A SURVEY OF Mg II ABSORPTION AT 2 < z < 6 WITH MAGELLAN/FIRE. I. SAMPLE AND EVOLUTION OF THE Mg II FREQUENCY

We present initial results from the first systematic survey for Mg II quasar absorption lines at z > 2.5. Using infrared spectra of 46 high-redshift quasars, we discovered 111 Mg II systems over a path covering 1.9 < z < 6.3. Five systems have z > 5, with a maximum of z = 5.33-the most d...

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Bibliographic Details
Main Authors: Matejek, Michael Scott (Contributor), Simcoe, Robert A. (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor), MIT Kavli Institute for Astrophysics and Space Research (Contributor)
Format: Article
Language:English
Published: IOP Publishing, 2014-08-06T16:24:41Z.
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Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Matejek, Michael Scott  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a MIT Kavli Institute for Astrophysics and Space Research  |e contributor 
100 1 0 |a Matejek, Michael Scott  |e contributor 
100 1 0 |a Simcoe, Robert A.  |e contributor 
700 1 0 |a Simcoe, Robert A.  |e author 
245 0 0 |a A SURVEY OF Mg II ABSORPTION AT 2 < z < 6 WITH MAGELLAN/FIRE. I. SAMPLE AND EVOLUTION OF THE Mg II FREQUENCY 
260 |b IOP Publishing,   |c 2014-08-06T16:24:41Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/88544 
520 |a We present initial results from the first systematic survey for Mg II quasar absorption lines at z > 2.5. Using infrared spectra of 46 high-redshift quasars, we discovered 111 Mg II systems over a path covering 1.9 < z < 6.3. Five systems have z > 5, with a maximum of z = 5.33-the most distant Mg II system now known. The comoving Mg II line density for weaker systems (W[subscript r] < 1.0 Å) is statistically consistent with no evolution from z = 0.4 to 5.5, while that for stronger systems increases three-fold until z ~ 3 before declining again toward higher redshifts. The equivalent width distribution, which fits an exponential, reflects this evolution by flattening as z → 3 before steepening again. The rise and fall of the strong absorbers suggests a connection to the star formation rate density, as though they trace galactic outflows or other byproducts of star formation. The weaker systems' lack of evolution does not fit within this interpretation, but may be reproduced by extrapolating low redshift scaling relations between host galaxy luminosity and absorbing halo radius to earlier epochs. For the weak systems, luminosity-scaled models match the evolution better than similar models based on Mg II occupation of evolving cold dark matter halo masses, which greatly underpredict dN/dz at early times unless the absorption efficiency of small halos is significantly larger at early times. Taken together, these observations suggest that the general structure of Mg II-bearing halos was put into place early in the process of galaxy assembly. Except for a transient appearance of stronger systems near the peak epoch of cosmic star formation, the basic properties of Mg II absorbers have evolved fairly little even as the (presumably) associated galaxy population grew substantially in stellar mass and half-light radius. 
520 |a National Science Foundation (U.S.) (Grant AST-0908920) 
546 |a en_US 
655 7 |a Article 
773 |t The Astrophysical Journal