2012MNRAS.425.1558D


Query : 2012MNRAS.425.1558D

2012MNRAS.425.1558D - Mon. Not. R. Astron. Soc., 425, 1558-1566 (2012/September-2)

Magnetars from magnetized cores.

DASS N.D.H. and SONI V.

Abstract (from CDS):

We consider a model in which magnetars arise from a high baryon density, magnetized core which forms when they are born. In this framework, magnetars are distinguished from pulsars by their higher masses and central density. In this model for magnetars, as core densities exceed a threshold, the strong interaction can induce a phase transition to a ground state that aligns nucleon magnetic moments. The core magnetic field is initially shielded by the ambient high-conductivity plasma. With time the shielding currents dissipate transporting the core field out, first to the crust and then breaking through the crust to the surface of the star. Recent observations provide support for this model which accounts for several properties of magnetars and also enables us to identify new magnetars.

Abstract Copyright: 2012 The Authors Monthly Notices of the Royal Astronomical Society 2012 RAS

Journal keyword(s): equation of state - magnetic fields - stars: neutron

CDS comments: In Table 1 PSR 0154-61 is a misprint for PSR 0154+61.

Simbad objects: 11

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Number of rows : 11
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 PSR B0154+61 Psr 01 57 49.9434 +62 12 26.648           ~ 127 0
2 PSR B0355+54 Psr 03 58 53.7165 +54 13 13.727           ~ 465 1
3 NAME Vela Pulsar Psr 08 35 20.65525 -45 10 35.1545     15.10     ~ 2446 1
4 PSR J1119-6127 Psr 11 19 14.30 -61 27 49.5           ~ 439 1
5 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
6 PSR J1718-3718 Psr 17 18 10.16 -37 18 53.8           ~ 73 0
7 PSR B1811-17.7 Psr 18 14 43.10 -17 44 48.0           ~ 77 0
8 PSR J1846-0258 Psr 18 46 24.75 -02 58 29.6           ~ 388 2
9 PSR J1847-0130 Psr 18 47 35.2 -01 30 46           ~ 44 0
10 PSR J1852+0040 Psr 18 52 38.5963516169 +00 40 20.164383034           ~ 98 1
11 GBS 1900+14 gB 19 07 13 +09 19.6           ~ 906 0

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