2013ApJ...768..114W


Query : 2013ApJ...768..114W

2013ApJ...768..114W - Astrophys. J., 768, 114 (2013/May-2)

Modeling the frequency dependence of radio beams for cone-dominant pulsars.

WANG P.F., HAN J.L. and WANG C.

Abstract (from CDS):

Beam radii for cone-dominant pulsars follow a power-law relation with frequency, θ = (ν/ν0)^ k ^ + θ0, which has not been well explained in previous works. We study this frequency dependence of beam radius (FDB) for cone-dominant pulsars by using the curvature radiation mechanism. Considering various density and energy distributions of particles in the pulsar open field-line region, we numerically simulate the emission intensity distribution across emission height and rotation phase, get integrated profiles at different frequencies, and obtain the FDB curves. For the density model of a conal-like distribution, the simulated profiles always shrink to one component at high frequencies. In the density model with two separated density patches, the profiles generally have two distinct components, and the power-law indices k are found to be in the range from -0.1 to -2.5, consistent with observational results. Energy distributions of streaming particles have significant influence on the frequency-dependence behavior. Radial energy decay of particles is desired to get proper θ0 in models. We conclude that by using the curvature radiation mechanism, the observed FDB for the cone-dominant pulsars can only be explained by the emission model of particles in two density patches with a Gaussian energy distribution and a radial energy loss.

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Journal keyword(s): pulsars: general - radiation mechanisms: non-thermal - relativistic processes - stars: magnetic field

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 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 B0525+21 Psr 05 28 52.308 +22 00 01.00     14.30     ~ 370 0
4 PSR B1133+16 Psr 11 36 03.09460 +15 51 15.9000           ~ 715 0
5 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 497 1
6 PSR B2020+28 Psr 20 22 37.0671 +28 54 23.104           ~ 330 1
7 PSR B2045-16 Psr 20 48 35.74000 -16 16 45.0000           ~ 344 0

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