J/A+A/686/A43          LOFAR-eFEDS value-added catalogue            (Igo+, 2024)

The LOFAR - eFEDS survey: The incidence of radio and X-ray AGN and the disk-jet connection. Igo Z., Merloni A., Hoang D., Buchner J., Liu T., Salvato M., Arcodia R., Bellstedt S., Bruggen M., Croston J.H., de Gasperin F., Georgakakis A., Hardcastle M.J., Nandra K., Ni Q., Pasini T., Shimwell T., Wolf J. <Astron. Astrophys. 686, A43 (2024)> =2024A&A...686A..43I 2024A&A...686A..43I (SIMBAD/NED BibCode)
ADC_Keywords: X-ray sources ; Photometry, SDSS ; Photometry, infrared Keywords: galaxies: active - galaxies: jets Abstract: Radio jets are present in a diverse sample of AGN. However, the mechanisms of jet powering are not fully understood, and it remains unclear to what extent they obey mass-invariant scaling relations similar to those found for the triggering and fuelling of X-ray-selected AGN. We use the multi-wavelength data in the eFEDS field observed by eROSITA/Spectrum-Roentgen-Gamma (SRG) and LOFAR to study the incidence of X-ray and radio AGN as a function of several stellar mass (M*)-normalised AGN power indicators. From the LOFAR-eFEDS survey, we defined a new sample of radio AGN, with optical counterparts from Legacy Survey DR9, according to a radio-excess relative to their host star formation rate. We further divided the sample into compact and complex radio morphologies. In this work, we used the subset matching to the well-characterised, highly complete spectroscopic GAMA09 galaxies (0<z<0.4). We release this value-added LOFAR-eFEDS catalogue. We calculated the fraction of GAMA09 galaxies hosting radio, X-ray, and both radio and X-ray AGN as functions of the specific black hole kinetic (lambdaJet) and radiative (lambdaEdd) power. Despite the soft-X-ray eROSITA-selected sample, the incidence of X-ray AGN as a function of lambdaEdd shows the same mass-invariance and power law slope (-0.65) as that found in previous studies once corrected for completeness. Across the M* range probed, the incidence of compact radio AGN as a function of lambdaJet is described by a power law with constant slope, showing that it is not only high mass galaxies hosting high power jets and vice versa. This slope is steeper than that of the X-ray incidence, which has a value of around ∼1.5. Furthermore, higher-mass galaxies are more likely to host radio AGN across the lambdaJet range, indicating some residual mass dependence of jet powering. Upon adding complex radio morphologies, including 34 FRIIs, three of which are giant radio galaxies, the incidence not only shows a larger mass dependence but also a jet power dependence, being clearly boosted at high lambdaJet values. Importantly, the latter effect cannot be explained by such radio AGN residing in more dense environments (or more massive dark matter haloes). The similarity in the incidence of quiescent and star-forming radio AGN reveals that radio AGN are not only found in "red and dead" galaxies. Overall, our incidence analysis reveals some fundamental statistical properties of radio AGN samples, but highlights open questions regarding the use of a single radio luminosity-jet power conversion. We explore how different mass and accretion rate dependencies of the incidence can explain the observed results for varying disk-jet