2011ApJ...731L...5M


Query : 2011ApJ...731L...5M

2011ApJ...731L...5M - Astrophys. J., 731, L5 (2011/April-2)

The angular momenta of neutron stars and black holes as a window on supernovae.

MILLER J.M., MILLER M.C. and REYNOLDS C.S.

Abstract (from CDS):

It is now clear that a subset of supernovae displays evidence for jets and is observed as gamma-ray bursts (GRBs). The angular momentum distribution of massive stellar endpoints provides a rare means of constraining the nature of the central engine in core-collapse explosions. Unlike supermassive black holes, the spin of stellar-mass black holes in X-ray binary systems is little affected by accretion and accurately reflects the spin set at birth. A modest number of stellar-mass black hole angular momenta have now been measured using two independent X-ray spectroscopic techniques. In contrast, rotation-powered pulsars spin down over time, via magnetic braking, but a modest number of natal spin periods have now been estimated. For both canonical and extreme neutron star parameters, statistical tests strongly suggest that the angular momentum distributions of black holes and neutron stars are markedly different. Within the context of prevalent models for core-collapse supernovae, the angular momentum distributions are consistent with black holes typically being produced in GRB-like supernovae with jets and with neutron stars typically being produced in supernovae with too little angular momentum to produce jets via magnetohydrodynamic processes. It is possible that neutron stars are with high spin initially and rapidly spun down shortly after the supernova event, but the available mechanisms may be inconsistent with some observed pulsar properties.

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Journal keyword(s): accretion, accretion disks - black hole physics - gamma-ray burst: general - stars: evolution - stars: neutron - supernovae: general

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 NAME M33 X-7 HXB 01 33 34.13 +30 32 11.3 17.50 18.80 18.70     O 187 2
2 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5 14.924   O8(f)p 700 0
3 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544           K3V-K7V 1144 0
4 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760         15.624 ~ 532 1
5 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
6 [GHJ2008] 3 HXB 16 50 00.980 -49 57 43.60           K4V 422 0
7 XTE J1652-453 XB* 16 52 20.330 -45 20 39.99           ~ 56 1
8 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
9 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
10 SAX J1711.6-3808 XB* 17 11 37.1 -38 07 06           ~ 45 0
11 XTE J1752-223 LXB 17 52 15.090 -22 20 32.36           ~ 229 0
12 2MAXI J1753-013 LXB 17 53 28.2898766424 -01 27 06.256555272 15.30 16.73 16.46 16.15 15.64 ~ 384 0
13 [KRL2007b] 353 HXB 19 08 53.080 +09 23 04.84     15.80     ~ 125 0
14 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
15 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0

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