2013ApJ...763..134F


Query : 2013ApJ...763..134F

2013ApJ...763..134F - Astrophys. J., 763, 134 (2013/February-1)

Compton dominance and the blazar sequence.

FINKE J.D.

Abstract (from CDS):

Does the "blazar sequence" exist, or is it a result of a selection effect, due to the difficulty in measuring the redshifts of blazars with both high synchrotron peak frequencies ( ≳ 1015 Hz) and luminosities ( ≳ 1046 erg/s)? We explore this question with a sample of blazars from the second catalog of active galactic nuclei from the Fermi Large Area Telescope. The Compton dominance, the ratio of the peak of the Compton to the synchrotron peak luminosities, is essentially a redshift-independent quantity and thus crucial to answering this question. We find that a correlation exists between Compton dominance and the peak frequency of the synchrotron component for all blazars in the sample, including ones with unknown redshift. We then construct a simple model to explain the blazar properties in our sample, where the difference between sources is due to only the magnetic field of the blazar jet emitting region, the external radiation field energy density, and the jet angle to the line of sight, with the magnetic field strength and external energy density being correlated. This model can reproduce the trends of the blazars in the sample and predicts that blazars may be discovered in the future with high synchrotron peak frequencies and luminosities. At the same time the simple model reproduces the lack of high-synchrotron-peaked blazars with high Compton dominances ( ≳ 1).

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Journal keyword(s): BL Lacertae objects: general - galaxies: active - gamma rays: galaxies - quasars: general - radiation mechanisms: non-thermal

Simbad objects: 10

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Number of rows : 10
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 RX J0059.2-0150 Bla 00 59 16.9278313536 -01 50 17.664890784   17.5       ~ 51 1
2 PMN J0630-2406 BLL 06 30 59.5217586120 -24 06 46.204083144 16.48 16.22 16.04 16   ~ 97 1
3 2FGL J0912.5+2758 BLL 09 12 11.2102430208 +27 59 27.880270260   19.38 18.91 19.1   ~ 47 0
4 7C 1015+3557 Bla 10 18 10.98810472 +35 42 39.4409041   18.62 18.07 17.65   ~ 212 1
5 RX J1023.6+3001 BLL 10 23 39.7366248552 +30 00 57.751171200   19.31 18.77 18.2   ~ 58 0
6 Z 184-50 BLL 11 04 27.3140835504 +38 12 31.798495872   13.50 12.90 8.31   ~ 2841 1
7 CRATES J115404+602229 Rad 11 54 04.53 +60 22 20.8           ~ 1 0
8 6C 115124+603931 Bla 11 54 04.5364398144 +60 22 20.823835944       19.6   ~ 69 1
9 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3205 2
10 9C J1521+4336 Bla 15 21 49.61387806 +43 36 39.2681695   19.30 18.95 18.09   ~ 129 1

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