{We present an investigation into how well the properties of the accretion flow on to a supermassive black hole may be coupled to those of the overlying hot corona. To do so, we specifically measure the characteristic spectral index, {$\Gamma$}, of a power-law energy distribution, over an energy range of 2-10 keV, for X-ray selected, broad-lined radio-quiet active galactic nuclei (AGN) up to z {\tilde} 2 in Cosmic Evolution Survey (COSMOS) and Extended Chandra Deep Field South (E-CDF-S). We test the previously reported dependence between {$\Gamma$} and black hole mass, full width at half-maximum (FWHM) and Eddington ratio using a sample of AGN covering a broad range in these parameters based on both the Mg II and H{$\alpha$} emission lines with the later afforded by recent near-infrared spectroscopic observations using Subaru/Fibre Multi Object Spectrograph. We calculate the Eddington ratios, {$\lambda$}$_{Edd}$, for sources where a bolometric luminosity (L$_{Bol}$) has been presented in the literature, based on spectral energy distribution fitting, or, for sources where these data do not exist, we calculate L$_{Bol}$ using a bolometric correction to the X-ray luminosity, derived from a relationship between the bolometric correction and L$_{X}$/L$_{3000}$. From a sample of 69 X-ray bright sources ({\gt}250 counts), where {$\Gamma$} can be measured with greatest precision, with an estimate of L$_{Bol}$, we find a statistically significant correlation between {$\Gamma$} and {$\lambda$}$_{Edd}$, which is highly significant with a chance probability of 6.59{\times} 10$^{-8}$. A statistically significant correlation between {$\Gamma$} and the FWHM of the optical lines is confirmed, but at lower significance than with {$\lambda$}$_{Edd}$ indicating that {$\lambda$}$_{Edd}$ is the key parameter driving conditions in the corona. Linear regression analysis reveals that {$\Gamma$} = (0.32 {\plusmn} 0.05) log$_{10}${$\lambda$}$_{Edd}$ + (2.27 {\plusmn} 0.06) and {$\Gamma$} = (-0.69 {\plusmn} 0.11) log$_{10}$(FWHM/km s$^{-1}$) + (4.44 {\plusmn} 0.42). Our results on {$\Gamma$}-{$\lambda$}$_{Edd}$ are in very good agreement with previous results. While the {$\Gamma$}-{$\lambda$}$_{Edd}$ relationship means that X-ray spectroscopy may be used to estimate black hole accretion rate, considerable dispersion in the correlation does not make this viable for single sources, however could be valuable for large X-ray spectral samples, such as those to be produced by eROSITA. }

A statistical relation between the X-ray spectral index and Eddington ratio of active galactic nuclei in deep surveys / M. Brightman;J. D. Silverman;V. Mainieri;Y. Ueda;M. Schramm;K. Matsuoka;T. Nagao;C. Steinhardt;J. Kartaltepe;D. B. Sanders;E. Treister;O. Shemmer;W. N. Brandt;M. Brusa;A. Comastri;L. C. Ho;G. Lanzuisi;E. Lusso;K. Nandra;M. Salvato;G. Zamorani;M. Akiyama;D. M. Alexander;A. Bongiorno;P. Capak;F. Civano;A. . Moro;A. Doi;M. Elvis;G. Hasinger;E. S. Laird;D. Masters;M. Mignoli;K. Ohta;K. Schawinski;Y. Taniguchi. - In: MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY. - ISSN 0035-8711. - STAMPA. - 433:(2013), pp. 2485-2496. [10.1093/mnras/stt920]

A statistical relation between the X-ray spectral index and Eddington ratio of active galactic nuclei in deep surveys

