2011ApJ...741....2L


Query : 2011ApJ...741....2L

2011ApJ...741....2L - Astrophys. J., 741, 2 (2011/November-1)

Constraint on the parameters of the inverse Compton scattering model for radio pulsars.

LV M., WANG H.G., LEE K.J., QIAO G.J. and XU R.X.

Abstract (from CDS):

The inverse Compton scattering (ICS) model can explain various pulse profile shapes and the diversity of the pulse profile evolution based on the mechanism where the radio emission is generated through ICS between secondary relativistic particles and radio waves from polar gap avalanches. In this paper, we study the parameter space of the ICS model for 15 pulsars that share the common pulse profile evolution phenomenon, where the pulse profiles are narrower at higher observing frequencies. Two key parameters, the initial Lorentz factor and the energy loss factor of secondary particles, are constrained using the least-squares fitting method, where we fit the theoretical curve of the "beam-frequency mapping" of the ICS model to the observed pulse widths at multiple frequencies. The uncertainty of the inclination and viewing angles are taken into account in the fitting process. It is found that the initial Lorentz factor is larger than 4000, and the energy loss factor is between 20 and 560. The Lorentz factor is consistent with the prediction of the inner vacuum gap model. Such high-energy loss factors suggest significant energy loss for secondary particles at altitudes of a few tens to hundreds of kilometers.

Abstract Copyright: ∼

Journal keyword(s): methods: data analysis - pulsars: general - radiation mechanisms: non-thermal

Simbad objects: 16

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Number of rows : 16
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 B0525+21 Psr 05 28 52.308 +22 00 01.00     14.30     ~ 370 0
3 PSR B0540+23 Psr 05 43 09.65 +23 29 06.1     14.40     ~ 278 0
4 PSR B0823+26 Psr 08 26 51.5068 +26 37 21.297           ~ 541 1
5 PSR B0919+06 Psr 09 22 13.85000 +06 38 19.0000           ~ 329 1
6 PSR B1039-19 Psr 10 41 36.19100 -19 42 13.7000           ~ 80 0
7 PSR B1133+16 Psr 11 36 03.09460 +15 51 15.9000           ~ 715 0
8 PSR B1702-19 Psr 17 05 36.09300 -19 06 39.2000           ~ 191 1
9 PSR B1706-16 Psr 17 09 26.45200 -16 40 59.2000           ~ 247 0
10 PSR B2016+28 Psr 20 18 03.8999255016 +28 39 54.940329468           ~ 374 0
11 PSR B2020+28 Psr 20 22 37.0671 +28 54 23.104           ~ 330 1
12 PSR B2021+51 Psr 20 22 49.8730 +51 54 50.233           ~ 288 1
13 PSR B2045-16 Psr 20 48 35.74000 -16 16 45.0000           ~ 344 0
14 PSR B2154+40 Psr 21 57 01.840 +40 17 45.89           ~ 155 0
15 PSR B2310+42 Psr 23 13 08.5976 +42 53 12.987           ~ 147 0
16 PSR B2319+60 Psr 23 21 55.213 +60 24 30.71     13.80     ~ 200 0

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