2010A&A...521A..63L


Query : 2010A&A...521A..63L

2010A&A...521A..63L - Astronomy and Astrophysics, volume 521, A63-63 (2010/10-1)

Massive star formation in Wolf-Rayet galaxies. V. Star-formation rates, masses and the importance of galaxy interactions.

LOPEZ-SANCHEZ A.R.

Abstract (from CDS):

We performed a comprehensive analysis of a sample of 20 starburst galaxies that show a substantial population of very young massive stars, most of them classified as Wolf-Rayet galaxies. In this paper, the last in the series, we analyze the global properties of our galaxy sample using multiwavelength data extracted from our own observations (Hα fluxes, B and H-band magnitudes) and from the literature, which include X-ray, FUV, FIR, and radio (both Hi spectral line and 1.4GHz radio-continuum) measurements. The agreement between our Hα-based star-formation rates (Sfr) and those provided by indicators at other wavelengths is remarkable, but we consider that the new Hα-based calibration provided by Calzetti et al. (2007ApJ...666..870C) should be preferred to older calibrations. The FUV-based Sfr provides a powerful tool for analyzing the star-formation activity on both global and local scales independently to the Hα emission. We provide empirical relationships between the ionized gas mass, neutral gas mass, dust mass, stellar mass, and dynamical mass with the B-luminosity. Although all mass estimations increase with increasing luminosity, we find important deviations to the general trend in some objects, which seem to be the consequence of their particular evolutionary histories. The analysis of the mass-to-light ratios give similar results. We investigate the mass-metallicity relations and conclude that both the nature and the star-formation history are needed to understand the relationships between both properties. The majority of the galaxies follow a Schmidt-Kennicutt scaling law of star-formation that agrees with that reported in individual star-forming regions within M 51 but not with that found in normal spiral galaxies. Dwarf galaxies seem to be forming stars more efficiently than the outskirts of spiral galaxies. We find a relation between the reddening coefficient and the warm dust mass indicating that the extinction is mainly internal to the galaxies. The comparison with the closed-box model also indicates that the environment has strongly affected their evolution. Considering all multiwavelength data, we found that 17 up to 20 galaxies are clearly interacting or merging with low-luminosity dwarf objects or HI clouds. The remaining three galaxies (Mkn 5, SBS 1054+364, and SBS 1415+437) show considerable divergences of some properties when comparing with similar objects. Many of the interacting/merging features are only detected when deep optical spectroscopy and a detailed multiwavelength analysis, including HI observations, are obtained. We conclude that interactions do play a fundamental role in the triggering mechanism of the strong star-formation activity observed in dwarf starburst galaxies.

Abstract Copyright:

Journal keyword(s): galaxies: starburst - galaxies: interactions - galaxies: dwarf - galaxies: abundances - stars: Wolf-Rayet - galaxies: kinematics and dynamics

Simbad objects: 40

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Number of rows : 40
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 Mrk 960 bCG 00 48 35.430 -12 42 59.77   15.5       ~ 105 0
2 UGC 1809 G 02 20 53.4333807984 +00 33 24.391158372           ~ 20 1
3 IRAS F02183+0019 AGN 02 20 54.530 +00 33 24.46   16.50       ~ 58 1
4 NGC 1512 GiP 04 03 54.281 -43 20 55.86 11.30 11.43 10.54 10.37   ~ 396 1
5 2MASX J04493799+0319296 GiP 04 49 38.0038924872 +03 19 29.834360688   16.27 15.48     ~ 15 1
6 Mrk 1087 AGN 04 49 44.469 +03 20 02.67   15.49 15.04     ~ 76 1
7 2MFGC 4113 G 05 01 35.550 -04 15 47.42   15.35   14.73   ~ 62 0
8 HCG 31 CGG 05 01 37 -04 15.4           ~ 128 0
9 HCG 31e G 05 01 37.5 -04 15 57           ~ 25 0
10 NGC 1741 EmG 05 01 38.3 -04 15 25   13.7   13.02 13.6 ~ 266 0
11 HCG 31f1 PoG 05 01 39.71 -04 16 22.2           ~ 10 0
12 HCG 31f AG? 05 01 40.02 -04 16 22.4           ~ 21 0
13 IC 399 EmG 05 01 44.0604445128 -04 17 19.319048052   15.0 14.8     ~ 70 0
14 Mrk 5 H2G 06 42 15.53 +75 37 32.6   17.0       ~ 110 0
15 Mrk 1199 GiG 07 23 43.5303502320 +33 26 30.926307192   13.7 13.13     ~ 110 0
16 2MFGC 6625 EmG 08 23 54.9678898128 +28 06 21.581238276   15.5       ~ 70 0
17 2MASX J08382309+6507160 SBG 08 38 23.093 +65 07 16.05     14.16     ~ 129 1
18 LB 555 EmG 09 30 06.4773062016 +60 26 53.169485316   17.0       ~ 36 0
19 LEDA 26955 AG? 09 30 09.041 +60 28 05.37           ~ 46 0
20 SBSG 0926+606B GiP 09 30 09.6 +60 28 04   18.0       ~ 12 0
21 APG 252 IG 09 44.8 -19 41           ~ 12 0
22 ESO 566-7 IG 09 44 58.4 -19 43 32   15.36   14.66   ~ 15 0
23 ESO 566-8 Sy2 09 44 59.65 -19 42 45.6   15.56   14.59   ~ 30 0
24 LEDA 28398 EmG 09 51 31.7596930512 +52 59 35.987746452   18       ~ 44 0
25 ESO 436-42 Sy2 10 34 38.727 -28 34 59.80   14.44 14.41 13.26   ~ 56 0
26 HIPASS J1034-28 ClG 10 34.8 -28 29           ~ 7 0
27 ESO 215-9 AG? 10 57 29.90 -48 10 43.0   16.03   15.02 15.0 ~ 78 0
28 Z 184-40 AG? 10 57 47.0075966640 +36 15 38.824306272   15.5 16     ~ 42 1
29 6dFGS gJ115111.7-203557 H2G 11 51 11.7 -20 35 56   15.67   15.35   ~ 85 1
30 LEDA 39055 EmG 12 14 02.4588226248 +53 45 17.525587212   18       ~ 83 0
31 NGC 5113 AG? 13 21 22.57 +57 41 29.5   15.2       ~ 20 0
32 LEDA 2816050 G 13 21 22.6 +57 41 29   18.5       ~ 26 0
33 M 51 Sy2 13 29 52.698 +47 11 42.93   9.26 8.36 8.40   ~ 4329 4
34 M 83 SBG 13 37 00.91920 -29 51 56.7400 8.85 8.11 7.52 7.21   ~ 2572 2
35 NGC 5253 AGN 13 39 55.990 -31 38 24.11 11.48 10.94 10.49 10.33 13.47 ~ 1365 4
36 NGC 5408 EmG 14 03 20.907 -41 22 39.75   12.59   11.96 12.2 ~ 349 3
37 MCG+07-29-060 QSO 14 17 01.716 +43 30 13.52   15.6       ~ 172 0
38 ESO 513-11 PaG 15 00 27.10 -26 26 57.0   15.85       ~ 53 0
39 LEDA 71605 EmG 23 30 09.7 +25 31 56   15.0       ~ 54 0
40 HCG 31h G ~ ~           ~ 8 0

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