2019ApJ...878..148R


Query : 2019ApJ...878..148R

2019ApJ...878..148R - Astrophys. J., 878, 148-148 (2019/June-3)

Radio emission from pulsars due to relativistic plasma.

ROY T. and GANGADHARA R.T.

Abstract (from CDS):

Pulsar radio emission is not well understood because of a lack of knowledge about the emission geometry and the plasma process involved. We develop a mechanism for pulsar radio emission that takes into account the detailed viewing geometry of pulsars and the dipolar magnetic field configuration. Using a suitably chosen geometry and plasma parameters, we derive analytical expressions for the Stokes parameters of the radiation field in the frame centered on the neutron star. We have simulated pulse profiles based on our analytical formulation. It seems that we can explain the enhanced radiation and most of the diverse polarization properties of radio pulsars. We have estimated the brightness temperature, which seems to agree with the observations. The polarization angle predicted by the model is in good agreement with the rotating vector model.

Abstract Copyright: © 2019. The American Astronomical Society.

Journal keyword(s): acceleration of particles - polarization - pulsars: general - radiation mechanisms: non-thermal

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 B0138+59 Psr 01 41 39.938 +60 09 32.30     12.85     ~ 120 0
2 PSR B0628-28 Psr 06 30 49.35000 -28 34 42.1000           ~ 313 1
3 PSR B0809+74 Psr 08 14 59.500 +74 29 05.70           ~ 425 0
4 PSR B0818-13 Psr 08 20 26.40700 -13 50 56.3200           ~ 229 0
5 PSR B0834+06 Psr 08 37 05.64620 +06 10 15.8700           ~ 472 0
6 PSR B1133+16 Psr 11 36 03.09460 +15 51 15.9000           ~ 715 0
7 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 497 1
8 PSR B2044+15 Psr 20 46 39.33600 +15 40 33.6000           ~ 109 0
9 PSR B2111+46 Psr 21 13 24.3295 +46 44 08.844           ~ 226 1
10 PSR B2154+40 Psr 21 57 01.840 +40 17 45.89           ~ 155 0

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