We investigate, for the first time at z â¼ 3, the clustering properties of 189 Type 1 and 157 Type 2 X-ray active galactic nuclei (AGNs) of moderate luminosity (ãL bolã=1045.3 erg s-1), with photometric or spectroscopic redshifts in the range 2.2 < z < 6.8. These samples are based on Chandra and XMM-Newton data in COSMOS. We find that Type 1 and Type 2 COSMOS AGNs at z â¼ 3 inhabit DMHs with typical mass of log Mh = 12.84-0.11+0.10 and 11.73-0.45+0.39 h -1 M â, respectively. This result requires a drop in the halo masses of Type 1 and 2 COSMOS AGNs at z â¼ 3 compared to z â² 2 XMM-COSMOS AGNs with similar luminosities. Additionally, we infer that unobscured COSMOS AGNs at z â¼ 3 reside in 10 times more massive halos compared to obscured COSMOS AGNs, at the 2.6Ï level. This result extends to z â¼ 3 the results found in COSMOS at z â² 2, and rules out the picture in which obscuration is purely an orientation effect. A model which assumes that the AGNs activity is triggered by major mergers is quite successful in predicting both the low halo mass of COSMOS AGNs and the typical mass of luminous SDSS quasars at z â¼ 3, with the latter inhabiting more massive halos respect to moderate luminosity AGNs. Alternatively we can argue, at least for Type 1 COSMOS AGNs, that they are possibly representative of an early phase of fast (i.e., Eddington limited) BH growth induced by cosmic cold flows or disk instabilities. Given the moderate luminosity, these new fast growing BHs have masses of â¼107-8 M â at z â¼ 3 which might evolve into â¼108.5-9 M â mass BHs at z=0. Following our clustering measurements, we argue that this fast BH growth at z â¼ 3 in AGNs with moderate luminosity occurs in DMHs with typical mass of â¼ 6Ã1012h -1 M â.
Clustering of moderate luminosity X-ray-selected type 1 and type 2 AGNS at z â¼ 3
Allevato, V.;Gilli, R.;Comastri, A.;Silverman, J.
2014
Abstract
We investigate, for the first time at z â¼ 3, the clustering properties of 189 Type 1 and 157 Type 2 X-ray active galactic nuclei (AGNs) of moderate luminosity (ãL bolã=1045.3 erg s-1), with photometric or spectroscopic redshifts in the range 2.2 < z < 6.8. These samples are based on Chandra and XMM-Newton data in COSMOS. We find that Type 1 and Type 2 COSMOS AGNs at z â¼ 3 inhabit DMHs with typical mass of log Mh = 12.84-0.11+0.10 and 11.73-0.45+0.39 h -1 M â, respectively. This result requires a drop in the halo masses of Type 1 and 2 COSMOS AGNs at z â¼ 3 compared to z â² 2 XMM-COSMOS AGNs with similar luminosities. Additionally, we infer that unobscured COSMOS AGNs at z â¼ 3 reside in 10 times more massive halos compared to obscured COSMOS AGNs, at the 2.6Ï level. This result extends to z â¼ 3 the results found in COSMOS at z â² 2, and rules out the picture in which obscuration is purely an orientation effect. A model which assumes that the AGNs activity is triggered by major mergers is quite successful in predicting both the low halo mass of COSMOS AGNs and the typical mass of luminous SDSS quasars at z â¼ 3, with the latter inhabiting more massive halos respect to moderate luminosity AGNs. Alternatively we can argue, at least for Type 1 COSMOS AGNs, that they are possibly representative of an early phase of fast (i.e., Eddington limited) BH growth induced by cosmic cold flows or disk instabilities. Given the moderate luminosity, these new fast growing BHs have masses of â¼107-8 M â at z â¼ 3 which might evolve into â¼108.5-9 M â mass BHs at z=0. Following our clustering measurements, we argue that this fast BH growth at z â¼ 3 in AGNs with moderate luminosity occurs in DMHs with typical mass of â¼ 6Ã1012h -1 M â.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.