Abstract

We present Herschel SPIRE-FTS observations of the Antennae (NGC 4038/39), a well studied, nearby (2222 Mpc) ongoing merger between two gas rich spiral galaxies. We detect 5 CO transitions (J=43J=4-3 to J=87J=8-7), both [CI] transitions and the [NII]205μm205\mu m transition across the entire system, which we supplement with ground based observations of the CO J=10J=1-0, J=21J=2-1 and J=32J=3-2 transitions, and Herschel PACS observations of [CII] and [OI]63μm63\mu m. Using the CO and [CI] transitions, we perform both a LTE analysis of [CI], and a non-LTE radiative transfer analysis of CO and [CI] using the radiative transfer code RADEX along with a Bayesian likelihood analysis. We find that there are two components to the molecular gas: a cold (Tkin1030T_{kin}\sim 10-30 K) and a warm (Tkin100T_{kin} \gtrsim 100 K) component. By comparing the warm gas mass to previously observed values, we determine a CO abundance in the warm gas of xCO5×105x_{CO} \sim 5\times 10^{-5}. If the CO abundance is the same in the warm and cold gas phases, this abundance corresponds to a CO J=10J=1-0 luminosity-to-mass conversion factor of $\alpha_{CO} \sim 7 \ M_{\odot}{pc^{-2} \ (K \ km \ s^{-1})^{-1}}inthecoldcomponent,similartothevaluefornormalspiralgalaxies.WeestimatethecoolingfromH in the cold component, similar to the value for normal spiral galaxies. We estimate the cooling from H_2,[CII],COand[OI], [CII], CO and [OI]63\mu mtobe to be \sim 0.01 L_{\odot}/M_{\odot}.WecomparePDRmodelstotheratioofthefluxofvariousCOtransitions,alongwiththeratiooftheCOfluxtothefarinfraredfluxinNGC4038,NGC4039andtheoverlapregion.WefindthatthedensitiesrecoveredfromournonLTEanalysisareconsistentwithabackgroundfarultravioletfieldofstrength. We compare PDR models to the ratio of the flux of various CO transitions, along with the ratio of the CO flux to the far-infrared flux in NGC 4038, NGC 4039 and the overlap region. We find that the densities recovered from our non-LTE analysis are consistent with a background far-ultraviolet field of strength G_0\sim 1000$. Finally, we find that a combination of turbulent heating, due to the ongoing merger, and supernova and stellar winds are sufficient to heat the molecular gas.Comment: 50 pages, 15 figures, 8 tables, Accepted for publication in The Astrophysical Journa

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