coupling models. Description: The LOFAR-eFEDS value added catalogue contains the 36631 LOFAR 144MHz detected radio sources in the eROSITA/eFEDS field (only 'inArea90', i.e. where the vignetted exposure time exceeds 500s). Legacy Survey DR9 optical counterparts are available, as well as host galaxy information from the GAMA09 survey (e.g. spectroscopic redshift, stellar mass, star formation rate) for those sources with counterparts in these catalogues. All (mass-complete) radio AGN in the GAMA09 field (flagged as 'G9_radioAGN') have been visually inspected to verify their counterpart association and their radio morphology. This subsample forms the basis of the work in the paper. 'FRII_flag' can be used to identify sources with FRII morphology; 'GRG_flag' can be used to identify giant radio galaxies. 'G9radioXraysources' mark the subset of radio sources which also have an eROSITA/eFEDS X-ray counterpart. For further information, see Appendix A of the paper. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file catalog.dat 377 36631 LOFAR-eFEDS value-added catalogue -------------------------------------------------------------------------------- See also: J/MNRAS/474/3875 : Galaxy And Mass Assembly (GAMA): DR3 (Baldry+, 2018) J/A+A/598/A104 : LOFAR Two-metre Sky Survey (Shimwell+, 2017) J/A+A/622/A1 : LOFAR Two-metre Sky Survey DR1 source catalog (Shimwell+, 2019) J/A+A/648/A2 : LOFAR Two-metre Sky Survey Deep Fields DR1 (Sabater+, 2021) J/A+A/648/A3 : LOFAR Two-metre Sky Survey Deep Fields DR1 (Kondapally+, 2021) J/A+A/659/A1 : LOFAR Two-metre Sky Survey (LoTSS) DR2 (Shimwell+, 2022) J/A+A/674/A119 : LoTTS Deep Fields ELAIS-N1 (Snidaric+, 2023) J/A+A/661/A1 : The eFEDS X-ray catalogs (V7.4) (Brunner+, 2022) Byte-by-byte Description of file: catalog.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 5 I5 --- LOFAR LOFAR unique number that identifies the source (LOFARSourceid) 7- 15 F9.5 deg RAdeg LOFAR Right ascension of the source (J2000) (for the equinox of the image) (LOFAR_RA) 17- 25 F9.5 deg DEdeg LOFAR Declination of the source (J2000) (for the equinox of the image) (LOFAR_DEC) 27- 38 F12.8 Jy Ftot LOFAR Total, integrated Stokes I flux density of the source at the reference frequency 144MHz (LOFARTotalflux) 40- 50 F11.9 Jy e_Ftot 1σ error on the total flux density of the source (LOFARETotal_flux) 52- 62 F11.6 Jy/beam Fpeak ?=- LOFAR Peak Stokes I flux density per beam of the source at 144MHz (LOFARPeakflux) 64- 74 F11.9 Jy/beam e_Fpeak ?=- 1σ error on the peak flux density per beam of the source (LOFAREPeak_flux) 76- 85 F10.8 deg Maj LOFAR FWHM of the major axis of the source (LOFAR_Maj) 87- 95 F9.6 arcsec epos LOFAR Positional error (LOFARposerr) 97 I1 --- scodeS [0/1] LOFAR Morphology Flag (LOFARscodeSflag) (1) 99 I1 --- Fluxratio [0/1] LOFAR Morphology Flag (LOFARfluxratioflag) (2) 101 I1 --- f_Maj [0/1] LOFAR Morphology Flag (LOFARmajflag) (3) 103 I1 --- Isolated [0/1] LOFAR Morphology Flag (LOFARisolatedflag) (4) 105 I1 --- Compact [0/1] LOFAR Morphology Flag (LOFARcompactflag) (5) 107-117 A11 --- LS9 Legacy Survey DR9 Unique source identifier, NNNNNN_NNNN (LS9UNIQUEOBJID) 119-121 A3 --- LS9Type LS9 Morphological model (LS9_TYPE) 123-131 F9.5 deg RALdeg ?=- LS9 Right ascension (J2000) (LS9_RA) 133-141 F9.5 deg DELdeg ?