2013MNRAS.431.2756J


Query : 2013MNRAS.431.2756J

2013MNRAS.431.2756J - Mon. Not. R. Astron. Soc., 431, 2756-2765 (2013/May-3)

An incomplete model of RRATs and of nulls mode changes and subpulses.

JONES P.B.

Abstract (from CDS):

A model for pulsars with polar-cap magnetic flux density \boldsymbol B antiparallel with spin \boldsymbol Ω is described. It recognizes the significance of two elementary processes, proton production in electromagnetic showers and photoelectric transitions in ions accelerated through the blackbody radiation field, which must be present at the polar cap in the \boldsymbol Ω⋅\boldsymbol B < 0 case, but not for pulsars of the opposite spin direction. The two populations are likely to be indistinguishable observationally until curvature radiation pair creation ceases to be possible. The model generates, and provides a physically realistic framework for, the polar-cap potential fluctuations and their time-scales that can produce mode changes and nulls. The rotating radio transients (RRATs) are then no more than an extreme case of the more commonly observed nulls. The model is also able to support the basic features of subpulse drift and to some extent the null-memory phenomenon that is associated with it. Unfortunately, it appears that the most important neutron-star parameter for quantitative predictive purposes is the whole-surface temperature Ts, a quantity which is not readily observable at the neutron-star ages concerned.

Abstract Copyright: © 2013 The Author Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): instabilities - plasma - stars: neutron - pulsars: 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 PSR J0420-5022 Psr 04 20 01.95 -50 22 48.1           ~ 5 0
2 PSR B0656+14 Psr 06 59 48.18800 +14 14 19.2000   24.85 24.90     ~ 943 1
3 PSR B0809+74 Psr 08 14 59.500 +74 29 05.70           ~ 425 0
4 PSR J0815+09 Psr 08 15 08.78 +09 39 50.7           ~ 42 0
5 PSR B0823+26 Psr 08 26 51.5068 +26 37 21.297           ~ 541 1
6 PSR B1112+50 Psr 11 15 38.400 +50 30 12.29           ~ 154 0
7 PSR J1554-5209 Psr 15 54 27.15 -52 09 38.3           ~ 12 0
8 PSR J1832+0029 Psr 18 32 50.7 +00 29 27           ~ 59 0
9 PSR J1840-1417 Psr 18 41.0 -14 18           ~ 22 0
10 PSR J1841-0500 Psr 18 41 18.14 -05 00 19.5           ~ 54 0
11 PSR B1839-04 Psr 18 42 26.4642900744 -04 00 00.516985452           ~ 81 0
12 PSR J1933+2421 Psr 19 33 37.83 +24 36 39.6           ~ 157 0
13 PSR B1944+17 Psr 19 46 53.044 +18 05 41.24           ~ 252 0
14 PSR B2315+21 Psr 23 17 57.8419 +21 49 48.019           ~ 119 0
15 PSR B2327-20 Psr 23 30 26.98600 -20 05 29.7500           ~ 133 0

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