2020RAA....20..135W


Query : 2020RAA....20..135W

2020RAA....20..135W - Research in Astron. and astroph., 20, 135-135 (2020/September-0)

The formation of neutron star systems through accretion-induced collapse in white-dwarf binaries.

WANG B. and LIU D.

Abstract (from CDS):

The accretion-induced collapse (AIC) scenario was proposed 40 years ago as an evolutionary end state of oxygen-neonwhite dwarfs (ONeWDs), linking them to the formation of neutron star (NS) systems. However, there has been no direct detection of any AIC event so far, even though there exists a lot of indirect observational evidence. Meanwhile, the evolutionary pathways resulting in NS formation through AIC are still not thoroughly investigated. In this article, we review recent studies on the two classic progenitor models of AIC events, i.e., the single-degenerate model (including the ONe WD+MS/RG/He star channels and the COWD+He star channel) and the double-degeneratemodel (including the double COWD channel, the double ONe WD channel and the ONe WD+CO WD channel). Recent progress on these progenitor models is reviewed, including the evolutionary scenarios leading to AIC events, the initial parameter space for producing AIC events and the related objects (e.g., the pre-AIC systems and the post-AIC systems). For the single-degenerate model, the pre-AIC systems (i.e., the progenitor systems of AIC events) could potentially be identified as supersoft X-ray sources, symbiotics and cataclysmic variables (such as classical novae, recurrent novae, Ne novae and He novae) in the observations, whereas the post-AIC systems (i.e., NS systems) could potentially be identified as low-/intermediate-mass X-ray binaries, and the resulting low-/intermediate-mass binary pulsars, most notably millisecond pulsars. For the double-degeneratemodel, the pre-AIC systems are close double WDs with short orbital periods, whereas the post-AIC systems are single isolated NSs that may correspond to a specific kind of NS with peculiar properties. We also review the predicted rates of AIC events, the mass distribution of NSs produced via AIC and the gravitational wave (GW) signals from doubleWDs that are potential GW sources in the Galaxy in the context of future spacebased GW detectors, such as LISA, TianQin, Taiji, etc. Recent theoretical and observational constraints on the detection of AIC events are summarized. In order to confirm the existence of the AIC process, and resolve this long-term issue presented by current stellar evolution theories, more numerical simulations and observational identifications are required.

Abstract Copyright: © 2020 National Astronomical Observatories

Journal keyword(s): binaries: close - white dwarfs - supernovae: general - stars: neutron - stars: evolution

Simbad objects: 29

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Number of rows : 29
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 GD 687 HS* 01 10 18.6196714608 -34 00 25.710906636   13.89 14.08 14.39   sdBHe1 40 0
2 PSR J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 613 0
3 PSR J0348+0432 Psr 03 48 43.6363173480 +04 32 11.461921260           ~ 311 2
4 G 160-51 WD* 04 12 26.3267623464 -11 17 47.278628664   15.6 15.446     DA 34 0
5 FRB 20181119D rB 05 31 58.6980 +33 08 52.588           ~ 933 0
6 2MASS J05513444+4135297 WD* 05 51 34.4546350920 +41 35 29.954200380           DA 25 0
7 HD 49798 HXB 06 48 04.7001531360 -44 18 58.436036028 6.758 8.017 8.287 8.391 8.543 sdO6 339 0
8 V* V445 Pup No* 07 37 56.8797787992 -25 56 58.837610328       13.654 12.849 ~ 197 0
9 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
10 ASAS J075731+2017.6 LP* 07 57 31.1231195640 +20 17 34.777522608   12.71 10.62     M2.0III 16 0
11 SN 2018kzr SN* 08 28 53.460 +01 06 38.71           SNIc 39 0
12 VTC J095517+690813 Rad 09 55 17.460 +69 08 13.02           ~ 5 0
13 SBSS 1150+599 PN 11 53 24.7392231288 +59 39 57.050391708   17.5       O(H)III-V 78 0
14 V* AM CVn CV* 12 34 54.6231062664 +37 37 44.120620056   14.02 14.13 14.47   DBnnp 434 0
15 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
16 V* R CrB RC* 15 48 34.4154827352 +28 09 24.295852440 6.44 6.31 5.71 5.26 5.08 G0Iep 798 0
17 V* T CrB Sy* 15 59 30.1622265912 +25 55 12.613382940   11.516 10.247 9.70   M3IIIe_sh 810 0
18 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
19 SN 2018cow SN* 16 16 00.254 +22 16 05.10           SNIb 305 0
20 V* U Sco CV* 16 22 30.7791646104 -17 52 43.166822628           F8+K2 592 0
21 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
22 V* RS Oph Sy* 17 50 13.1591484960 -06 42 28.480729788   11.884 10.776 11.228   K5.5/M0IIIe 1163 0
23 V* V745 Sco Sy* 17 55 22.2260994408 -33 14 58.551839808     17.987   13.353 M2/M6IIIe 265 1
24 PSR J1802-2124 Psr 18 02 05.334393 -21 24 03.67600           ~ 101 1
25 V* V691 CrA LXB 18 25 46.8185061768 -37 06 18.529336656 14.30 15.20 15.1     ~ 461 0
26 PN M 4-12 PN 19 13 05.4493583551 +15 46 39.915114808   16.327 15.095 15.678   ~ 100 0
27 KPD 1930+2752 HS* 19 32 14.8088063952 +27 58 35.445679608 12.80 13.75 13.82     sdB 167 0
28 V* V458 Vul PN 19 54 24.6304743344 +20 52 52.134341488   17.76 15.96 17.9   ~ 135 0
29 MCT 2020-4234 WD* 20 23 59.5069330104 -42 24 25.846993944 13.73 14.70 14.89     DA1.6 59 0

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