Kinematics of the intermediate-mass black hole candidate HLX-1

We studied the optical spectrum of HLX-1 during its latest outburst, using the FORS2 spectrograph on the Very Large Telescope. We detect an Hα emission line centered at λ = 6718.9 ± 0.9 Å and find that its projected radial velocity with respect to the nucleus of ESO 243–49 is 424 ± 27 km s–1, while...

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Main Authors: Soria, Roberto, Hau, G., Pakull, M.
Format: Journal Article
Published: Institute of Physics Publishing 2013
Subjects:
Online Access:http://hdl.handle.net/20.500.11937/19722
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author Soria, Roberto
Hau, G.
Pakull, M.
author_facet Soria, Roberto
Hau, G.
Pakull, M.
author_sort Soria, Roberto
building Curtin Institutional Repository
collection Online Access
description We studied the optical spectrum of HLX-1 during its latest outburst, using the FORS2 spectrograph on the Very Large Telescope. We detect an Hα emission line centered at λ = 6718.9 ± 0.9 Å and find that its projected radial velocity with respect to the nucleus of ESO 243–49 is 424 ± 27 km s–1, while the maximum rotational velocity of the stars in that galaxy is 209 km s–1. This suggests that HLX-1 and its surrounding stars were not formed in situ, but came either from a disrupted dwarf galaxy or from a nuclear recoil. We also find that the Hα emission line is resolved with FWHM 400 km s–1, suggesting a nebular rather than disk origin for the emission. Its luminosity (L Hα = a few 1037 erg s–1, equivalent width = 70 Å) is also consistent with emission from a nebula photoionized by HLX-1.
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spelling curtin-20.500.11937-197222017-09-13T13:48:14Z Kinematics of the intermediate-mass black hole candidate HLX-1 Soria, Roberto Hau, G. Pakull, M. individual (Abell 2877) galaxies: clusters galaxies: individual (ESO 243–49) accretion accretion disks black hole physics We studied the optical spectrum of HLX-1 during its latest outburst, using the FORS2 spectrograph on the Very Large Telescope. We detect an Hα emission line centered at λ = 6718.9 ± 0.9 Å and find that its projected radial velocity with respect to the nucleus of ESO 243–49 is 424 ± 27 km s–1, while the maximum rotational velocity of the stars in that galaxy is 209 km s–1. This suggests that HLX-1 and its surrounding stars were not formed in situ, but came either from a disrupted dwarf galaxy or from a nuclear recoil. We also find that the Hα emission line is resolved with FWHM 400 km s–1, suggesting a nebular rather than disk origin for the emission. Its luminosity (L Hα = a few 1037 erg s–1, equivalent width = 70 Å) is also consistent with emission from a nebula photoionized by HLX-1. 2013 Journal Article http://hdl.handle.net/20.500.11937/19722 10.1088/2041-8205/768/1/L22 Institute of Physics Publishing fulltext
spellingShingle individual (Abell 2877)
galaxies: clusters
galaxies: individual (ESO 243–49)
accretion
accretion disks
black hole physics
Soria, Roberto
Hau, G.
Pakull, M.
Kinematics of the intermediate-mass black hole candidate HLX-1
title Kinematics of the intermediate-mass black hole candidate HLX-1
title_full Kinematics of the intermediate-mass black hole candidate HLX-1
title_fullStr Kinematics of the intermediate-mass black hole candidate HLX-1
title_full_unstemmed Kinematics of the intermediate-mass black hole candidate HLX-1
title_short Kinematics of the intermediate-mass black hole candidate HLX-1
title_sort kinematics of the intermediate-mass black hole candidate hlx-1
topic individual (Abell 2877)
galaxies: clusters
galaxies: individual (ESO 243–49)
accretion
accretion disks
black hole physics
url http://hdl.handle.net/20.500.11937/19722