2010MNRAS.401.1781D


Query : 2010MNRAS.401.1781D

2010MNRAS.401.1781D - Mon. Not. R. Astron. Soc., 401, 1781-1795 (2010/January-3)

The nature of pulsar radio emission.

DYKS J., RUDAK B. and DEMOREST P.

Abstract (from CDS):

High-quality averaged radio profiles of some pulsars exhibit double, highly symmetric features both in emission and in absorption. It is shown that both types of feature are produced by a split fan beam of extraordinary-mode curvature radiation that is emitted/absorbed by radially extended streams of magnetospheric plasma. With no emissivity in the plane of the stream, such a beam produces bifurcated emission components (BFCs) when our line of sight passes through the plane. An example of a double component created in this way is present in the averaged profile of the 5-ms pulsar J1012+5307. We show that the component can indeed be very well fitted by the textbook formula for the non-coherent beam of curvature radiation in the polarization state that is orthogonal to the plane of electron trajectory. The observed width of the BFC decreases with increasing frequency at a rate that confirms the curvature origin. Likewise, the double absorption features (double notches) are produced by the same beam of the extraordinary-mode curvature radiation, when it is eclipsed by thin plasma streams. The intrinsic property of curvature radiation to create bifurcated fan beams explains the double features in terms of a very natural geometry and implies the curvature origin of pulsar radio emission. Similarly, the `double conal' profiles of class D result from a cut through a wider stream with finite extent in magnetic azimuth. Therefore, their width reacts very slowly to changes of viewing geometry resulting from geodetic precession. The stream-cut interpretation implies a highly non-orthodox origin of both the famous S-swing of polarization angle and the low-frequency pulse broadening in D profiles. The azimuthal structure of polarization modes in the curvature radiation beam provides an explanation for the polarized `multiple imaging' and the edge depolarization of pulsar profiles.

Abstract Copyright: © 2009 The Authors. Journal compilation © 2009 RAS

Journal keyword(s): radiation mechanisms: non-thermal - pulsars: general - pulsars: individual: J1012+5307 - pulsars: individual: J0437-4715 - pulsars: individual: B0525+21 - pulsars: individual: B1913+16

CDS comments: In chap. 6.3.2 : PSR B0834+26 is a misprint for PSR B0834+06

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 - 2026
#notes
1 PSR B0301+19 Psr 03 04 33.115 +19 32 51.40           ~ 247 0
2 PSR B0329+54 Psr 03 32 59.3370698592 +54 34 45.028206408           ~ 690 1
3 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
4 PSR B0525+21 Psr 05 28 52.308 +22 00 01.00     14.30     ~ 370 0
5 PSR J0737-3039A Psr 07 37 51.24669 -30 39 40.6895           ~ 317 1
6 PSR J0737-3039 Psr 07 37 51.248 -30 39 40.83           ~ 445 1
7 PSR J0737-3039B Psr 07 37 51.24927 -30 39 40.7195           ~ 222 1
8 PSR B0751+32 Psr 07 54 40.688 +32 31 56.20           ~ 88 0
9 PSR B0834+06 Psr 08 37 05.64620 +06 10 15.8700           ~ 472 0
10 PSR B0950+08 Psr 09 53 09.31210 +07 55 36.9000           ~ 806 2
11 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
12 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 757 0
13 PSR B1133+16 Psr 11 36 03.09460 +15 51 15.9000           ~ 715 0
14 PSR J1141-6545 Psr 11 41 07.00060 -65 45 19.0500     25.08 24.38   ~ 207 1
15 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 497 1
16 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
17 PSR B1745-12 Psr 17 48 17.4310 -13 00 53.400           ~ 68 0
18 PSR J1906+0749 Psr 19 06 48.67 +07 46 28.6           ~ 172 1
19 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
20 PSR B1919+21 Psr 19 21 44.815 +21 53 02.25           ~ 411 0
21 PSR B1929+10 Psr 19 32 14.0570 +10 59 33.380           ~ 801 0
22 PSR B2020+28 Psr 20 22 37.0671 +28 54 23.104           ~ 330 1
23 PSR B2044+15 Psr 20 46 39.33600 +15 40 33.6000           ~ 109 0
24 PSR B2053+21 Psr 20 55 39.151 +22 09 27.22           ~ 55 0

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