2015MNRAS.454.2216D


Query : 2015MNRAS.454.2216D

2015MNRAS.454.2216D - Mon. Not. R. Astron. Soc., 454, 2216-2227 (2015/December-1)

The ratio of profile peak separations as a probe of pulsar radio-beam structure.

DYKS J. and PIERBATTISTA M.

Abstract (from CDS):

The known population of pulsars contains objects with four- and five-component profiles, for which the peak-to-peak separations between the inner and outer components can be measured. These Q- and M-type profiles can be interpreted as a result of sightline cut through a nested-cone beam, or through a set of azimuthal fan beams. We show that the ratio RW of the components' separations provides a useful measure of the beam shape, which is mostly independent of parameters that determine the beam scale and complicate interpretation of simpler profiles. In particular, the method does not depend on the emission altitude and the dipole tilt distribution. The different structures of the radio beam imply manifestly different statistical distributions of RW, with the conal model being several orders of magnitude less consistent with data than the fan-beam model. To bring the conal model into consistency with data, strong effects of observational selection need to be called for, with 80 per cent of Q and M profiles assumed to be undetected because of intrinsic blending effects. It is concluded that the statistical properties of Q and M profiles are more consistent with the fan-shaped beams, than with the traditional nested-cone geometry.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

Journal keyword(s): radiation mechanisms: non-thermal - pulsars: general - pulsars: individual: J0631+1036

Simbad objects: 30

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Number of rows : 30
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 B0329+54 Psr 03 32 59.3370698592 +54 34 45.028206408           ~ 690 1
2 PSR B0403-76 Psr 04 01 51.75000 -76 08 12.9500           ~ 57 0
3 PSR B0621-04 Psr 06 24 20.02500 -04 24 50.5600           ~ 78 0
4 PSR J0631+10 Psr 06 31 27.369 +10 37 05.63           ~ 152 0
5 PSR B0740-28 Psr 07 42 49.0730 -28 22 43.510           ~ 445 0
6 PSR J1034-3224 Psr 10 34 19.46000 -32 24 26.2000           ~ 57 0
7 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 757 0
8 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 497 1
9 PSR B1323-58 Psr 13 26 58.2170 -58 59 29.290           ~ 82 0
10 PSR B1323-62 Psr 13 27 17.1760 -62 22 45.460           ~ 100 0
11 PSR J1536-3602 Psr 15 36 17.382 -36 02 58.80           ~ 17 0
12 PSR J1651-7642 Psr 16 51 07.87 -76 42 39.5           ~ 12 0
13 PSR B1737+13 Psr 17 40 07.3455 +13 11 56.690           ~ 191 0
14 PSR B1738-08 Psr 17 41 22.5629 -08 40 31.711           ~ 98 0
15 PSR B1804-08 Psr 18 07 38.02590 -08 47 43.2800           ~ 139 0
16 PSR J1819+1305 Psr 18 19 56.226 +13 05 15.25           ~ 41 0
17 PSR B1821+05 Psr 18 23 30.9731 +05 50 24.310           ~ 136 0
18 PSR B1831-04 Psr 18 34 25.62100 -04 26 15.7000           ~ 103 0
19 PSR B1845-01 Psr 18 48 23.59600 -01 23 58.4800           ~ 154 0
20 PSR B1857-26 Psr 19 00 47.54200 -26 00 44.8000           ~ 195 1
21 PSR B1910+20 Psr 19 12 43.3391 +21 04 33.926           ~ 81 0
22 PSR B1918+19 Psr 19 21 03.799 +19 48 44.70           ~ 119 0
23 PSR B1919+21 Psr 19 21 44.815 +21 53 02.25           ~ 411 0
24 PSR B1929+10 Psr 19 32 14.0570 +10 59 33.380           ~ 801 0
25 PSR B1952+29 Psr 19 54 22.5107 +29 23 16.150           ~ 149 0
26 PSR B2003-08 Psr 20 06 16.36500 -08 07 02.1600           ~ 113 0
27 PSR B2028+22 Psr 20 30 40.446 +22 28 21.83           ~ 54 0
28 PSR B2210+29 Psr 22 12 23.3444 +29 33 05.411           ~ 54 0
29 PSR B2310+42 Psr 23 13 08.5976 +42 53 12.987           ~ 147 0
30 PSR B2319+60 Psr 23 21 55.213 +60 24 30.71     13.80     ~ 200 0

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