2016
DOI: 10.1051/0004-6361/201527152
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A multi-epoch spectroscopic study of the BAL quasar APM 08279+5255

Abstract: Context. The study of high-redshift bright quasars is crucial to gather information about the history of galaxy assembly and evolution. Variability analyses can provide useful data on the physics of quasar processes and their relation with the host galaxy. Aims. In this study, we aim to measure the black hole mass of the bright lensed BAL QSO APM 08279+5255 at z = 3.911 through reverberation mapping, and to update and extend the monitoring of its C IV absorption line variability. Methods. We perform the first … Show more

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Cited by 27 publications
(49 citation statements)
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References 82 publications
(196 reference statements)
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“…The red channel is shortpassed to reject a large fraction of Meinel rovibrational emissions which grow rapidly at wavelengths longer than ∼ 700 nm. Quasar spectra were taken from: QSO J0831+5245 [79], QSO B0350-073 (SDSS DR14, [52]), and QSO B0422+004 [80]. The skyglow spectrum is from Ref.…”
Section: Discussionmentioning
confidence: 99%
“…The red channel is shortpassed to reject a large fraction of Meinel rovibrational emissions which grow rapidly at wavelengths longer than ∼ 700 nm. Quasar spectra were taken from: QSO J0831+5245 [79], QSO B0350-073 (SDSS DR14, [52]), and QSO B0422+004 [80]. The skyglow spectrum is from Ref.…”
Section: Discussionmentioning
confidence: 99%
“…This technique combines the virial theorem with the BLR radius -luminosity relation (see e.g. Kaspi et al 2005;Bentz et al 2013;Saturni et al 2016), allowing an estimate of the black hole mass from measurements of the BLR line width and AGN luminosity. Different empirical relations have been calibrated in recent years (e.g.…”
Section: Nuclear Propertiesmentioning
confidence: 99%
“…Hence the black hole mass of APM 08279+5255 must be larger than 4 × 10 9 M⊙ even in the unlikely case that R is the same. While the upper limit of the magnification factor is estimated by the reverberation mapping (Saturni et al 2016), the lower limit is not. Here, we simply set a lower limit to be µ = 2 since no magnification µ = 1 seems to be unlikely for such a high luminosity object.…”
Section: Broadband Sed and Quasar Parametersmentioning
confidence: 99%