2009ApJ...706.1527B


Query : 2009ApJ...706.1527B

2009ApJ...706.1527B - Astrophys. J., 706, 1527-1544 (2009/December-1)

High-mass star formation in normal late-type galaxies: observational constraints to the initial mass function.

BOSELLI A., BOISSIER S., CORTESE L., BUAT V., HUGHES T.M. and GAVAZZI G.

Abstract (from CDS):

We use Hα and far-ultraviolet (FUV, 1539 Å) Galaxy Evolution Explorer (GALEX) data for a large sample of nearby objects to study the high-mass (m≥ 2 M) star formation activity of normal late-type galaxies. The data are corrected for dust attenuation using the most accurate techniques available at present, namely the Balmer decrement for Hα data and the total far-infrared to FUV flux ratio for GALEX data. The sample shows a highly dispersed distribution in the Hα to FUV flux ratio (log f(Hα)/f(FUV) = 1.10±0.34 Å) indicating that two of the most commonly used star formation tracers give star formation rates (SFRs) with uncertainties up to a factor of 2-3. The high dispersion is partly due to the presence of active galactic nuclei, where the UV and the Hα emission can be contaminated by nuclear activity, highly inclined galaxies, for which the applied extinction corrections are probably inaccurate, or starburst galaxies, where the stationarity in the star formation history required for transforming Hα and UV luminosities into SFRs is not satisfied. Excluding these objects, normal late-type galaxies have log f(Hα)/f(FUV) = 0.94±0.16 Å, which corresponds to an uncertainty of ∼50% on the SFR. The Hα to FUV flux ratio of the observed galaxies increases with their total stellar mass. If limited to normal star-forming galaxies, however, this relationship reduces to a weak trend that might be totally removed using different extinction correction recipes. In these objects, the Hα to FUV flux ratio seems also barely related to the FUV - H color, the H-band effective surface brightness, the total star formation activity, and the gas fraction. The data are consistent with a Kroupa and Salpeter initial mass function (IMF) in the high-mass stellar range (m > 2 M) and imply, for a Salpeter IMF, that the variations of the slope γ cannot exceed 0.25, from γ = 2.35 for massive galaxies to γ = 2.60 in low luminosity systems. We show however that these observed trends, if real, can be due to the different micro-history of star formation in massive galaxies with respect to dwarf systems.

Abstract Copyright:

Journal keyword(s): galaxies: evolution - galaxies: fundamental parameters - galaxies: general - galaxies: spiral - H II regions - stars: formation

Simbad objects: 19

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Number of rows : 19
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 NAME Magellanic Stream HVC 00 32 -30.0           ~ 971 1
2 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17438 0
3 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2019 2
4 NGC 2798 GiP 09 17 22.9 +42 00 00 13.03 13.04 12.32     ~ 325 3
5 APG 283 PaG 09 17 26.99 +41 59 48.8   12.2       ~ 193 1
6 M 81 Sy2 09 55 33.1726556496 +69 03 55.062505368   7.89 6.94     ~ 4450 3
7 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 5861 6
8 NGC 3424 GiP 10 51 46.322 +32 54 02.44   13.2       ~ 163 1
9 NGC 3683 H2G 11 27 31.890 +56 52 36.15   12.7       ~ 187 0
10 NGC 4383 AGN 12 25 25.5 +16 28 12 12.41 12.67 12.12     ~ 253 1
11 NAME Virgo Cluster ClG 12 26 32.1 +12 43 24           ~ 6648 0
12 Mrk 772 GiG 12 32 33.5217697464 +09 10 24.875570172   15.4       ~ 81 0
13 NGC 4437 AGN 12 32 45.586 +00 06 54.14   11.1   11.1 10.6 ~ 285 0
14 M 90 Sy2 12 36 49.8009839880 +13 09 46.523813040 10.56 10.26 9.54     ~ 899 1
15 NGC 4631 GiP 12 42 08.009 +32 32 29.44   9.78 9.19 9.10   ~ 1095 2
16 NGC 5145 SBG 13 25 13.9112423568 +43 16 02.366691636   13.6       ~ 105 0
17 NGC 5348 GiP 13 54 11.254 +05 13 37.91   14.5       ~ 96 0
18 IC 1048 GiP 14 42 57.876 +04 53 24.46   14.0       ~ 104 0
19 NGC 7771 GiG 23 51 24.880 +20 06 42.57 13.42 13.08 12.25     ~ 338 4

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