2013ApJ...778..187F


Query : 2013ApJ...778..187F

2013ApJ...778..187F - Astrophys. J., 778, 187 (2013/December-1)

The high-ion content and kinematics of low-redshift Lyman limit systems.

FOX A.J., LEHNER N., TUMLINSON J., HOWK J.C., TRIPP T.M., PROCHASKA J.X., O'MEARA J.M., WERK J.K., BORDOLOI R., KATZ N., OPPENHEIMER B.D. and DAVE R.

Abstract (from CDS):

We study the high-ion content and kinematics of the circumgalactic medium around low-redshift galaxies using a sample of 23 Lyman limit systems (LLSs) at 0.08 < z < 0.93 observed with the Cosmic Origins Spectrograph on board the Hubble Space Telescope. In Lehner et al., we recently showed that low-z LLSs have a bimodal metallicity distribution. Here we extend that analysis to search for differences between the high-ion and kinematic properties of the metal-poor and metal-rich branches. We find that metal-rich LLSs tend to show higher O VI columns and broader O VI profiles than metal-poor LLSs. The total H I line width (Δv90statistic) in LLSs is not correlated with metallicity, indicating that the H I kinematics alone cannot be used to distinguish inflow from outflow and gas recycling. Among the 17 LLSs with O VI detections, all but two show evidence of kinematic sub-structure, in the form of O VI-H I centroid offsets, multiple components, or both. Using various scenarios for how the metallicities in the high-ion and low-ion phases of each LLS compare, we constrain the ionized hydrogen column in the O VI phase to lie in the range log N(H II) ∼ 17.6-20. The O VI phase of LLSs is a substantial baryon reservoir, with M(high-ion) ∼ 108.5–10.9 (r/150 kpc)2 M☉, similar to the mass in the low-ion phase. Accounting for the O VI phase approximately doubles the contribution of low-z LLSs to the cosmic baryon budget.

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Journal keyword(s): galaxies: halos - galaxies: kinematics and dynamics - intergalactic medium

Simbad objects: 18

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Number of rows : 18
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 QSO J0155-4506 QSO 01 55 13.2179169408 -45 06 11.577944484   15.1       ~ 54 0
2 4C -04.06 QSO 02 35 07.3418452008 -04 02 05.317096956   16.61 16.46 16.2   ~ 222 1
3 PKS 0405-123 Bla 04 07 48.4309841856 -12 11 36.659928408   15.09 14.86 14.7   ~ 531 1
4 QSO J0440-5248 QSO 04 40 12.0482632416 -52 48 17.514120888     16.10     ~ 42 0
5 2MASS J05522451-6402108 Sy1 05 52 24.5023213488 -64 02 10.757771160     15.04     ~ 55 1
6 QSO J0635-7516 Bla 06 35 46.5079301472 -75 16 16.816418256   15.96 15.75 15.82   ~ 625 1
7 QSO J0943+0531 QSO 09 43 31.6146408840 +05 31 31.475664912   17.50 17.30     ~ 57 0
8 Ton 1388 Sy1 11 19 08.6786220240 +21 19 17.987085948   14.91 14.80     ~ 492 0
9 SBSG 1123+594A QSO 11 25 53.7896103984 +59 10 21.552070044   17.02 16.80     ~ 69 0
10 QSO J1208+4540 QSO 12 08 58.0107013896 +45 40 35.421692952   16.00 15.70     ~ 194 0
11 PG 1216+069 Sy1 12 19 20.9318278680 +06 38 38.467059252   15.68 15.65     ~ 302 0
12 QSO J1341+4123 QSO 13 41 00.7893930432 +41 23 14.130152880   17.04 16.76     ~ 131 0
13 QSO J1409+2618 QSO 14 09 23.9085820008 +26 18 21.056458176   16.07 15.74     ~ 193 0
14 PB 2049 QSO 14 19 10.2069131136 +42 07 46.911715896   16.9 17.31 17.1   ~ 50 0
15 QSO J1435+3604 QSO 14 35 11.5257590496 +36 04 37.175594052   17.30 17.22     ~ 63 0
16 QSO B1521+1009 QSO 15 24 24.5234088744 +09 58 29.087917572   15.74 16.2     ~ 145 0
17 QSO J1619+3342 QSO 16 19 16.5426908544 +33 42 38.375748828   17.30 17.26     ~ 61 0
18 QSO B1630+3744 QSO 16 32 01.1117931960 +37 37 49.980505332   16.50 16.30     ~ 183 0

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