Compton-Thick (CT) active galactic nuclei (AGN) are a key ingredient of cosmic X-ray background (CXB) synthesis models, but are still an elusive component of the AGN population beyond the local universe. Multiwavelength surveys are the only way to find them at z > ∼ 0.1, and a deep X-ray coverage is crucial in order to clearly identify them among star-forming galaxies. As an example, the deep and wide COSMOS survey allowed us to select a total of 34 CT sources. This number is computed from the 64 nominal CT candidates, each counted for its NH probability distribution function. For each of these sources, rich multiwavelength information is available, which is used to confirm their obscured nature by comparing the expected AGN luminosity from spectral energy distribution fitting with the absorption-corrected X-ray luminosity. While Chandra is more efficient, for a given exposure, in detecting CT candidates in current surveys (by a factor ∼ 2), deep XMM–Newton pointings of bright sources are vital to fully characterize their properties, for example, NH distribution above 1025 cm− 2, reflection intensity, etc., all crucial parameters of CXB models. Since luminous CT AGN at high redshift are extremely rare, the future of CT studies at high redshift will have to rely on the large-area surveys currently under way, such as XMM-XXL and Stripe82, and will then require dedicated follow-up with XMM–Newton, while waiting for the advent of the ESA mission Athena.

X-ray selection of Compton-Thick AGN at high redshift

LANZUISI, GIORGIO
Writing – Original Draft Preparation
2017

Abstract

Compton-Thick (CT) active galactic nuclei (AGN) are a key ingredient of cosmic X-ray background (CXB) synthesis models, but are still an elusive component of the AGN population beyond the local universe. Multiwavelength surveys are the only way to find them at z > ∼ 0.1, and a deep X-ray coverage is crucial in order to clearly identify them among star-forming galaxies. As an example, the deep and wide COSMOS survey allowed us to select a total of 34 CT sources. This number is computed from the 64 nominal CT candidates, each counted for its NH probability distribution function. For each of these sources, rich multiwavelength information is available, which is used to confirm their obscured nature by comparing the expected AGN luminosity from spectral energy distribution fitting with the absorption-corrected X-ray luminosity. While Chandra is more efficient, for a given exposure, in detecting CT candidates in current surveys (by a factor ∼ 2), deep XMM–Newton pointings of bright sources are vital to fully characterize their properties, for example, NH distribution above 1025 cm− 2, reflection intensity, etc., all crucial parameters of CXB models. Since luminous CT AGN at high redshift are extremely rare, the future of CT studies at high redshift will have to rely on the large-area surveys currently under way, such as XMM-XXL and Stripe82, and will then require dedicated follow-up with XMM–Newton, while waiting for the advent of the ESA mission Athena.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/588350
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