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Obscured goods active galactic nuclei and their host galaxies at z <1.25: the slow black hole growth phase

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Obscured goods active galactic nuclei and their host galaxies at z <1.25: the slow black hole growth phase. / Simmons, B. D.; Van Duyne, J.; Urry, C. M. et al.
In: The Astrophysical Journal, Vol. 734, No. 2, 121, 20.06.2011.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Simmons, BD, Van Duyne, J, Urry, CM, Treister, E, Koekemoer, AM & Grogin, NA 2011, 'Obscured goods active galactic nuclei and their host galaxies at z <1.25: the slow black hole growth phase', The Astrophysical Journal, vol. 734, no. 2, 121. https://doi.org/10.1088/0004-637X/734/2/121

APA

Simmons, B. D., Van Duyne, J., Urry, C. M., Treister, E., Koekemoer, A. M., & Grogin, N. A. (2011). Obscured goods active galactic nuclei and their host galaxies at z <1.25: the slow black hole growth phase. The Astrophysical Journal, 734(2), Article 121. https://doi.org/10.1088/0004-637X/734/2/121

Vancouver

Simmons BD, Van Duyne J, Urry CM, Treister E, Koekemoer AM, Grogin NA. Obscured goods active galactic nuclei and their host galaxies at z <1.25: the slow black hole growth phase. The Astrophysical Journal. 2011 Jun 20;734(2):121. doi: 10.1088/0004-637X/734/2/121

Author

Simmons, B. D. ; Van Duyne, J. ; Urry, C. M. et al. / Obscured goods active galactic nuclei and their host galaxies at z <1.25 : the slow black hole growth phase. In: The Astrophysical Journal. 2011 ; Vol. 734, No. 2.

Bibtex

@article{6c2501c362384288b9e3ca7e4758b7a5,
title = "Obscured goods active galactic nuclei and their host galaxies at z <1.25: the slow black hole growth phase",
abstract = "We compute black hole masses and bolometric luminosities for 87 obscured active galactic nuclei (AGNs) in the redshift range 0.25 ≤ z ≤ 1.25, selected from the GOODS deep multi-wavelength survey fields via their X-ray emission. We fit the optical images and obtain morphological parameters for the host galaxy, separating the galaxy from its central point source, thereby obtaining a four-band optical spectral energy distribution (SED) for each active nucleus. We calculate bolometric luminosities for these AGNs by reddening a normalized mean SED of GOODS broad-line AGNs to match the observed central point-source SED of each obscured AGN. This estimate of L bol has a smaller spread than simple bolometric corrections to the X-ray luminosity or direct integration of the observed multi-wavelength SED, suggesting it is a better measure. We estimate central black hole masses from the bulge luminosities. The black hole masses span a wide range, 7 × 106 M ☉ to 6 × 109 M ☉; the median black hole mass is 5 × 108 M ☉. The majority of these AGNs have L/L Edd ≤ 0.01, and we detect no significant evolution of the mean Eddington ratio to z = 1.25. This implies that the bulk of black hole growth in these obscured AGNs must have occurred at z gsim 1 and that we are observing these AGNs in a slow- or no-growth state.",
author = "Simmons, {B. D.} and {Van Duyne}, J. and Urry, {C. M.} and E. Treister and Koekemoer, {A. M.} and Grogin, {N. A.}",
year = "2011",
month = jun,
day = "20",
doi = "10.1088/0004-637X/734/2/121",
language = "English",
volume = "734",
journal = "The Astrophysical Journal",
issn = "0004-637X",
publisher = "Institute of Physics Publishing",
number = "2",

}

RIS

TY - JOUR

T1 - Obscured goods active galactic nuclei and their host galaxies at z <1.25

T2 - the slow black hole growth phase

AU - Simmons, B. D.

AU - Van Duyne, J.

AU - Urry, C. M.

AU - Treister, E.

AU - Koekemoer, A. M.

AU - Grogin, N. A.

PY - 2011/6/20

Y1 - 2011/6/20

N2 - We compute black hole masses and bolometric luminosities for 87 obscured active galactic nuclei (AGNs) in the redshift range 0.25 ≤ z ≤ 1.25, selected from the GOODS deep multi-wavelength survey fields via their X-ray emission. We fit the optical images and obtain morphological parameters for the host galaxy, separating the galaxy from its central point source, thereby obtaining a four-band optical spectral energy distribution (SED) for each active nucleus. We calculate bolometric luminosities for these AGNs by reddening a normalized mean SED of GOODS broad-line AGNs to match the observed central point-source SED of each obscured AGN. This estimate of L bol has a smaller spread than simple bolometric corrections to the X-ray luminosity or direct integration of the observed multi-wavelength SED, suggesting it is a better measure. We estimate central black hole masses from the bulge luminosities. The black hole masses span a wide range, 7 × 106 M ☉ to 6 × 109 M ☉; the median black hole mass is 5 × 108 M ☉. The majority of these AGNs have L/L Edd ≤ 0.01, and we detect no significant evolution of the mean Eddington ratio to z = 1.25. This implies that the bulk of black hole growth in these obscured AGNs must have occurred at z gsim 1 and that we are observing these AGNs in a slow- or no-growth state.

AB - We compute black hole masses and bolometric luminosities for 87 obscured active galactic nuclei (AGNs) in the redshift range 0.25 ≤ z ≤ 1.25, selected from the GOODS deep multi-wavelength survey fields via their X-ray emission. We fit the optical images and obtain morphological parameters for the host galaxy, separating the galaxy from its central point source, thereby obtaining a four-band optical spectral energy distribution (SED) for each active nucleus. We calculate bolometric luminosities for these AGNs by reddening a normalized mean SED of GOODS broad-line AGNs to match the observed central point-source SED of each obscured AGN. This estimate of L bol has a smaller spread than simple bolometric corrections to the X-ray luminosity or direct integration of the observed multi-wavelength SED, suggesting it is a better measure. We estimate central black hole masses from the bulge luminosities. The black hole masses span a wide range, 7 × 106 M ☉ to 6 × 109 M ☉; the median black hole mass is 5 × 108 M ☉. The majority of these AGNs have L/L Edd ≤ 0.01, and we detect no significant evolution of the mean Eddington ratio to z = 1.25. This implies that the bulk of black hole growth in these obscured AGNs must have occurred at z gsim 1 and that we are observing these AGNs in a slow- or no-growth state.

U2 - 10.1088/0004-637X/734/2/121

DO - 10.1088/0004-637X/734/2/121

M3 - Journal article

VL - 734

JO - The Astrophysical Journal

JF - The Astrophysical Journal

SN - 0004-637X

IS - 2

M1 - 121

ER -