Abstract:We present VLT/SINFONI observations of 35 quasars at 2.1 < z < 3.2, the majority of which were selected from the Clusters Around Radio-Loud AGN (CARLA) survey. CARLA quasars have large C iv-based black hole masses (M BH > 10 9 M ) and powerful radio emission (P 500 MHz > 27.5 W Hz −1 ). We estimate Hα-based M BH , finding a scatter of 0.35 dex compared to C iv. We evaluate several recipes for correcting C iv-based masses, which reduce the scatter to 0.24 dex. The radio power of the radio-loud quasars is at mos… Show more
“…Their optical spectra can be of both type 1 and type 2 AGN. I Zw 1 is however not a very extreme object: the most extreme accretors show spectra similar to the one of PHL 1092 [86]. Note that the equivalent width is increased, as shown in Figures 11 and A2 but, since there is a corresponding increase in Hβ, the R FeII is left unaffected.…”
The issue of the difference between optical and UV properties of radio-quiet and radio-loud (relativistically “jetted”) active galactic nuclei (AGN) is a long standing one, related to the fundamental question of why a minority of powerful AGN possess strong radio emission due to relativistic ejections. This paper examines a particular aspect: the singly-ionized iron emission in the spectral range 4400–5600 Å, where the prominent HI Hβ and [Oiii]λλ4959,5007 lines are also observed. We present a detailed comparison of the relative intensity of Feii multiplets in the spectral types of the quasar main sequence where most jetted sources are found, and afterwards discuss radio-loud narrow-line Seyfert 1 (NLSy1) nuclei with γ-ray detection and with prominent Feii emission. An Feii template based on I Zw 1 provides an accurate representation of the optical Feii emission for RQ and, with some caveats, also for RL sources. CLOUDY photoionization simulations indicate that the observed spectral energy distribution can account for the modest Feii emission observed in composite radio-loud spectra. However, spectral energy differences alone cannot account for the stronger Feii emission observed in radio-quiet sources, for similar physical parameters. As for RL NLSy1s, they do not seem to behave like other RL sources, likely because of their different physical properties, that could be ultimately associated with a higher Eddington ratio. active galactic nuclei; optical spectroscopy; ionized gas; broad line region
“…Their optical spectra can be of both type 1 and type 2 AGN. I Zw 1 is however not a very extreme object: the most extreme accretors show spectra similar to the one of PHL 1092 [86]. Note that the equivalent width is increased, as shown in Figures 11 and A2 but, since there is a corresponding increase in Hβ, the R FeII is left unaffected.…”
The issue of the difference between optical and UV properties of radio-quiet and radio-loud (relativistically “jetted”) active galactic nuclei (AGN) is a long standing one, related to the fundamental question of why a minority of powerful AGN possess strong radio emission due to relativistic ejections. This paper examines a particular aspect: the singly-ionized iron emission in the spectral range 4400–5600 Å, where the prominent HI Hβ and [Oiii]λλ4959,5007 lines are also observed. We present a detailed comparison of the relative intensity of Feii multiplets in the spectral types of the quasar main sequence where most jetted sources are found, and afterwards discuss radio-loud narrow-line Seyfert 1 (NLSy1) nuclei with γ-ray detection and with prominent Feii emission. An Feii template based on I Zw 1 provides an accurate representation of the optical Feii emission for RQ and, with some caveats, also for RL sources. CLOUDY photoionization simulations indicate that the observed spectral energy distribution can account for the modest Feii emission observed in composite radio-loud spectra. However, spectral energy differences alone cannot account for the stronger Feii emission observed in radio-quiet sources, for similar physical parameters. As for RL NLSy1s, they do not seem to behave like other RL sources, likely because of their different physical properties, that could be ultimately associated with a higher Eddington ratio. active galactic nuclei; optical spectroscopy; ionized gas; broad line region
“…The slightly longer cosmic times available to quasars at z 6 make it significantly "easier" to go from a 100 M seed to a SMBH of a few times 10 9 M compared to the quasars at z 7 (e.g., Bañados et al 2018b;Marinello et al 2020;Pacucci & Loeb 2021). For example, assuming constant accretion with Eddington ratios of 0.8-1.3 onto a seed formed at z f = 20 − 10 is able to produce a SMBH like that in J0836 by z = 5.82, while the quasar ULAS J1342+0928 at z = 7.54 requires the existence of a >1000 M seed as early as z = 45 assuming standard Eddington rate accretion (Bañados et al 2018b).…”
Observations of luminous quasars and their supermassive black holes at z 6 suggest that they formed at dense matter peaks in the early universe. However, few studies have found definitive evidence that the quasars lie at cosmic density peaks, in clear contrast with theory predictions. Here we present new evidence that the radio-loud quasar SDSS J0836+0054 at z = 5.8 could be part of a surprisingly rich structure of galaxies. This conclusion is reached by combining a number of findings previously reported in the literature. Bosman et al. ( 2020) obtained the redshifts of three companion galaxies, confirming an overdensity of i 775 -dropouts found by Zheng et al. (2006). By comparing this structure with those found near other quasars and large overdense regions in the field at z ∼ 6 − 7, we show that the SDSS J0836+0054 field is among the densest structures known at these redshifts. One of the spectroscopic companions is a very massive star-forming galaxy (log 10 (M /M ) = 10.3 +0.3 −0.2 ) based on its unambiguous detection in a Spitzer 3.6 µm image. This suggests that the quasar field hosts not one, but at least two rare, massive dark matter halos (log 10 (M h /M ) 12), corresponding to a galaxy overdensity of at least 20. We discuss the properties of the young radio source. We conclude that the environment of SDSS J0836+0054 resembles, at least qualitatively, the type of conditions that may have spurred the direct collapse of a massive black hole seed according to recent theory.
“…For z>4, M BH estimates historically rely on the CIVλ1549 high-ionization line, and the highest-z sources appear almost always high-accretors [666,667]. The source of concern is that high-ionization lines such as CIVλ1549 are subject to a considerable broadening and blueshifts associated with outflow motions already at low redshift [668,669,670,671]. Overestimates of the virial broadening by a factor as large as 5 -10 [672, 673, 674, 675] for SMBHs at high z may pose a spurious challenge to concordance cosmology [676] and lead to erroneous inferences on the properties of the seed BHs believed to be fledgling precursors of massive BHs.…”
Section: Scaling Laws For Agn Black Hole Mass Estimatesmentioning
We review the properties of the established Scaling Relations (SRs) of galaxies and active galactic nuclei (AGN), focusing on their origin and expected evolution back in time, providing a short history of the most important progresses obtained up to now and discussing the possible future studies. We also try to connect the observed SRs with the physical mechanisms behind them, examining to what extent current models reproduce the observational data.The emerging picture clarifies the complexity intrinsic to the galaxy formation and evolution process as well as the basic uncertainties still affecting our knowledge of the AGN phenomenon. At the same time, however, it suggests that the detailed analysis of the SRs can profitably contribute to our understanding of galaxies and AGN.
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