2013A&A...557A..59B


Query : 2013A&A...557A..59B

2013A&A...557A..59B - Astronomy and Astrophysics, volume 557A, 59-59 (2013/9-1)

VLT/VIMOS integral field spectroscopy of luminous and ultraluminous infrared galaxies: 2D kinematic properties.

BELLOCCHI E., ARRIBAS S., COLINA L. and MIRALLES-CABALLERO D.

Abstract (from CDS):

(Ultra) Luminous infrared galaxies [(U)LIRGs] host the most extreme star-forming events in the present universe and are places where a significant fraction of the past star formation beyond z ∼1 has occurred. The kinematic characterization of this population is important to constrain the processes that govern such events. We present and discuss the 2D kinematic properties of the ionized gas (Hα) in sample local (U)LIRGs, for which relatively high linear resolution and signal-to-noise (S/N) ratio can be obtained. We have obtained Very Large Telescope VIMOS optical integral field spectroscopy (IFS) for 38 local (z<0.1) (U)LIRGs (31 LIRGs and 7 ULIRGs, 51 individual galaxies). This sample covers well the less studied LIRG luminosity range, and it includes the morphological types corresponding to the different phases along the merging process (i.e., isolated disks, interacting and merging systems). The vast majority of objects have two main kinematically distinct components. One component (i.e., narrow or systemic) extends over the whole line-emitting region and is characterized by small-to-intermediate velocity dispersions (i.e., σ from 30 to 160km/s). The second component (broad) has a larger velocity dispersion (up to 320km/s); it is mainly found in the inner regions and is generally blueshifted with respect to the systemic component. The largest extensions and extreme kinematic properties are observed in interacting and merging systems, and they are likely associated with nuclear outflows. The systemic component traces the overall velocity field, showing a large variety of kinematic 2D structures, from very regular velocity patterns typical of pure rotating disks (29%) to kinematically perturbed disks (47%) and highly disrupted and complex velocity fields (24%). Thus, most of the objects (76%) are dominated by rotation. We find that rotation is more relevant in LIRGs than in ULIRGs. There is a clear correlation between the different phases of the merging process and the mean kinematic properties inferred from the velocity maps. In particular, isolated disks, interacting galaxies, and merging systems define a sequence of increasing mean velocity dispersion and decreasing velocity field amplitude, characterized by average dynamical ratios (vshear*/ σmean) of 4.7, 3.0 and 1.8, respectively. We also find that the σcentralmean vs. σmean plane is an excellent discriminating plane between disks and interacting/merging systems: disks show a mean ratio a factor of 2 larger than those characterizing the other two classes. The LIRGs classified as isolated disks have similar velocity amplitudes but larger mean velocity dispersions (44 vs. 24km/s) than local spirals, implying a larger turbulence and thicker disks. Interacting systems and mergers have values closer to those of low velocity dispersion elliptical/lenticular galaxies (E/SOs). The subclass of (U)LIRGs classified as mergers have kinematical properties similar to those shown by the Lyman break analogs (LBAs), although the dynamical mass of LBAs is five times lower on average. Therefore, despite the difference in mass and dust content, the kinematics of these two local populations appears to have significantly noncircular motions. These motions may be induced by the tidal forces, producing dynamically hot systems. The dynamical masses range from ∼0.04m* to 1.4m* (i.e., m*=1.4x1011M), with ULIRGs being more massive (i.e., ∼0.5±0.2m*) than LIRGs by, on average, a factor of about 2. The mass ratio of individual pre-coalescence galaxies is <2.5 for most of the systems, confirming that most (U)LIRG mergers involve sub-m* galaxies of similar mass.

Abstract Copyright:

