2002MNRAS.333..943W


Query : 2002MNRAS.333..943W

2002MNRAS.333..943W - Mon. Not. R. Astron. Soc., 333, 943-951 (2002/July-2)

The spin evolution of nascent neutron stars.

WATTS A.L. and ANDERSSON N.

Abstract (from CDS):

The loss of angular momentum owing to unstable r-modes in hot young neutron stars has been proposed as a mechanism for achieving the spin rates inferred for young pulsars. One factor that could have a significant effect on the action of the r-mode instability is fallback of supernova remnant material. The associated accretion torque could potentially counteract any gravitational-wave-induced spin-down, and accretion heating could affect the viscous damping rates and hence the instability. We discuss the effects of various external agents on the r-mode instability scenario within a simple model of supernova fallback on to a hot young magnetized neutron star. We find that the outcome depends strongly on the strength of the magnetic field of the star. Our model is capable of generating spin rates for young neutron stars that accord well with initial spin rates inferred from pulsar observations. The combined action of r-mode instability and fallback appears to cause the spin rates of neutron stars born with very different spin rates to converge, on a time-scale of approximately 1 year. The results suggest that stars with magnetic fields ≤1013 G could emit a detectable gravitational wave signal for perhaps several years after the supernova event. Stars with higher fields (magnetars) are unlikely to emit a detectable gravitational wave signal via the r-mode instability. The model also suggests that the r-mode instability could be extremely effective in preventing young neutron stars from going dynamically unstable to the bar-mode.

Abstract Copyright: 2002 Blackwell Science Ltd

Journal keyword(s): accretion, accretion discs - gravitation - magnetic fields - waves - stars: neutron

Simbad objects: 24

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Number of rows : 24
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 SNR G130.7+03.1 SNR 02 05 37.0 +64 49 42           ~ 620 4
2 PSR J0205+6449 Psr 02 05 37.92 +64 49 42.8           ~ 248 1
3 M 1 SNR 05 34 30.9 +22 00 53           ~ 6192 1
4 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5259 0
5 PSR B0540-69 Psr 05 40 11.2000490438 -69 19 54.198559829           ~ 904 3
6 NAME Vela Pulsar Psr 08 35 20.65525 -45 10 35.1545     15.10     ~ 2315 1
7 PSR J1016-58 Psr 10 16 21.266 -58 57 11.70           ~ 118 3
8 SNR G284.3-01.8 Rad 10 18.3 -59 00           ~ 115 2
9 PSR J1119-6127 Psr 11 19 14.30 -61 27 49.5           ~ 403 1
10 SNR G292.2-00.5 SNR 11 19.3 -61 28           ~ 90 1
11 PSR J1124-5916 Psr 11 24 39.1 -59 16 20           ~ 163 1
12 SNR G292.0+01.8 SNR 11 24 59 -59 19.1           ~ 327 1
13 3A 1510-590 Psr 15 13 17.000 -59 04 54.00           ~ 403 3
14 PSR B1509-58 Psr 15 13 55.52 -59 08 08.8     13.06     ~ 844 1
15 PSR B1757-24 Psr 18 01 00.016 -24 51 27.50           ~ 244 1
16 NAME Duck Redux Rad 18 02 10.000 -24 54 00.00           ~ 179 3
17 SNR G011.2-00.3 SNR 18 11 28.9 -19 25 29           ~ 286 1
18 PSR J1811-1926 Psr 18 11 29.15 -19 25 25.4           ~ 126 1
19 SNR G029.7-00.2 SNR 18 46 22.8 -02 59 47           ~ 350 2
20 PSR J1846-0258 Psr 18 46 24.94 -02 58 30.1           ~ 347 2
21 PSR B1853+01 Psr 18 56 10.65 +01 13 21.3           ~ 199 1
22 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 964 2
23 SNR G068.8+02.6 SNR 19 52 55 +32 54.2           ~ 352 1
24 PSR B1951+32 Psr 19 52 58.181 +32 52 40.98           ~ 596 2

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