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The relationship between X-ray emission and accretion in X-ray selected AGNs

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Mem. S.A.It. Vol. 84, 717

SAIt 2013 c Memorie

della

The relationship between X-ray emission and accretion in X-ray selected AGNs

R. Fanali 1,2 , A. Caccianiga 1 , P. Severgnini 1 , R. Della Ceca 1 , M. Dotti 2 , and E. Marchese 2,1

1

INAF - Osservatorio Astronomico di Brera, via Brera 28, I-20121 Milano, Italy

2

Universit`a degli Studi di Milano Bicocca, Piazza Della Scienza 3, I-20126 Milano, Italy e-mail: rossella.fanali@brera.inaf.it

Abstract. We study the link between the X-ray emission in radio-quiet AGNs and the accretion rate on the central Supermassive Black-Hole (SMBH) using a well-defined and statistically complete sample of 70 type1 AGNs extracted from the XMM-Newton Bright Serendipitous survey (XBS). To this end, we search and quantify the statistical correlations between the main parameters that characterize the X-ray emission (i. e. the X-ray spectral slope and the X-ray loudness), and the accretion rate, both absolute ( ˙ M) and relative to the Eddington limit (Eddington ratio, λ). Here, we summarize and discuss the main statistical correlations found and their possible implications on current disk-corona models.

Key words. active galaxies, X-ray properties, accretion rate

1. Introduction

It is now accepted that the engine of AGNs is powered by the accretion of matter onto the SMBH, placed in the center of the host galaxy:

the matter is heated (∼ 10

6

K) through vis- cous and magnetic process and forms an ac- cretion disk around the SMBH emitting in the UV-optical region. A fraction of energy is also emitted in the X-ray band with a spectrum that can be represented, at a zeroth order, by a power-law from 0.1 to 100 keV. It is believed that X-rays are produced in a hot corona (∼ 10

8

K) reprocessing the primary UV-optical emis- sion of the disk via inverse-Compton mech- anism (Haardt & Maraschi 1991). The main properties of X-ray emission change signifi-

Send offprint requests to: R. Fanali

cantly from source to source. Recent results

suggest that the differences can be partly re-

lated to the value of accretion rate or to the

black-hole mass (Grupe et al. 2010, Risaliti

et al. 2009, Vasudevan & Fabian 2009). The

aim of this work is to establish the actual link

between X-ray properties and the parameters

that quantify the accretion rate by analyzing a

well defined sample of 70 type1 AGNs selected

from the XMM-Newton Bright Serendipitous

survey (XBS). In this work we study the spec-

tral index Γ between 0.5 and 10 keV and the

bolometric correction K

bol

, defined as the ratio

between bolometric luminosity and 2 − 10 keV

luminosity. Γ gives direct information about

the energy distribution of the electrons in the

corona, while K

bol

quantifies the relative im-

portance between disk and corona. The ap-

proach followed is to search for statistically

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718 R. Fanali et al.: X-ray emission and accretion rate

Fig. 1. Theoretical spectral energy distribu- tions that represent two extreme cases of accre- tion: λ ∼ 10

−3

(upper panel) and λ ∼ 1 (lower panel). See text for more details.

significant correlations between these param- eters and the value of accretion rate, absolute ( ˙ M) and normalized to Eddington limit (λ), presented in (Caccianiga et al. 2013).

2. Results

We find that Γ depends significantly on λ while the dependence on ˙ M is weak. By using partial correlation we demonstrate that the observed correlations are not induced by redshift. We find a similar Γ − λ correlation also using the hard 2 − 10 keV spectral index. Therefore the observed correlation is directly linked to the primary component of the X-ray emission and not due to secondary spectral component (e.g.

soft excess). We also find a correlation between K

bol

and λ while, again, the dependece on ˙ M is weak. We represent graphically the results of the Γ − λ and K

bol

− λ correlations by showing the theoretical SEDs in two extreme cases of low and high Eddington ratios (Fig. 1): these SEDs were built using a Shakura & Sunyaev disk model plus a power-law in the range be- tween 0.01 and 100 keV with a cut-off at 0.1 keV. The values of Γ and K

bol

are taken from our fits of the Γ − λ and K

bol

− λ correlations.

To simplify the comparison, we assume the same disk emission normalization in both cases. The comparison of the two SEDs sug- gests that the variation of K

bol

could be en- tirely attributed to the variation of Γ. We also test this idea by using the partial correlation analysis and we conclude that the correlations observed in this work can be in principle ex- plained by the Γ − λ correlation alone. This re- sult suggests a speculative interpretation based on the electron cooling of corona: for high val- ues of λ, a large number of photons comes from the accretion disk and cools corona electrons rapidly, thus poducing steep X-ray spectra and high values of K

bol

. For low λ, less photons are available and this makes electron cooling inef- ficient, thus producing flat X-ray spectra and low values of K

bol

.

Full details are reported in Fanali et al.

(2013).

Acknowledgements. We acknowledge Francesco Haardt for the useful discussions and ASI (grant n.

I/008/06/0) for financial support.

References

Caccianiga et al., 2013, A&A, 549, A119.

Fanali et al. 2013, MNRAS, 1400.

Grupe et al. 2010, ApJ, 187, 64.

Haardt & Maraschi, 1991, ApJ, 380, L51.

Risaliti et al., 2009, ApJ, 700, L6

Vasudevan & Fabian, 2009, MNRAS, 392,

1124.

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