2019ApJ...870..137K


Query : 2019ApJ...870..137K

2019ApJ...870..137K - Astrophys. J., 870, 137-137 (2019/January-2)

The relation between galaxy ISM and circumgalactic O VI gas kinematics derived from observations and ΛCDM Simulations.

KACPRZAK G.G., VANDER VLIET J.R., NIELSEN N.M., MUZAHID S., POINTON S.K., CHURCHILL C.W., CEVERINO D., ARRAKI K.S., KLYPIN A., CHARLTON J.C. and LEWIS J.

Abstract (from CDS):

We present the first galaxy-O VI absorption kinematic study for 20 absorption systems (EW > 0.1 Å) associated with isolated galaxies (0.15 <= z <= 0.55) that have accurate redshifts and rotation curves obtained using Keck/ESI. Our sample is split into two azimuthal angle bins: major axis (Φ < 25°) and minor axis (Φ > 33°). O VI absorption along the galaxy major axis is not correlated with galaxy rotation kinematics, with only 1/10 of systems that could be explained with rotation/accretion models. This is in contrast to corotation commonly observed for Mg II absorption. O VI along the minor axis could be modeled by accelerating outflows, but only for small opening angles, while the majority of the O VI is decelerating. Along both axes, stacked O VI profiles reside at the galaxy systemic velocity with the absorption kinematics spanning the entire dynamical range of their galaxies. The O VI found in AMR cosmological simulations exists within filaments and in halos of ∼50 kpc surrounding galaxies. Simulations show that major-axis O VI gas inflows along filaments and decelerates as it approaches the galaxy, while increasing in its level of corotation. Minor-axis outflows in the simulations are effective within 50-75 kpc; beyond that they decelerate and fall back onto the galaxy. Although the simulations show clear O VI kinematic signatures, they are not directly comparable to observations. When we compare kinematic signatures integrated through the entire simulated galaxy halo, we find that these signatures are washed out owing to full velocity distribution of O VI throughout the halo. We conclude that O VI alone does not serve as a useful kinematic indicator of gas accretion, outflows, or star formation and likely best probes the halo virial temperature.

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

Journal keyword(s): galaxies: halos - quasars: absorption lines

Simbad objects: 15

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Number of rows : 15
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 J0125-0006 Bla 01 25 28.8438355224 -00 05 55.930595964   16.92 16.64 16.30   ~ 305 1
2 3C 95 Sy1 03 51 28.5673217616 -14 29 08.257870248 15.62 16.55 16.22     ~ 192 1
3 QSO J0456-2159 Bla 04 56 08.9237717400 -21 59 09.399816312 15.76 16.16 16.10 15.9   ~ 196 1
4 QSO J0914+2823 QSO 09 14 40.3889730816 +28 23 30.631322940   17.5 18.10 17.6   ~ 43 0
5 QSO J0943+0531 QSO 09 43 31.6146408840 +05 31 31.475664912   17.50 17.30     ~ 57 0
6 QSO B0946+487 QSO 09 50 00.7413113688 +48 31 29.333280720   17.56 17.47     ~ 73 0
7 QSO J1009+0713 QSO 10 09 02.0682581400 +07 13 43.900917312   17.41 17.27     ~ 72 1
8 4C 06.41 BLL 10 41 17.16249940 +06 10 16.9237327   16.86 16.70 16.14   ~ 302 1
9 QSO J1139-1350 Bla 11 39 10.7025556152 -13 50 43.639196064   16.38 16.17 16.4   ~ 284 1
10 QSO J1241+5721 QSO 12 41 54.0240017616 +57 21 07.358808924   18.03 17.94     ~ 51 0
11 [JCM2015] J132222.46+464546.1 G 13 22 22.470 +46 45 46.17   20.2   18.6 18.6 ~ 14 0
12 LBQS 1340-0038 QSO 13 42 51.6065445120 -00 53 45.385834848   17.15 16.98 17.418 16.198 ~ 87 0
13 QSO J1555+3628 QSO 15 55 04.4016223056 +36 28 47.958261960   17.3 18.10 17.6   ~ 48 0
14 QSO B2128-123 BLL 21 31 35.2617909696 -12 07 04.795364172   16.33 16.11 15.87   ~ 470 1
15 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 3004 2

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