1. The far-infrared/radio correlation and radio spectral index of galaxies in the SFR-M* plane up to z ~ 2.
- Author
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Magnelli, B., Ivison, R. J., Lutz, D., Valtchanov, I., Farrah, D., Berta, S., Bertoldi, F., Bock, J., Cooray, A., Ibar, E., Karim, A., Le Floc'h, E., Nordon, R., Oliver, S. J., Page, M., Popesso, P., Pozzi, F., Rigopoulou, D., Riguccini, L., and Rodighiero, G.
- Subjects
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FAR infrared lasers , *STELLAR mass , *STELLAR evolution , *REDSHIFT , *STELLAR luminosity function , *INFRARED astronomy , *RADIO astronomy - Abstract
We study the evolution of the radio spectral index and far-infrared/radio correlation (FRC) across the star-formation rate - stellarmasse (i.e. SFR-M*) plane up to z ~ 2.We start from a stellar-mass-selected sample of galaxies with reliable SFR and redshift estimates. We then grid the SFR-M* plane in several redshift ranges and measure the infrared luminosity, radio luminosity, radio spectral index, and ultimately the FRC index (i.e. qFIR) of each SFR-M*- z bin. The infrared luminosities of our SFR-M*- z bins are estimated using their stacked far-infrared flux densities inferred from observations obtained with the Herschel Space Observatory. Their radio luminosities and radio spectral indices (i.e. α, where Sv α v-α) are estimated using their stacked 1.4 GHz and 610MHz flux densities from the Very Large Array and Giant Metre-wave Radio Telescope, respectively. Our far-infrared and radio observations include the most widely studied blank extragalactic fields - GOODS-N, GOODS-S, ECDFS, and COSMOS - covering a total sky area of ~2.0 deg². Using this methodology, we constrain the radio spectral index and FRC index of star-forming galaxies with M* > 1010 M⊙ and 0 < z < 2.3. We find that α1.4 GHz610MHz does not evolve significantly with redshift or with the distance of a galaxy with respect to the main sequence (MS) of the SFR-M* plane (i.e. △log(SSFR)MS = log[SSFR(galaxy)/SSFRMS(M*, z)]). Instead, star-forming galaxies have a radio spectral index consistent with a canonical value of 0.8, which suggests that their radio spectra are dominated by non-thermal optically thin synchrotron emission. We find that the FRC index, qFIR, displays a moderate but statistically significant redshift evolution as qFIR(z) = (2.35±0.08)×(1+z)-0.12 ± 0.04, consistent with some previous literature. Finally, we find no significant correlation between qFIR and ?log(SSFR)MS, though a weak positive trend, as observed in one of our redshift bins (i.e. △[qFIR]/△[△log(SSFR)MS] = 0.22 ± 0.07 at 0.5 < z < 0.8), cannot be firmly ruled out using our dataset. [ABSTRACT FROM AUTHOR]
- Published
- 2015
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