2011MNRAS.414..759J


Query : 2011MNRAS.414..759J

2011MNRAS.414..759J - Mon. Not. R. Astron. Soc., 414, 759-769 (2011/June-2)

Instabilities, nulls and subpulse drift in radio pulsars.

JONES P.B.

Abstract (from CDS):

This paper continues a previous study of neutron stars with positive polar-cap corotational charge density in which free emission of ions maintains the surface electric field boundary condition E⋅B= 0. The composition of the accelerated plasma on any subset of open magnetic flux lines above the polar cap alternates between two states: protons or positrons and ions, of which the proton state cannot support electron–positron pair creation at higher altitudes. The two states coexist at any instant of time above different moving elements of area on the polar cap and provide a physically consistent basis for a description of pulse nulls and subpulse drift. In the latter case, it is shown that the band separation P3 is determined not by the E{x}B drift velocity, as is generally assumed, but by the diffusion time for protons produced in reverse-electron showers to reach the region of the atmosphere from which they are accelerated. An initial comparison is made with the survey of subpulse drift published by Weltevrede et al.

Abstract Copyright: 2011 The Author Monthly Notices of the Royal Astronomical Society2011 RAS

Journal keyword(s): instabilities - plasmas - stars: neutron - pulsars: general

Simbad objects: 10

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Number of rows : 10
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 B0628-28 Psr 06 30 49.35000 -28 34 42.1000           ~ 313 1
2 PSR B0656+14 Psr 06 59 48.18800 +14 14 19.2000   24.85 24.90     ~ 943 1
3 PSR B0826-34 Psr 08 28 16.6 -34 17 07           ~ 167 0
4 PSR B0834+06 Psr 08 37 05.64620 +06 10 15.8700           ~ 472 0
5 PSR B0943+10 Psr 09 46 07.31 +09 51 57.3           ~ 364 1
6 PSR B0950+08 Psr 09 53 09.31210 +07 55 36.9000           ~ 806 2
7 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 757 0
8 PSR B1133+16 Psr 11 36 03.09460 +15 51 15.9000           ~ 715 0
9 PSR B1929+10 Psr 19 32 14.0570 +10 59 33.380           ~ 801 0
10 PSR J1933+2421 Psr 19 33 37.83 +24 36 39.6           ~ 157 0

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