2015MNRAS.451.2123T


Query : 2015MNRAS.451.2123T

2015MNRAS.451.2123T - Mon. Not. R. Astron. Soc., 451, 2123-2144 (2015/August-1)

Ultra-stripped supernovae: progenitors and fate.

TAURIS T.M., LANGER N. and PODSIADLOWSKI P.

Abstract (from CDS):

The explosion of ultra-stripped stars in close binaries can lead to ejecta masses <0.1M☉ and may explain some of the recent discoveries of weak and fast optical transients. In Tauris et al., it was demonstrated that helium star companions to neutron stars (NSs) may experience mass transfer and evolve into naked ∼ 1.5M☉ metal cores, barely above the Chandrasekhar mass limit. Here, we elaborate on this work and present a systematic investigation of the progenitor evolution leading to ultra-stripped supernovae (SNe). In particular, we examine the binary parameter space leading to electron-capture (EC SNe) and iron core-collapse SNe (Fe CCSNe), respectively, and determine the amount of helium ejected with applications to their observational classification as Type Ib or Type Ic. We mainly evolve systems where the SN progenitors are helium star donors of initial mass MHe = 2.5-3.5M☉ in tight binaries with orbital periods of Porb = 0.06-2.0d, and hosting an accreting NS, but we also discuss the evolution of wider systems and of both more massive and lighter - as well as single - helium stars. In some cases, we are able to follow the evolution until the onset of silicon burning, just a few days prior to the SN explosion. We find that ultra-stripped SNe are possible for both EC SNe and Fe CCSNe. EC SNe only occur for MHe = 2.60-2.95M☉ depending on Porb. The general outcome, however, is an Fe CCSN above this mass interval and an ONeMg or CO white dwarf for smaller masses. For the exploding stars, the amount of helium ejected is correlated with Porb - the tightest systems even having donors being stripped down to envelopes of less than 0.01M☉. We estimate the rise time of ultra-stripped SNe to be in the range 12h-8d, and light-curve decay times between 1 and 50 d. A number of fitting formulae for our models are provided with applications to population synthesis. Ultra-stripped SNe may produce NSs in the mass range 1.10-1.80M☉ and are highly relevant for LIGO/VIRGO since most (possibly all) merging double NS systems have evolved through this phase. Finally, we discuss the low-velocity kicks which might be imparted on these resulting NSs at birth.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

Journal keyword(s): binaries: close - stars: mass-loss - stars: neutron - supernovae: general - white dwarfs - X-rays: binaries

Errata: erratum vol. 467, p. 2145 (2017)

Simbad objects: 15

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Number of rows : 15
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 SN 2005E SN* 02 39 14.34 +01 05 55.0     16.8     SNIb/c 128 1
2 Z 524-49 GiG 03 05 43.3485597816 +36 47 10.359553848   13.5       ~ 47 0
3 SN 2005ek SN* 03 05 48.96 +36 46 10.6     17.5     SNIc: 76 1
4 PSR J0348+0432 Psr 03 48 43.6363173480 +04 32 11.461921260           ~ 311 2
5 SN 2010X SN* 04 48 27.90 +73 28 14.8           SNIc 85 1
6 PSR J0453+1559 Psr 04 53 45.41372 +15 59 21.3000           ~ 92 0
7 PSR J0737-3039 Psr 07 37 51.248 -30 39 40.83           ~ 445 1
8 PSR J1141-6545 Psr 11 41 07.00060 -65 45 19.0500     25.08 24.38   ~ 207 1
9 SN 1994I SN* 13 29 54.072 +47 11 30.50     12.9     SNIc 645 1
10 PSR J1753-2240 Psr 17 53 39.847 -22 40 42.00           ~ 53 1
11 PSR B1809-17.6 Psr 18 11 55.034 -17 36 37.70           ~ 114 1
12 PSR J1930-1852 Psr 19 30 29.7156 -18 51 46.270           ~ 54 0
13 PSR J1952+2630 Psr 19 52.6 +26 30           ~ 44 0
14 V* V1521 Cyg HXB 20 32 25.78 +40 57 27.9           WN4/5-6/7 2035 2
15 PSR J2305+4707 Psr 23 05 55.842 +47 07 45.32           ~ 227 1

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