2005ApJ...621..725C


Query : 2005ApJ...621..725C

2005ApJ...621..725C - Astrophys. J., 621, 725-737 (2005/March-2)

Kinematics of low-z ultraluminous infrared galaxies and implications for dynamical mass derivations in high-z star-forming galaxies.

COLINA L., ARRIBAS S. and MONREAL-IBERO A.

Abstract (from CDS):

The kinematic properties of the gaseous and stellar components of 11 ultraluminous infrared galaxies (ULIRGs; 14 nuclei) are investigated by means of integral field spectroscopy (IFS) with the INTEGRAL system and available IR and CO millimeter spectroscopy. The sample of ULIRGs cover different phases of the merging process and span all levels of activity from pure starbursts to Seyfert nuclei. The IFS data show that the ionized gas has a complex velocity structure with peak-to-peak velocity differences of a few to several hundred km/s, detected in tidal tails or extranuclear star-forming regions. The velocity field of the ionized gas on scales of a few to several kiloparsecs is dominated by tidally induced flows and does not, in general, correspond to rotationally supported systems with a privileged orientation along the major rotating axis. The central velocity amplitude of the ionized gas and stars shows discrepancies in some galaxies but has, on average, a similar value (ratio of 0.92±0.37), while the velocity amplitude of the molecular gas is a factor of 2 larger (ratio of 1.9±0.6) than that of the stars and ionized gas. The central velocity amplitude measured using different kinematic tracers should therefore not be used in ULIRGs as a reliable tracer of mass, in general. The IFS data also show that the velocity dispersion of the ionized gas maps the large-scale motions associated with tidal tails and extranuclear regions, with often the highest velocity dispersion not being associated with the nucleus galaxies. There is, however, a good agreement between the central ionized gas and stellar velocity dispersions (ratio of 1.01±0.13), while the cold molecular gas velocity dispersion has lower values (average of about 0.8 that of the stellar and ionized gas). The central ionized gas velocity dispersion is therefore a robust and homogeneous observable and a good tracer of the dynamical mass in these systems. The IFS-based central ionized gas velocity dispersion measurements confirm that ULIRGs' hosts are moderate-mass (≤m*) galaxies, as previously concluded by Tacconi and coworkers. In general, velocity amplitudes should not be used to estimate the dynamical mass in high-z star-forming systems, such as Lyman break and in particular submillimeter galaxies, since they show irregular stellar and gaseous structures similar to those present in low-z merging systems such as ULIRGs, the subject of this study. A more reliable method is to measure the central velocity dispersion using the strong, high equivalent width, rest-frame optical emission lines, provided the location of the nucleus is independently established by high angular resolution red or near-IR rest-frame imaging. The kinematics derived from the millimeter CO line suggest that the cold gas in ULIRGs does not share the velocity field of the stars and ionized gas and seems to be more rotationally supported. This result needs to be investigated in more detail with a larger sample of low-z ULIRGs before using the millimeter CO line widths as a dynamical mass tracer in high-z submillimeter galaxies.

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Journal keyword(s): Galaxies: Active - Galaxies: Interactions - Galaxies: Kinematics and Dynamics - Galaxies: Nuclei - Galaxies: Starburst - Infrared: Galaxies

Simbad objects: 20

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Number of rows : 20
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 NAME SMM J02399-0136 rG 02 39 51.87 -01 35 58.8       21.20   ~ 201 2
2 SAS-LBG Q0256-C17 G 02 58 59.850 +00 10 52.60       23.89   ~ 6 0
3 [PKS98] Q0347-383 C5 G 03 49 43.5 -38 10 05           ~ 9 0
4 IRAS 08572+3915 LIN 09 00 25.38288 +39 03 54.2988     16.66     ~ 450 1
5 SDSS J090025.61+390349.2 GiP 09 00 25.6120608672 +39 03 49.407843816           ~ 19 1
6 [CGM90] IRAS 12112+0305 SW rG 12 13 45.9376041667 +02 48 39.097125317           ~ 36 0
7 IRAS 12112+0305 PaG 12 13 45.98880 +02 48 39.9600           ~ 373 0
8 [CGM90] IRAS 12112+0305 NE rG 12 13 46.10735 +02 48 41.4959           ~ 369 0
9 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
10 Z 271-60 Sy2 13 44 42.1883001099 +55 53 13.596220922   15.68 14.91     ~ 958 3
11 NAME SMM J14011+0252 rG 14 01 04.95 +02 52 24.0           ~ 156 1
12 LEDA 52270 Sy1 14 37 38.2867288488 -15 00 24.087592692   16.58 16.40     ~ 300 2
13 [CGM90] IRAS 14348-1447 NE GiP 14 37 38.35 -15 00 21.3           ~ 24 0
14 IRAS 15206+3342 Sy2 15 22 38.104 +33 31 35.90           ~ 111 0
15 2MASX J15265942+3558372 LIN 15 26 59.44451 +35 58 37.0521   15.61       ~ 295 1
16 IC 1127 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 3090 4
17 2MASX J16023279+3734532 LIN 16 02 32.798 +37 34 53.28           ~ 19 0
18 LEDA 60189 LIN 17 23 21.96264 -00 17 00.8088   15.1       ~ 454 0
19 LEDA 90352 LIN 20 11 23.86872 -02 59 50.7588   17.80   16.41   ~ 78 0
20 LEDA 90429 SyG 23 39 01.26960 +36 21 08.5896   16.17       ~ 232 1

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