2023ApJ...947...86B


Query : 2023ApJ...947...86B

2023ApJ...947...86B - Astrophys. J., 947, 86 (2023/April-3)

Estimating the Evolution of Sparks in the Partially Screened Gap of Pulsars from Subpulse Drifting.

BASU R., MITRA D. and MELIKIDZE G.I.

Abstract (from CDS):

A novel scheme has been developed to show that the observed phase behavior associated with subpulse drifting from two pulsars, J1034-3224 and J1720-2933, can be used to obtain the magnetic field configuration in the partially screened gap (PSG). The outflowing plasma along the open magnetic field line region of pulsars is generated as a result of spark discharges in an inner acceleration region (IAR) above the polar cap. The IAR has been modeled as a PSG with a steady supply of positively charged ions emitted from the heated polar cap surface dominated by strong non-dipolar magnetic fields. In a PSG the sparks are tightly packed and constrained to be present along the polar cap boundary. The sparks lag behind the rotation of the star during their lifetimes. As a result, the sparking pattern evolves along two different directions in a clockwise and counterclockwise manner around a stationary central spark and can be associated with the observed phenomenon of subpulse drifting. PSR J1034-3224 has four prominent components and exhibits bi-drifting where alternate components show the opposite sense of drifting, while PSR J1720-2933 has a single component profile and shows systematically coherent drift bands. We show that the differences in their drifting behavior can be directly linked to different natures of the non-dipolar surface magnetic field configurations.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Pulsars - Radio pulsars

Simbad objects: 2

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Number of rows : 2
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 J1034-3224 Psr 10 34 19.46000 -32 24 26.2000           ~ 57 0
2 PSR B1717-29 Psr 17 20 34.13100 -29 33 14.0000           ~ 80 0

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