2011A&A...525A..92P

The Great Nebula in Carina is one of the most massive (M_*,total>25000M_☉) star-forming complexes in our Galaxy and contains several stars with (initial) masses exceeding ≃100M_☉; it is therefore a superb location in which to study the physics of violent massive star-formation and the resulting feedback effects, including cloud dispersal and triggered star-formation. We aim to reveal the cold dusty clouds in the Carina Nebula complex, to determine their morphology and masses, and to study the interaction of the luminous massive stars with these clouds. We used the Large APEX Bolometer Camera LABOCA at the APEX telescope to map a 1.25°x1.25° (=50x50pc²) region at 870µm with 18'' angular resolution (=0.2pc at the distance of the Carina Nebula) and an rms noise level of ≃20mJy/beam. From a comparison to Hα images we infer that about 6% of the 870µm flux in the observed area is likely free-free emission from the HII region, while about 94% of the flux is very likely thermal dust emission. The total (dust + gas) mass of all clouds for which our map is sensitive is ∼60000M_☉, in good agreement with the mass of the compact clouds in this region derived from ¹³CO line observations. There is a wide range of different cloud morphologies and sizes, from large, massive clouds with several 1000M_☉, to small diffuse clouds containing just a few M_☉. We generally find good agreement in the cloud morphology seen at 870µm and the Spitzer 8µm emission maps, but also identify a prominent infrared dark cloud. Finally, we construct a radiative transfer model for the Carina Nebula complex that reproduces the observed integrated spectral energy distribution reasonably well. Our analysis suggests a total gas + dust mass of about 200000M_☉ in the investigated area; most of this material is in the form of molecular clouds, but a widely distributed component of (partly) atomic gas, containing up to ∼50% of the total mass, may also be present. Currently, only some 10% of the gas is in sufficiently dense clouds to be immediately available for future star formation, but this fraction may increase with time owing to the ongoing compression of the strongly irradiated clouds and the expected shockwaves of the imminent supernova explosions.