=- LS9 Declination (J2000) (LS9_DEC) 143-153 F11.9 arcsec ePosL ?=- LS9 Positional error (LS9poserr) 155-162 F8.4 mag g0mag ?=- LS9 De-reddened g-band magnitude (LS9magg_dered) 164-171 F8.4 mag r0mag ?=- LS9 De-reddened r-band magnitude (LS9magr_dered) 173-180 F8.4 mag z0mag ?=- LS9 De-reddened z-band magnitude (LS9magz_dered) 182-189 F8.4 mag W10mag ?=- LS9 De-reddened W1-band magnitude (LS9magW1_dered) 191-198 F8.4 mag W20mag ?=- LS9 De-reddened W2-band magnitude (LS9magW2_dered) 200-207 F8.4 mag W30mag ?=- LS9 De-reddened W2-band magnitude (LS9magW3_dered) 209-216 F8.4 mag W40mag ?=- LS9 De-reddened W4-band magnitude (LS9magW4_dered) 218-226 F9.6 arcsec Sep ?=- Separation between LOFAR source and best-match LS9 counterpart (CTP_Separation) 228-235 F8.6 --- pi [0/1]?=- Probability for the counterpart to be the correct one (p_i) 237-244 F8.6 --- pany [0/1]?=- Probability for a source to have any counterpart in the search region, optimal: pany>0.06 (p_any) 246-260 I15 --- GAMAID ?=- GAMA09 Unique GAMA ID of object, (uberID) 262-268 I7 --- CATAID ?=- GAMA09 Unique numeric GAMA object identifier (CATAID) 270-278 F9.5 deg RAcdeg ?=- Right Ascension of flux-weighted centre (ICRS) (RAcen) 280-288 F9.5 deg DEcdeg ?=- Declination of flux-weighted centre (ICRS) (Deccen) 290-296 F7.5 --- zsp ?=- Spectroscopic redshift (Z) 298-309 E12.6 Msun Mass50 ?=- Median stellar mass from MCMC chain (StellarMass_50) 311-322 E12.6 Msun Mass16 ?=- 16th percentile stellar mass from MCMC chain (StellarMass_16) 324-335 E12.6 Msun Mass84 ?=- 84th percentile stellar mass from MCMC chain (StellarMass_84) 337-343 F7.3 Msun/yr SFR50 ?=- Median SFR from MCMC chain (SFR_50) 345-351 F7.3 Msun/yr SFR16 ?=- 16th percentile SFR from MCMC chain (SFR_16) 353-359 F7.3 Msun/yr SFR84 ?=- 84th percentile SFR from MCMC chain (SFR_84) 361 I1 --- SC [6/8]? Science sample class SC≥6 is used her (SC) 363 I1 --- RadioAGN [0/1] 1 if LOFAR source (with SNR>5, pany>0.06) fulfils radio-excess criterion (radioAGN_flag) 365 I1 --- visInsp [0/1] 1 if source has been visually inspected (vis_inspected) 367 I1 --- G9radioAGN [0/1] Final sample of mass-complete G9 radio AGN, with visual inspection results applied (G9_radioAGN) 369-371 F3.1 --- FRII [0/1] 1, 0.5, 0: secure, likely, unlikely FRII-morphology, respectively (FRII_flag) 373 I1 --- GRG [0/1] Giant radio galaxy flag (largest linear size >0.7Mpc (GRG_flag) 375 I1 --- G9RXr [0/1] 1 if the LOFAR source has an X-ray match in eROSITA eFEDS (G9radioXraysources) 377 I1 --- Special [0/1] 1 if source required special cross-matching and/or property estimation (special_flag) -------------------------------------------------------------------------------- Note (1): scodeS flag as follows: 1 = LOFARScode=S, i.e. fit with only a single Gaussian by PyBDSF Note (2): Fluxratio flag as follows: 1 = LOFARTotalFlux/LOFARPeakFlux<3.6 Note (3): f_Maj flag as follows: 1 = LOFAR_Maj<19.1arcsec Note (4): Isolated flag as follows: 1 = no nearest neighbours within 45arcsec Note (5): Compact flag as follows: 1 = compact source; all four flags above are 1 0 = complex source -------------------------------------------------------------------------------- Acknowledgements: Zsofi Igo, zigo(at)mpe.mpg.de
(End) Patricia Vannier [CDS] 21-Feb-2024
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