r-process peak (Z = 38 - 47) is the moderately neutron-rich (0.4 < Ye < 0.5) neutrino-driven ejecta of explosive environments, such as core-collapse supernovae and neutron star mergers, where the weak r-process operates. This nucleosynthesis exhibits uncertainties from the absence of experimental data from (α, xn) reactions on neutron-rich nuclei, which are currently based on statistical model estimates. In this work, we report on a new study of the nuclear reaction impact using a Monte Carlo approach and improved (α, xn) rates based on the Atomki-V2 α optical model potential. We compare our results with observations from an up-to-date list of metal-poor stars with [Fe/H] < -1.5 to find conditions of the neutrino-driven wind where the lighter heavy elements can be synthesized. We identified a list of (α, xn) reaction rates that affect key elemental ratios in different astrophysical conditions. Our study aims to motivate more nuclear physics experiments on (α, xn) reactions using the current and new generation of radioactive beam facilities and also more observational studies of metal-poor stars.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Core-collapse supernovae - Nuclear astrophysics - Nucleosynthesis - R-process - Nuclear reaction cross sections

Simbad objects: 18

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Number of rows : 18
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 4306 SB* 00 45 27.1616035344 -09 32 39.785396712 9.80 9.75 9.02 8.75   G3/5w(A) 168 0
2 BPS CS 22942-0035 Pe* 01 03 57.4766862600 -23 52 45.274726956   15.17 14.56     ~ 13 0
3 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
4 BD+42 621 * 02 45 32.4541690680 +42 43 28.889531940   10.60 10.38     A2 13 0
5 HD 23798 Pe* 03 46 45.7220393712 -30 51 13.333194972   9.35 8.32     G8/K1(III)wF0/3 77 0
6 BD+06 648 Pe* 04 13 13.1126763288 +06 36 01.768985496   10.27 9.09 8.58   K0 117 0
7 HD 237846 Pe* 09 52 38.6827483320 +57 54 58.614479532   10.60 9.95     CEMP-no 105 0
8 HD 85773 Pe* 09 53 39.2426826504 -22 50 08.424342096   10.51 9.43     Gwl: 106 0
9 HD 88609 Pe* 10 14 28.9853799600 +53 33 39.342740796 9.930 9.540 8.620 7.78 7.15 G5IIIw 217 0
10 HD 107752 Pe* 12 22 52.7183284776 +11 36 25.486007148   10.79 10.1     KIIvw 83 0
11 HD 110184 SB* 12 40 14.0781612216 +08 31 38.057301300 10.20 9.45 8.27 8.52   KIIvw 153 0
12 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
13 HD 115444 Pe* 13 16 42.4590842616 +36 22 52.692135420   9.77 8.97 8.3 7.88 G9V 252 0
14 HD 122563 Pe* 14 02 31.8455084952 +09 41 09.944391876 7.47 7.10 6.19 5.37 4.79 G8:III:Fe-5 920 0
15 HD 140283 Pe* 15 43 03.0971190219 -10 56 00.595693188 7.508 7.711 7.212 6.63 8.21 F9VkA5mA1 985 0
16 BPS CS 22892-0052 Pe* 22 17 01.6558764360 -16 39 27.051026544   14.03 13.20 13.06 12.19 KIIvw 472 0
17 HE 2217-0706 Pe* 22 20 17.9990567088 -06 51 16.544943144     14.958   13.680 ~ 6 0
18 HD 221170 Pe* 23 29 28.8087143040 +30 25 57.849303180 9.43 8.74 7.66     CEMP-r 306 0

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