1999MNRAS.307..830G


Query : 1999MNRAS.307..830G

1999MNRAS.307..830G - Mon. Not. R. Astron. Soc., 307, 830-840 (1999/August-3)

Propagation effects on polarization of pulsar radio emission.

GANGADHARA R.T., LESCH H. and KRISHAN V.

Abstract (from CDS):

We consider the role of a propagation effect such as stimulated Raman scattering on the polarization of radio pulses. When an intense electromagnetic wave with frequency close to the plasma frequency interacts with the plasma in the pulsar magnetosphere, the incident wave undergoes stimulated Raman scattering. Using typical plasma and magnetic field parameters, we compute the growth rate and estimate the polarization properties of the scattered mode. Under some conditions, we find that the polarization properties of the scattered mode can become significantly different from those of the incident wave. The frequencies at which strong Raman scattering occurs in the outer parts of the magnetosphere fall into the observable radio band. In some pulsars, for example PSR B0628-28 and B1914+13, a large and symmetric type of circular polarization has been observed. We propose that such an unusual circular polarization is produced by the propagation effects.

Abstract Copyright: 1999, Royal Astronomical Society

Journal keyword(s): plasmas - polarization - radiative transfer - waves - stars: magnetic fields - pulsars: general

CDS comments: PSR B2048-78 misprint for PSR B2048-72

Simbad objects: 7

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Number of rows : 7
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 B0835-41 Psr 08 37 21.1943 -41 35 14.563     12.69     ~ 149 0
3 PSR B1240-64 Psr 12 43 17.2912183824 -64 23 23.082548820           ~ 119 0
4 PSR B1859+03 Psr 19 01 31.7700 +03 31 04.960           ~ 156 0
5 PSR B1914+13 Psr 19 16 58.67000 +13 12 50.0000           ~ 99 0
6 PSR B1933+16 Psr 19 35 47.7011639352 +16 16 40.034899524           ~ 328 1
7 PSR B2048-72 Psr 20 53 47.28000 -72 00 42.4800           ~ 60 0

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