2005ApJ...634..534S


Query : 2005ApJ...634..534S

2005ApJ...634..534S - Astrophys. J., 634, 534-541 (2005/November-3)

Supernova neutrino effects on r-process nucleosynthesis in black hole formation.

SASAQUI T., KAJINO T. and BALANTEKIN A.B.

Abstract (from CDS):

Very massive stars with mass ≥8 M☉culminate their evolution by supernova explosions, which are presumed to be the most viable candidates for the astrophysical sites of r-process nucleosynthesis. If the models for the supernova r-process are correct, then the results of nucleosynthesis could also put a significant constraint on the remnants of supernova explosions, i.e., a neutron star or black hole. In the case of very massive core collapse for a progenitor mass 20-40 M☉, a remnant stellar black hole is thought to be formed. Intense neutrino flux from the neutronized core and the neutrinosphere might suddenly cease during the Kelvin-Helmholtz cooling phase because of the black hole formation. It is important and interesting to explore the observable consequences of such a neutrino flux truncation. It has recently been argued in the literature that even the neutrino mass can be determined from the time delay of the deformed neutrino energy spectrum after the cessation of neutrino ejection (neutrino cutoff effect). Here we study the expected theoretical response of the r-process nucleosynthesis to the neutrino cutoff effect in order to look for another independent signature of this phenomenon. We found a sensitive response of the r-process yield if the neutrino cutoff occurs after the critical time when the expanding materials in the neutrino-driven wind drop out of nuclear statistical equilibrium (NSE). The r-process nucleosynthesis yields drastically change if the cutoff occurs during the r-process, having maximal effect on the change in abundance of 232Th and 235,238U. There is a large probability of finding this effect in elemental abundances of r-process-enhanced metal-deficient halo stars whose chemical composition is presumed to be affected by Population III supernovae in the early Galaxy. Using this result, connected with future detection of the time variation of the SN neutrino spectrum, we are able to identify when the black hole formation occurs in the course of SN collapse.

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Journal keyword(s): Black Hole Physics - Neutrinos - Nuclear Reactions, Nucleosynthesis, Abundances - Stars: Supernovae: General

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 BPS CS 29497-0004 Pe* 00 28 06.9155612016 -26 03 04.269055032   14.76 14.07 13.583 13.116 ~ 64 0
2 HD 6268 Pe* 01 03 18.1716378504 -27 52 49.953768852   9.725 9.046 8.601   F/Gw 166 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 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
5 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
6 HD 108577 Pe* 12 28 16.8614710944 +12 20 41.089853184   10.18 9.6 9.8   KIIvw 84 0
7 HD 110184 SB* 12 40 14.0781612216 +08 31 38.057301300 10.20 9.45 8.27 8.52   KIIvw 153 0
8 HD 115444 Pe* 13 16 42.4590842616 +36 22 52.692135420   9.77 8.97 8.3 7.88 G9V 252 0
9 BD+08 2856 Pe* 14 23 58.1664038424 +08 01 33.333124908   10.90 10.08     KIIvw 70 0
10 BPS CS 30306-0132 Pe* 15 14 18.9191634456 +07 27 02.680959780   13.62 12.73 12.421 11.948 ~ 43 0
11 NGC 6341 7018 RG* 17 16 37.4894075472 +43 06 15.600437640   13.47 12.18     ~ 77 0
12 M 92 GlC 17 17 07.39 +43 08 09.4     6.52     ~ 2240 0
13 HD 186478 SB* 19 45 14.1409752672 -17 29 27.071239056   10.116 9.302 8.527 7.961 K2III 166 0
14 NGC 7078 341 RG* 21 29 54.9258244080 +12 13 22.484816292   13.72 12.54   11.22 ~ 61 0
15 NGC 7078 462 RG* 21 29 56.6627934840 +12 09 46.341312228   14.45 12.90     ~ 40 0
16 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0
17 NGC 7078 583 RG* 21 29 58.5643129152 +12 09 21.382732260   14.26 12.83     ~ 34 0
18 BPS CS 22892-0052 Pe* 22 17 01.6558764360 -16 39 27.051026544   14.03 13.20 13.06 12.19 KIIvw 472 0

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