The 12CO J=4-3 to J=13-12 lines of the interstellar medium from nearby galaxies, newly observable with the Herschel SPIRE Fourier Transform Spectrometer (FTS), offer an opportunity to study warmer, more luminous molecular gas than that traced by 12CO
J=1-0. Here we present a survey of 17 nearby infrared-luminous galaxy systems (21 pointings). In addition to photometric modeling of dust, we modeled full 12CO spectral line energy distributions from J=1-0 to J=13-12 with two components of warm and cool CO gas, and included LTE analysis of [CI], [CII], [NII] and H2 lines. CO is emitted from a low-pressure/high-mass component traced by the low-J lines and a high-pressure/low-mass component which dominates the luminosity. We found that, on average, the ratios of the warm/cool pressure, mass, and 12CO luminosity are 60 +/- 30, 0.11 +/- 0.02, and 15.6 +/- 2.7. The gas-to-dust-mass ratios are < 120 throughout the sample. The 12CO luminosity is dominated by the high-J lines and is 4 $times 10^{-4}$ LFIR on average. We discuss systematic effects of single-component and multi-component CO modeling (e.g., single-component J < 3 models overestimate gas pressure by ~ 0.5 dex), as well as compare to Galactic star-forming regions. With this comparison, we show the molecular interstellar medium of starburst galaxies is not simply an ensemble of Galactic-type GMCs. The warm gas emission is likely dominated by regions resembling the warm extended cloud of Sgr B2.
We present new images of Arp 220 from the Atacama Large Millimeter/submillimeter Array with the highest combination of frequency (691 GHz) and resolution ($0.36 times 0.20^{primeprime}$) ever obtained for this prototypical ultraluminous infrared gala
xy. The western nucleus is revealed to contain warm (200 K) dust that is optically thick ($tau_{434mu m} = 5.3$), while the eastern nucleus is cooler (80 K) and somewhat less opaque ($tau_{434mu m} = 1.7$). We derive full-width half-maximum diameters of $ 76 times le 70$ pc and $123 times 79$ pc for the western and eastern nucleus, respectively. The two nuclei combined account for ($83 ^{+65}_{-38}$ (calibration) $^{+0}_{-34}$ (systematic))% of the total infrared luminosity of Arp 220. The luminosity surface density of the western nucleus ($ log(sigma T^4) = 14.3pm 0.2 ^{+0}_{-0.7}$ in units of L$_odot$ kpc$^{-2}$) appears sufficiently high to require the presence of an AGN or a hot starburst, although the exact value depends sensitively on the brightness distribution adopted for the source. Although the role of any central AGN remains open, the inferred mean gas column densities of $0.6-1.8 times 10^{25}$ cm$^{-2}$ mean that any AGN in Arp 220 must be Compton-thick.
We present the observations of the starburst galaxy M82 taken with the Herschel SPIRE Fourier Transform Spectrometer. The spectrum (194-671 {mu}m) shows a prominent CO rotational ladder from J = 4-3 to 13-12 emitted by the central region of M82. The
fundamental properties of the gas are well constrained by the high J lines observed for the first time. Radiative transfer modeling of these high-S/N 12CO and 13CO lines strongly indicates a very warm molecular gas component at ~500 K and pressure of ~3x10^6 K cm^-3, in good agreement with the H_2 rotational lines measurements from Spitzer and ISO. We suggest that this warm gas is heated by dissipation of turbulence in the interstellar medium (ISM) rather than X-rays or UV flux from the straburst. This paper illustrates the promise of the SPIRE FTS for the study of the ISM of nearby galaxies.