Journal keyword(s): Galaxy: evolution - Galaxy: kinematics and dynamics

Simbad objects: 48

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Number of rows : 48
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 ESO 244-12 PaG 01 18 08.31 -44 27 43.4           ~ 87 1
2 MCG-07-03-014 Sy1 01 18 08.370 -44 27 43.29   14.43   13.06   ~ 79 0
3 NGC 633 EmG 01 36 23.418 -37 19 17.64   13.50   12.50   ~ 93 1
4 ESO 297-12 Sy2 01 36 24.1505027520 -37 20 25.708312896   15.06   13.76 14.7 ~ 50 1
5 NGC 1614 Sy1 04 34 00.027 -08 34 44.57   14.66 13.99     ~ 667 0
6 LEDA 17155 Sy2 05 21 01.3994605776 -25 21 45.321827832   15.47 14.75     ~ 498 0
7 LEDA 89499 Sy2 06 02 54.066 -71 03 10.48   15.6       ~ 94 1
8 IRAS 06076-2139 Sy2 06 09 45.7858957392 -21 40 23.614857120   15.64   14.46   ~ 79 0
9 LEDA 89500 Sy2 06 21 01.188 -63 17 23.81   16.70   15.27   ~ 68 1
10 ESO 255-7 EmG 06 27 22.588 -47 10 46.45   14.48   13.60   ~ 67 0
11 ESO 557-2 EmG 06 31 47.217 -17 37 17.09   15.03   13.21   ~ 68 0
12 IRAS 06592-6313 Sy2 06 59 40.2750782328 -63 17 53.022471360   15.61   14.28   ~ 55 0
13 LEDA 90054 Sy2 07 03 24.2524870728 -60 15 22.448628792   16.02   14.72   ~ 57 1
14 NGC 2369 Sy1 07 16 37.753 -62 20 37.51   13.23   11.56 12.3 ~ 130 0
15 2MASX J08370182-4954302 G 08 37 01.827 -49 54 30.27           ~ 59 0
16 ESO 432-6 AG? 08 44 27.2 -31 41 51   16.4       ~ 33 0
17 ESO 60-16 G 08 52 30.77 -69 01 59.8           ~ 43 0
18 LEDA 24922 G 08 52 32.047 -69 01 55.74   16.01   15.17   ~ 40 0
19 NAME IRAS F08572+3915 NW LIN 09 00 25.364 +39 03 54.23     16.66     ~ 420 1
20 2MASX J09041268-3627007 G 09 04 12.689 -36 27 00.76           ~ 85 0
21 IC 563 AG? 09 46 20.361 +03 02 43.86   14.7       ~ 91 0
22 IC 564 rG 09 46 21.0998750808 +03 04 17.078546964   14.1       ~ 97 0
23 NGC 3110 Sy1 10 04 02.0 -06 28 29   13.4   13.3 12.5 ~ 174 3
24 IC 2545 Sy1 10 06 04.581 -33 53 05.55   15.27 14.27 14.25   ~ 111 0
25 NGC 3256 Sy2 10 27 51.284 -43 54 13.55   11.83 11.33 10.62 11.9 ~ 847 2
26 ESO 264-36 Sy2 10 43 07.676 -46 12 44.50   14.34   12.55   ~ 77 0
27 ESO 264-57 AG? 10 59 01.794 -43 26 25.81   15.02   13.22   ~ 70 0
28 ESO 319-22 EmG 11 27 54.0785626512 -41 36 52.264754784   14.56   16.21   ~ 63 0
29 ESO 320-30 EmG 11 53 11.722 -39 07 48.72   13.30   11.86   ~ 186 1
30 ESO 440-58 IG 12 06 51.8 -31 56 47   15.44   14.89   ~ 61 0
31 ESO 267-30 Sy1 12 14 12.839 -47 13 43.42   14.20   12.69 12.9 ~ 78 0
32 2MASX J12142211-5632332 G 12 14 22.0958120832 -56 32 33.317528712   16.8       ~ 59 0
33 MCG-02-33-098 AG? 13 02 19.5 -15 46 05   14       ~ 89 0
34 MCG-02-33-099 GiG 13 02 20.3897926848 -15 45 59.619522384   18   13.16   ~ 29 0
35 ESO 507-70 Sy1 13 02 52.3177169808 -23 55 17.932558692   14.77 14.78 13.24 13.59 ~ 121 0
36 NGC 5135 Sy2 13 25 44.059 -29 50 01.24   12.58 13.35 11.53 12.2 ~ 474 1
37 IC 4518 Sy2 14 57 45.6 -43 07 58   14.5       ~ 74 0
38 IC 4553 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 2959 4
39 IRAS 17138-1017 Sy2 17 16 35.83992 -10 20 38.9832   17.43   14.59   ~ 131 0
40 LEDA 60189 LIN 17 23 21.943 -00 17 00.96   15.1       ~ 424 0
41 IC 4686 AG? 18 13 38.7810951072 -57 43 57.306382932   14.67   13.52   ~ 67 1
42 IC 4687 AGN 18 13 39.829 -57 43 31.25   14.35 14.3 12.78   ~ 136 1
43 IC 4689 Sy2 18 13 40.334 -57 44 54.25   15.07   13.48   ~ 50 0
44 2MASX J21161852-4433374 G 21 16 18.5751072336 -44 33 37.139108652   17.48   16.24   ~ 26 1
45 NGC 7130 Sy2 21 48 19.5412287192 -34 57 04.492024884   12.86 13.87 11.57   ~ 450 0
46 IC 5179 Sy1 22 16 09.1191653256 -36 50 37.117603752   12.29 11.89 11.38   ~ 204 1
47 NAME South America H2G 22 51 49.307 -17 52 23.96   16.97       ~ 327 3
48 ESO 148-2 Sy2 23 15 46.772 -59 03 15.94   14.94 14.73 13.95   ~ 265 1

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