2010ApJ...710.1017Z


Query : 2010ApJ...710.1017Z

2010ApJ...710.1017Z - Astrophys. J., 710, 1017-1031 (2010/February-3)

X-ray radiation mechanisms and beaming effect of hot spots and knots in active galactic nuclear jets.

ZHANG J., BAI J.M., CHEN L. and LIANG E.

Abstract (from CDS):

The observed radio-optical-X-ray spectral energy distributions (SEDs) of 22 hot spots and 45 knots in the jets of 35 active galactic nuclei are complied from the literature and modeled with single-zone lepton models. It is found that the observed luminosities at 5 GHz (L_5 GHz_) and at 1 keV (L_1 keV_) are tightly correlated, and the two kinds of sources can be roughly separated with a division of L_1 keV_= L_5 GHz_. Our SED fits show that the mechanisms of the X-rays are diverse. While the X-ray emission of a small fraction of the sources is a simple extrapolation of the synchrotron radiation for the radio-to-optical emission, an inverse Compton (IC) scattering component is necessary to model the X-rays for most of the sources. Considering the sources at rest (the Doppler factor δ = 1), the synchrotron-self-Compton (SSC) scattering would dominate the IC process. This model can interpret the X-rays of some hot spots with a magnetic field strength (B ^δ = 1^ssc) being consistent with the equipartition magnetic field (B ^δ = 1^eq) in 1 order of magnitude, but an unreasonably low B ^δ = 1^ssc is required to model the X-rays for all knots. Measuring the deviation between B ^δ = 1^ssc and B ^δ = 1^eqwith ratio RB≡ B ^δ = 1^eq/B ^δ = 1^ssc, we find that RB is greater than 1 and it is tightly anti-correlated with ratio RL≡ L_1 keV/L 5 GHz_ for both the knots and the hot spots. We propose that the deviation may be due to the neglect of the relativistic bulk motion for these sources. Considering this effect, the IC/cosmic microwave background (CMB) component would dominate the IC process. We show that the IC/CMB model well explains the X-ray emission for most sources under the equipartition condition. Although the derived beaming factor (δ) and co-moving equipartition magnetic field (B'eq) of some hot spots are comparable to the knots, the δ values of the hot spots tend to be smaller and their B'eq values tend to be larger than that of the knots, favoring the idea that the hot spots are jet termination and knots are a part of a well-collimated jet. Both {B_eq^{′}} and δ are tentatively correlated with RL. Corrected by the beaming effect, the L'_5 GHz–L'1 keV_ relations for the two kinds of sources are even tighter than the observed ones. These facts suggest that, under the equipartition condition, the observational differences of the X-rays from the knots and hot spots may be mainly due to the differences on the Doppler boosting effect and the co-moving magnetic field of the two kinds of sources. Our IC scattering models predict a prominent GeV-TeV component in the SEDs for some sources, which are detectable with H.E.S.S. and Fermi/LAT.

Abstract Copyright:

Journal keyword(s): galaxies: jets - magnetic fields - radiation mechanisms: non-thermal - X-rays: galaxies

Simbad objects: 35

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Number of rows : 35
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 3C 15 BiC 00 37 04.1107321824 -01 09 08.407668996   15.34       ~ 223 1
2 NGC 383 rG 01 07 24.9647814840 +32 24 45.132586200   13.6 12.14     ~ 778 3
3 2C 94 Sy2 01 08 52.8701830824 +13 20 14.262799812   15.19       ~ 477 2
4 UGC 1841 Sy1 02 23 11.41124925 +42 59 31.3853324   15.71 14.81     ~ 561 2
5 PKS 0405-123 Sy1 04 07 48.4309841856 -12 11 36.659928408   15.09 14.86 14.7   ~ 510 1
6 Mrk 1506 Sy1 04 33 11.0956735296 +05 21 15.619461552   15.72 15.05 10.08   ~ 2000 2
7 NAME Pic A Sy1 05 19 49.7229323856 -45 46 43.852662732   15.73 15.77 14.85   ~ 666 1
8 ESO 362-21 Sy1 05 22 57.98464178 -36 27 30.8512953   15.26 14.62 14.48   ~ 834 2
9 QSO J0635-7516 Bla 06 35 46.5079301472 -75 16 16.816418256   15.96 15.75 15.82   ~ 589 1
10 Z 150-14 Sy2 08 40 02.336 +29 49 02.73   20.00 19.62     ~ 193 1
11 ICRF J084047.5+131223 Sy1 08 40 47.58842599 +13 12 23.5637506   18.58 18.15 17.622   ~ 434 1
12 3C 228 rG 09 50 10.7 +14 19 58   21       ~ 166 2
13 4C 12.37 QSO 10 42 44.6052783816 +12 03 31.263917976   18.03 17.77     ~ 440 2
14 NAME Crt A Sy1 11 39 10.7025556152 -13 50 43.639196064   16.38 16.17 16.4   ~ 272 1
15 ICRF J113957.0+654749 Sy1 11 39 57.0254367168 +65 47 49.483232880   16.50 16.32     ~ 518 1
16 LB 2136 Sy1 11 53 24.46663994 +49 31 08.8301372   17.94 17.66     ~ 499 1
17 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 5802 1
18 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7196 3
19 4C -02.55 QSO 12 32 00.0159535440 -02 24 04.793069304   17.41 17.06 16.4   ~ 432 1
20 ICRF J124357.6+162253 Sy1 12 43 57.6491122968 +16 22 53.395049244   19.23 19.00     ~ 313 1
21 2C 1066 SyG 12 56 57.5 +47 20 20   22.0       ~ 281 0
22 [OKM2018] SWIFT J1357.0+1929 Sy1 13 57 04.4366598768 +19 19 07.371837768   16.33 16.03 15.3   ~ 455 2
23 3C 295 Sy2 14 11 20.6 +52 12 09   22.34 20.80 18.54   ~ 979 5
24 QSO B1421-490 QSO 14 24 32.24039 -49 13 49.7513   18.5       ~ 76 1
25 ICRF J144302.7+520137 Sy1 14 43 02.76069031 +52 01 37.2985156   18.96 18.29     ~ 300 3
26 NAME Her B Sy1 16 42 58.80997043 +39 48 36.9939552   16.81 16.59 16.84   ~ 1725 2
27 3C 346.0 BLL 16 43 48.605 +17 15 49.43   17.2       ~ 264 0
28 3C 351.0 Sy1 17 04 41.3742408840 +60 44 30.520617000   15.65 15.40 15.30   ~ 757 1
29 3C 371 BLL 18 06 50.6802916920 +69 49 28.109609256   14.77 14.22 11.39   ~ 856 2
30 ICRF J184208.9+794617 Sy1 18 42 08.9904975672 +79 46 17.127835104   16.06 15.38     ~ 1316 0
31 4C 73.18 BLL 19 27 48.4947009120 +73 58 01.572558816     16.06 15.11   ~ 534 2
32 3C 403.0 Sy2 19 52 15.7996999344 +02 30 24.238200816   15.42 16.5     ~ 338 1
33 NAME Cyg A Sy2 19 59 28.35656837 +40 44 02.0972325   16.22 15.10     ~ 2368 2
34 4C 04.77 BLL 22 04 17.6521146096 +04 40 02.027503020   16.20 15.2 10.2   ~ 206 2
35 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 2848 2

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