OUTFLOW VERSUS INFALL IN SPIRAL GALAXIES: METAL ABSORPTION IN THE HALO OF NGC 891

Gas accreting onto a galaxy will be of low metallicity while halo gas due to a galactic fountain will be of near-solar metallicity. We test these predictions by measuring the metal absorption line properties of halo gas 5 kpc above the plane of the edge-on galaxy NGC 891, using observations taken wi...

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Bibliographic Details
Main Authors: Bregman, Joel N. (Author), Seitzer, Patrick (Author), Cowley, C. R. (Author), Miller, Matthew J. (Author), Miller, Eric D (Author)
Other Authors: MIT Kavli Institute for Astrophysics and Space Research (Contributor), Miller, Eric D. (Contributor)
Format: Article
Language:English
Published: IOP Publishing, 2015-02-18T14:26:22Z.
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042 |a dc 
100 1 0 |a Bregman, Joel N.  |e author 
100 1 0 |a MIT Kavli Institute for Astrophysics and Space Research  |e contributor 
100 1 0 |a Miller, Eric D.  |e contributor 
700 1 0 |a Seitzer, Patrick  |e author 
700 1 0 |a Cowley, C. R.  |e author 
700 1 0 |a Miller, Matthew J.  |e author 
700 1 0 |a Miller, Eric D  |e author 
245 0 0 |a OUTFLOW VERSUS INFALL IN SPIRAL GALAXIES: METAL ABSORPTION IN THE HALO OF NGC 891 
260 |b IOP Publishing,   |c 2015-02-18T14:26:22Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/94577 
520 |a Gas accreting onto a galaxy will be of low metallicity while halo gas due to a galactic fountain will be of near-solar metallicity. We test these predictions by measuring the metal absorption line properties of halo gas 5 kpc above the plane of the edge-on galaxy NGC 891, using observations taken with HST/STIS toward a bright background quasar. Metal absorption lines of Fe II, Mg II, and Mg I in the halo of NGC 891 are clearly seen, and when combined with recent deep H I observations, we are able to place constraints on the metallicity of the halo gas for the first time. The H I line width defines the line broadening, from which we model opacity effects in these metal lines, assuming that the absorbing gas is continuously distributed in the halo. The gas-phase metallicities are [Fe/H] = -1.18 ± 0.07 and [Mg/H] = -0.23 + 0.36/ - 0.27 (statistical errors) and this difference is probably due to differential depletion onto grains. When corrected for such depletion using Galactic gas as a guide, both elements have approximately solar or even supersolar abundances. This suggests that the gas is from the galaxy disk, probably expelled into the halo by a galactic fountain, rather than from accretion of intergalactic gas, which would have a low metallicity. The abundances would be raised by significant amounts if the absorbing gas lies in a few clouds with thermal widths smaller than the rotational velocity of the halo. If this is the case, both the abundances and [Mg/Fe] would be supersolar. 
520 |a United States. National Aeronautics and Space Administration (Hubble Space Telescope Grant) 
520 |a United States. National Aeronautics and Space Administration (Long Term Space Astrophysics Grant) 
520 |a United States. National Aeronautics and Space Administration (Astrophysics Data Analysis Program Grant) 
546 |a en_US 
655 7 |a Article 
773 |t The Astrophysical Journal