Measuring the low mass end of the M• - σ relation

We show that high quality laser guide star (LGS) adaptive optics (AO) observations of nearby early-type galaxies are possible when the tip-tilt correction is done by guiding on nuclei while the focus compensation due to the changing distance to the sodium layer is made 'open loop'. We achi...

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Main Authors: Krajnović, D, McDermid, R, Cappellari, M, Davies, R
Format: Journal article
Language:English
Published: 2010
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author Krajnović, D
McDermid, R
Cappellari, M
Davies, R
author_facet Krajnović, D
McDermid, R
Cappellari, M
Davies, R
author_sort Krajnović, D
collection OXFORD
description We show that high quality laser guide star (LGS) adaptive optics (AO) observations of nearby early-type galaxies are possible when the tip-tilt correction is done by guiding on nuclei while the focus compensation due to the changing distance to the sodium layer is made 'open loop'. We achieve corrections such that 40% of flux comes from R<0.2 arcsec. To measure a black hole mass (M•) one needs integral field observations of both high spatial resolution and large field of view. With these data it is possible to determine the lower limit to M• even if the spatial resolution of the observations are up to a few times larger than the sphere of influence of the black hole. © 2010 American Institute of Physics.
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spelling oxford-uuid:ea89d1a1-0d50-47ae-9ea4-1653f700cde92022-03-27T11:03:04ZMeasuring the low mass end of the M• - σ relationJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:ea89d1a1-0d50-47ae-9ea4-1653f700cde9EnglishSymplectic Elements at Oxford2010Krajnović, DMcDermid, RCappellari, MDavies, RWe show that high quality laser guide star (LGS) adaptive optics (AO) observations of nearby early-type galaxies are possible when the tip-tilt correction is done by guiding on nuclei while the focus compensation due to the changing distance to the sodium layer is made 'open loop'. We achieve corrections such that 40% of flux comes from R<0.2 arcsec. To measure a black hole mass (M•) one needs integral field observations of both high spatial resolution and large field of view. With these data it is possible to determine the lower limit to M• even if the spatial resolution of the observations are up to a few times larger than the sphere of influence of the black hole. © 2010 American Institute of Physics.
spellingShingle Krajnović, D
McDermid, R
Cappellari, M
Davies, R
Measuring the low mass end of the M• - σ relation
title Measuring the low mass end of the M• - σ relation
title_full Measuring the low mass end of the M• - σ relation
title_fullStr Measuring the low mass end of the M• - σ relation
title_full_unstemmed Measuring the low mass end of the M• - σ relation
title_short Measuring the low mass end of the M• - σ relation
title_sort measuring the low mass end of the m• σ relation
work_keys_str_mv AT krajnovicd measuringthelowmassendofthemsrelation
AT mcdermidr measuringthelowmassendofthemsrelation
AT cappellarim measuringthelowmassendofthemsrelation
AT daviesr measuringthelowmassendofthemsrelation