Dust temperature and CO  →  H2 conversion factor variations in the SFR-M∗ plane

• Published in: Astronomy and astrophysics (Berlin) Vol. 548
• Main Authors: Magnelli, B., Saintonge, A., Lutz, D., Tacconi, L. J., Berta, S., Bournaud, F., Charmandaris, V., Dannerbauer, H., Elbaz, D., Förster-Schreiber, N. M., Graciá-Carpio, J., Ivison, R., Maiolino, R., Nordon, R., Popesso, P., Rodighiero, G., Santini, P., Wuyts, S.
• Format: Journal Article
• Language: English
• Published: Les Ulis EDP Sciences 01.12.2012
• Subjects: Astronomy; Earth, ocean, space; Exact sciences and technology; galaxies: evolution; galaxies: starburst; infrared: galaxies; Blackbody; Galaxy evolution; galaxies: starburst; Critical value; infrared: galaxies; Starburst galaxies; galaxies: evolution; Luminosity; Star formation; Metallicity; Classification; Infrared galaxies; Models; Gas to dust ratio
• ISSN: 0004-6361; 1432-0746
• DOI: 10.1051/0004-6361/201220074

Deep Herschel PACS/SPIRE imaging and 12CO(2−1) line luminosities from the IRAM Plateau de Bure Interferometer are combined for a sample of 17 galaxies at z > 1 from the GOODS-N field. The sample includes galaxies both on and above the main sequence (MS) traced by star-forming galaxies in the SFR-M∗ plane. The far-infrared data are used to derive dust masses, Mdust, following the Draine & Li (2007, ApJ, 657, 810) models. Combined with an empirical prescription for the dependence of the gas-to-dust ratio on metallicity (δGDR(μ0)), the CO luminosities and Mdust values are used to derive for each galaxy the CO-to-H2 conversion factor, αCO. Like in the local Universe, the value of αCO is a factor of  ~5 smaller in starbursts compared to normal star-forming galaxies (SFGs). We additionally uncover a relation between αCO and dust temperature (Tdust; αCO decreasing with increasing Tdust) as obtained from modified blackbody fits to the far-infrared data. While the absolute normalization of the αCO(Tdust) relation is uncertain, the global trend is robust against possible systematic biases in the determination of Mdust, δGDR(μ0) or metallicity. Although we cannot formally distinguish between a step and a smooth evolution of αCO with the dust temperature, we can unambiguously conclude that in galaxies of near-solar metallicity, a critical value of Tdust = 30 K can be used to determine whether the appropriate αCO is closer to the “starburst” value (1.0 M⊙ (K km s-1 pc2)-1, when Tdust > 30 K) or closer to the Galactic value (4.35 M⊙ (K km s-1 pc2)-1, when Tdust < 30 K). This indicator has the great advantage of being less subjective than visual morphological classifications of mergers/SFGs, which can be difficult at high z because of the clumpy nature of SFGs. Using Tdust to select the appropriate αCO is also more indicative of ISM conditions than a fixed LIR criterion. In the absence of far-infrared data, the offset of a galaxy from the star formation main sequence (i.e., Δlog (SSFR)MS = log  [SSFR(galaxy)/SSFRMS(M∗,z)]) can be used to identify galaxies requiring the use of an αCO conversion factor lower than the Galactic value (i.e., when Δlog (SSFR)MS ≳ 0.3 dex).