J/A+A/621/A139      VLA-COSMOS 3GHz sources average radio SED   (Tisanic+, 2019)

The VLA-COSMOS 3 GHz Large Project: Average radio spectral energy distribution of highly star-forming galaxies. Tisanic K., Smolcic V., Delhaize J., Novak M., Intema H., Delvecchio I., Schinnerer E., Zamorani G., Bondi M., Vardoulaki E. <Astron. Astrophys. 621, A139 (2019)> =2019A&A...621A.139T 2019A&A...621A.139T (SIMBAD/NED BibCode)
ADC_Keywords: Galaxies, radio ; Radio continuum Keywords: galaxies: evolution - galaxies: statistics - radio continuum: galaxies - galaxies: star formation Abstract: We construct the average radio spectral energy distribution (SED) of highly star-forming galaxies (HSFGs) up to z∼4. Infrared and radio luminosities are bound by a tight correlation that is defined by the so-called q parameter. This infrared-radio correlation provides the basis for the use of radio luminosity as a star-formation tracer. Recent stacking and survival analysis studies find q to be decreasing with increasing redshift. It was pointed out that a possible cause of the redshift trend could be the computation of rest-frame radio luminosity via a single power-law assumption of the star-forming galaxies' (SFGs) SED. To test this, we constrained the shape of the radio SED of a sample of HSFGs. To achieve a broad rest-frame frequency range, we combined previously published Very Large Array observations of the COSMOS field at 1.4GHz and 3GHz with unpublished Giant Meterwave Radio Telescope (GMRT) observations at 325MHz and 610MHz by employing survival analysis to account for non-detections in the GMRT maps. We selected a sample of HSFGs in a broad redshift range (z∈[0.3,4], SFR≥100M/yr) and constructed the average radio SED. By fitting a broken power-law, we find that the spectral index changes from σ1=0.42±0.06 below a rest-frame frequency of 4.3GHz to σ2=0.94±0.06 above 4.3GHz. Our results are in line with previous low-redshift studies of HSFGs (SFR>10M/yr) that show the SED of HSFGs to differ from the SED found for normal SFGs (SFR<10M_☉/yr). The difference is mainly in a steeper spectrum around 10GHz, which could indicate a smaller fraction of thermal free-free emission. Finally, we also discuss the impact of applying this broken power-law SED in place of a simple power-law in K-corrections of HSFGs and a typical radio SED for normal SFGs drawn from the literature. We find that the shape of the radio SED is unlikely to be the root cause of the q-z trend in SFGs. Description: The table of cross-matched fluxes in the COSMOS field for the analysis presented in the paper. The flux densities at 325MHz, 610MHz, 1.4GHz and 3GHz are given in uJy and are rounded to 1uJy (which is less than the respective RMS values). The fluxes are given without errors, since the errors were not used in the analysis and will be published separately in the 325MHz and 610MHz catalogs. In case a source was not detected at 325MHz or 610MHz, the value given in the table is 5x the local RMS value at its position. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file matched.dat 55 306 Table of cross-matched fluxes -------------------------------------------------------------------------------- See also: J/ApJS/188/384 : The VLA-COSMOS survey. IV. (Schinnerer+, 2010) J/A+A/602/A1 : VLA-COSMOS 3 GHz Large Project (Smolcic+, 2017) Byte-by-byte Description of file: matched.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 10 A10 --- --- [COSMOSVLA3] 12- 30 A19 --- COSMOSVLA3 VLA-COSMOS name of the source, JHHMMSS.ss+DDMMSS.s 32- 35 I4 uJy F325MHz 325MHz flux density 36- 39 A4 --- l_F325MHz [Det Ulim] Detection or upper limit at 325MHz 41- 43 I3 uJy F610MHz 610MHz flux density 44- 47 A4 --- l_F610MHz [Det Ulim] Detection or upper limit at 610MHz 49- 51 I3 uJy F1.4GHz 1.4GHz flux density (1) 53- 55 I3 uJy F3GHz 3 GHz flux density (2) -------------------------------------------------------------------------------- Note (1): Flux densities from Schinnerer et al. (2010, Cat. J/ApJS/188/384) Note (2): Flux densities from Smolcic et al. (2017, Cat. J/A+A/602/A1) -------------------------------------------------------------------------------- Acknowledgements: Kresimir Tisanic, ktisanic(at)phy.hr
(End) Patricia Vannier [CDS] 30-Nov-2018
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