1986
DOI: 10.1086/163973
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Relativistic beaming and quasar emission lines

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Cited by 277 publications
(310 citation statements)
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“…In bin B1 we are probably considering a subsample of FRII that show narrower profile than the majority of the population. If the FWHM is affected by orientation as expected (e.g., Wills & Browne 1986;Sulentic et al 2003;Rokaki et al 2003;Runnoe et al 2013;Zamfir et al 2008), we are observing sources that tend to be seen at a smaller viewing angle than the general FRII population. If the wind flow follows a bent path over the accretion disk (Elvis 2000) or if the flow is constrained closer to the disk plane, the absence of a blueshift might therefore be related more to orientation than to full suppression of disk winds in RL sources by the pressure of a cocoon associated with the relativistic ejections (Norman & Miley 1984).…”
Section: Radio Quiet and Radio Loudmentioning
confidence: 54%
“…In bin B1 we are probably considering a subsample of FRII that show narrower profile than the majority of the population. If the FWHM is affected by orientation as expected (e.g., Wills & Browne 1986;Sulentic et al 2003;Rokaki et al 2003;Runnoe et al 2013;Zamfir et al 2008), we are observing sources that tend to be seen at a smaller viewing angle than the general FRII population. If the wind flow follows a bent path over the accretion disk (Elvis 2000) or if the flow is constrained closer to the disk plane, the absence of a blueshift might therefore be related more to orientation than to full suppression of disk winds in RL sources by the pressure of a cocoon associated with the relativistic ejections (Norman & Miley 1984).…”
Section: Radio Quiet and Radio Loudmentioning
confidence: 54%
“…Note that this BH mass is a factor of 3 lower than the lowest BH mass of the radio-loud quasars in the PG sample and the accretion rate is much higher than predicted by the relation between L=L Edd and the radio loudness of Ho (2002). However, if the broad-line region is flat, the small line width can be due to inclination effects (Wills & Browne 1986). In this case, the BH mass could be severely underestimated.…”
Section: Discussionmentioning
confidence: 76%
“…We again see a preferred thick disk geometry in 3C 120 and the inclination angle of the system is well-constrained at θ i = 17.6 +5.4 −3.3 relative to the observer. 3C 120 is of particular interest because there are external indicators of inclination angle in the system obtained from radio jet orientation, which has shown to be linked to the BLR rotation axis (e.g., Wills & Browne 1986;Marscher et al 2002;Jorstad et al 2005;Agudo et al 2012). Marscher et al (2002) first determined the upper limit on the jet viewing angle to be 20 degrees, and further work by Jorstad et al (2005) measured a viewing angle of 20.5 ± 1.8 degrees.…”
Section: Mrk 1501mentioning
confidence: 99%