BRUSA, MARCELLA;LANZUISI, GIORGIO;
2013

Abstract

{We present an investigation into how well the properties of the accretion flow on to a supermassive black hole may be coupled to those of the overlying hot corona. To do so, we specifically measure the characteristic spectral index, {$\Gamma$}, of a power-law energy distribution, over an energy range of 2-10 keV, for X-ray selected, broad-lined radio-quiet active galactic nuclei (AGN) up to z {\tilde} 2 in Cosmic Evolution Survey (COSMOS) and Extended Chandra Deep Field South (E-CDF-S). We test the previously reported dependence between {$\Gamma$} and black hole mass, full width at half-maximum (FWHM) and Eddington ratio using a sample of AGN covering a broad range in these parameters based on both the Mg II and H{$\alpha$} emission lines with the later afforded by recent near-infrared spectroscopic observations using Subaru/Fibre Multi Object Spectrograph. We calculate the Eddington ratios, {$\lambda$}$_{Edd}$, for sources where a bolometric luminosity (L$_{Bol}$) has been presented in the literature, based on spectral energy distribution fitting, or, for sources where these data do not exist, we calculate L$_{Bol}$ using a bolometric correction to the X-ray luminosity, derived from a relationship between the bolometric correction and L$_{X}$/L$_{3000}$. From a sample of 69 X-ray bright sources ({\gt}250 counts), where {$\Gamma$} can be measured with greatest precision, with an estimate of L$_{Bol}$, we find a statistically significant correlation between {$\Gamma$} and {$\lambda$}$_{Edd}$, which is highly significant with a chance probability of 6.59{\times} 10$^{-8}$. A statistically significant correlation between {$\Gamma$} and the FWHM of the optical lines is confirmed, but at lower significance than with {$\lambda$}$_{Edd}$ indicating that {$\lambda$}$_{Edd}$ is the key parameter driving conditions in the corona. Linear regression analysis reveals that {$\Gamma$} = (0.32 {\plusmn} 0.05) log$_{10}${$\lambda$}$_{Edd}$ + (2.27 {\plusmn} 0.06) and {$\Gamma$} = (-0.69 {\plusmn} 0.11) log$_{10}$(FWHM/km s$^{-1}$) + (4.44 {\plusmn} 0.42). Our results on {$\Gamma$}-{$\lambda$}$_{Edd}$ are in very good agreement with previous results. While the {$\Gamma$}-{$\lambda$}$_{Edd}$ relationship means that X-ray spectroscopy may be used to estimate black hole accretion rate, considerable dispersion in the correlation does not make this viable for single sources, however could be valuable for large X-ray spectral samples, such as those to be produced by eROSITA. }
2013
A statistical relation between the X-ray spectral index and Eddington ratio of active galactic nuclei in deep surveys / M. Brightman;J. D. Silverman;V. Mainieri;Y. Ueda;M. Schramm;K. Matsuoka;T. Nagao;C. Steinhardt;J. Kartaltepe;D. B. Sanders;E. Treister;O. Shemmer;W. N. Brandt;M. Brusa;A. Comastri;L. C. Ho;G. Lanzuisi;E. Lusso;K. Nandra;M. Salvato;G. Zamorani;M. Akiyama;D. M. Alexander;A. Bongiorno;P. Capak;F. Civano;A. . Moro;A. Doi;M. Elvis;G. Hasinger;E. S. Laird;D. Masters;M. Mignoli;K. Ohta;K. Schawinski;Y. Taniguchi. - In: MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY. - ISSN 0035-8711. - STAMPA. - 433:(2013), pp. 2485-2496. [10.1093/mnras/stt920]
M. Brightman;J. D. Silverman;V. Mainieri;Y. Ueda;M. Schramm;K. Matsuoka;T. Nagao;C. Steinhardt;J. Kartaltepe;D. B. Sanders;E. Treister;O. Shemmer;W. N. Brandt;M. Brusa;A. Comastri;L. C. Ho;G. Lanzuisi;E. Lusso;K. Nandra;M. Salvato;G. Zamorani;M. Akiyama;D. M. Alexander;A. Bongiorno;P. Capak;F. Civano;A. . Moro;A. Doi;M. Elvis;G. Hasinger;E. S. Laird;D. Masters;M. Mignoli;K. Ohta;K. Schawinski;Y. Taniguchi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/229686
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