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Article Contents
- ABSTRACT
- 1.INTRODUCTION
- 1.1.A brief overview of obscured
AGN
- 1.2.The importance of identifying
obscured AGN
- 2.IDENTIFICATION OF OBSCURED AGN
- 2.1.Selection of obscured AGN in the
ultra-violet to near-infrared waveband
- 2.1.1.Broad-band continuum
techniques
- 2.1.2.Spectroscopic
techniques
- 2.2.Selection of obscured AGN in
the X-ray waveband
- 2.3.Selection of obscured AGN in
the mid-infrared waveband
- 2.3.1.Broad-band continuum
techniques
- 2.3.2.Spectroscopic techniques
- 2.4.Selection of obscured AGN at
far-infrared-radio wavelengths
- 2.4.1.Far-infrared-millimeter
wavelengths
- 2.4.2.Radio wavelengths
- 2.5.Multi-wavelength identification
and a comparison of selection methods
- 3.THE DEMOGRAPHICS OF THE OBSCURED AGN
POPULATION
- 4.THE PHYSICAL NATURE OF OBSCURATION
IN AGN
- 4.1.The nuclear torus and the
unified AGN model
- 4.1.1.The basic torus
properties are well-constrained
- 4.1.2.The torus is clumpy
- 4.1.3.The torus can have a
range of covering factors, with dependence on AGN properties
- 4.1.4.The torus is dynamic
- 4.1.5.The torus may extend in the
polar direction, and to large scales
- 4.2.Obscuration by nuclear
starbursts
- 4.3.Obscuration by galaxy-scale
material
- 5.IMPLICATIONS FOR OBSCURED AGN IN
OBSERVATIONAL COSMOLOGY
- 5.1.The evolutionary sequence and
the SMBH-galaxy connection
- 5.2.The evolution of obscured SMBHs
at high redshift
- 5.3.Obscured AGN, the cosmic X-ray
background, and the radiative efficiency of black hole accretion
- 6.CONCLUSIONS AND FUTURE PROSPECTS
- 6.1.Forecasts for future
facilities
- 6.1.1.UV-Near-IR
- 6.1.2.X-rays
- 6.1.3.Mid-IR
- 6.1.4.Far-IR-radio
- 6.2.Prospects for theoretical
models
- 6.3.Outstanding questions
- 6.3.1.What is the physical
origin of the torus?
- 6.3.2.What is the evolution of AGN
obscuration and the connection to galaxy formation?
- 6.3.3.How do we find the most
heavily obscured AGN?
- 6.3.4.What is the role of
obscured accretion at the dawn of the first SMBHs?
- REFERENCES