2024ApJ...973...35M


Query : 2024ApJ...973...35M

2024ApJ...973...35M - Astrophys. J., 973, 35 (2024/September-3)

Behavior of the Position and Ellipticity Angles at Polarization Mode Transitions in Pulsar Radio Emission.

McKINNON M.M.

Abstract (from CDS):

Polarization observations of radio pulsars show that abrupt transitions in the polarization vector's position angle can be accompanied by large excursions in the vector's ellipticity angle, suggesting the vector passes near the right or left circular pole of the Poincaré sphere. The behavior of the angles can be explained by a transition in dominance of the orthogonal polarization modes or a vector rotation caused by a change in the phase difference between the modes. Four polarization models are examined to quantify and understand the behavior of the angles at a mode transition: coherent polarization modes, partially coherent modes, incoherent modes with nonorthogonal polarization vectors, and incoherent orthogonal modes with an elliptically polarized emission component. In all four models, the trajectory of the mode transition on the Poincaré sphere follows the geodesic that connects the orientations of the mode polarization vectors. The results from the models can be similar, indicating that the interpretation of an observed transition within the context of a particular model is not necessarily unique. The polarization fraction of the emission and the average ellipticity angle depend upon the statistical character of the mode intensity fluctuations. The polarization fraction increases as the fluctuations increase. The excursion in ellipticity angle can be large when the mode intensities are quasi-stable and is suppressed when the intensity fluctuations are large.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Radio pulsars

Simbad objects: 6

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Number of rows : 6
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 J0134-2937 Psr 01 34 18.69390 -29 37 17.1570           ~ 60 0
2 PSR B0329+54 Psr 03 32 59.3370698592 +54 34 45.028206408           ~ 690 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 B1154-62 Psr 11 57 15.2070 -62 24 50.930           ~ 118 0
6 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 532 0

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