2000ApJ...545..100H


Query : 2000ApJ...545..100H

2000ApJ...545..100H - Astrophys. J., 545, 100-106 (2000/December-2)

Pair plasma dominance in the parsec-scale relativistic jet of 3C 345.

HIROTANI K., IGUCHI S., KIMURA M. and WAJIMA K.

Abstract (from CDS):

We investigate whether a parsec-scale jet of 3C 345 is dominated by a normal plasma or an electron-positron plasma. We present a general condition that a jet component becomes optically thick for synchrotron self-absorption by extending the method originally developed by Reynolds and coworkers. The general condition gives a lower limit of the electron number density, with the aid of the surface brightness condition, which enables us to compute the magnetic field density. Comparing the lower limit with another independent constraint for the electron density that is deduced from the kinetic luminosity, we can distinguish the matter content. We apply the procedure to the five components of 3C 345 (C2, C3, C4, C5, and C7) of which angular diameters and radio fluxes at the peak frequencies were obtainable from literature. Evaluating the representative values of Doppler beaming factors by their equipartition values, we find that all the five components are likely dominated by an electron-positron plasma. The conclusion does not depend on the lower cutoff energy of the power-law distribution of radiating particles.

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Journal keyword(s): Galaxies: Active - quasars: individual (3C 345) - Radio Continuum: Galaxies

Simbad objects: 8

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Number of rows : 8
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 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7815 3
2 3C 279C3 Rad 12 56 11.0 -05 47 21           ~ 11 0
3 3C 279C4 Rad 12 56 11.0 -05 47 21           ~ 25 0
4 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3205 2
5 3C 345 Bla 16 42 58.80997043 +39 48 36.9939552   16.81 16.59 16.84   ~ 1808 3
6 3C 345C5 Rad ~ ~           ~ 24 0
7 3C 345C3 Rad ~ ~           ~ 19 0
8 3C 345C2 Rad ~ ~           ~ 18 0

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