J/A+A/647/A195      Unknown active galactic nuclei study       (Giuliani+, 2021)

A new panchromatic classification of unclassified Burst Alert Telescope active galactic nuclei. Giuliani L., Ghisellini G., Sbarrato T. <Astron. Astrophys., 647, A195 (2021)> =2021A&A...647A.195G 2021A&A...647A.195G (SIMBAD/NED BibCode)
ADC_Keywords: Active gal. nuclei ; Energy distributions ; Gamma rays ; X-ray sources Keywords: radiation mechanisms: non-thermal - radiation mechanisms: thermal - galaxies: active - galaxies: jets - X-rays: general - galaxies: nuclei Abstract: We collect data at all frequencies for the new sources classified as unknown active galactic nuclei (AGNs) in the latest Burst Alert Telescope all-sky hard X-ray catalog. Focusing on the 36 sources with measured redshift, we compute their spectral energy distribution (SED) from radio to γ-rays with the aim to classify these objects. We apply emission models that attempt to reproduce the obtained SEDs, including: (i) a standard thin accretion disk together with an obscuring torus and a X-ray corona; (ii) a two temperature thick advection-dominated flow; (iii) an obscured AGN model, accounting for absorption along the line of sight at kiloelectronvolt energies and in the optical band; and (iv) a phenomenological model to describe the jet emission in blazar-like objects. We integrate the models with the SWIRE template libraries to account for the emission of the host galaxy. For every source we found a good agreement between data and our model. Considering that the sources were selected in the hard X-ray band, which is rather unaffected by absorption, we expected and found a large fraction of absorbed radio-quiet AGNs (31 out of 36) and some additional rare radio-loud sources (5 out of 36), since the jet emission in hard X-rays is important for aligned jets owing to the boost produced by the beaming effect. With our work we can confirm the hypothesis that a number of galaxies, whose optical spectra lack AGN emission features, host an obscured active nucleus. The approach we used proved to be efficient in rapidly identifying objects, which commonly used methods were not able to classify. Description: Considering that the sources are selected in the hard X-ray band, which is rather unaffected by absorption, we expected and found a relatively large fraction of absorbed radio-quiet AGNs and some more rare radio-loud sources. In fact, the jet emission in hard X-rays becomes important for aligned jets as a result of the boost produced by the beaming effect. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file table1.dat 125 31 Fit results for the sources SWIFT soft-X spectra table2.dat 124 5 Fit parameters for the unknown AGNs (phenomenological jet model with accretion disk) identified as blazars table3.dat 103 31 Fit parameters for unknown AGNs (obscured AGN emission model) table4.dat 37 36 BAT 105 unknown AGNs classification as results from our work -------------------------------------------------------------------------------- Byte-by-byte Description of file: table1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 18 A18 --- Source Source name (SWIFT JHHMM.m+DDSS) 20- 24 F5.3 --- z Source redshift 26- 29 F4.1 ks ttot ?=- Total exposure time 31- 36 F6.3 --- alpha0.3-2 ?=- Photon index in the 0.3-2keV band (1) 38- 43 F6.3 --- b_alpha0.3-2 ?=- Lower value of alpha0.3-2 interval 45- 50 F6.3 --- B_alpha0.3-2 ?=- Upper value of alpha0.3-2 interval 52- 59 E8.3 mW/m2 f0.3-2 ?=- Total flux in the 0.3-2keV band 61- 68 E8.3 mW/m2 b_f0.3-2 ?=- Lower value of f0.3-2 interval 70- 77 E8.3 mW/m2 B_f0.3-2 ?=- Upper value of f0.3-2 interval 79- 84 F6.3 --- alpha2-10 ?=- Photon index in the 2-10keV band (1) 86- 91 F6.3 --- b_alpha2-10 ?=- Lower value of alpha2-10 interval 93- 98 F6.3 --- B_alpha2-10 ?=- Upper value of alpha2-10 interval 100-107 E8.3 mW/m2 f2-10 ?=- Total flux in the 2-10keV 109-116 E8.3 mW/m2 b_f2-10 ?=- Lower value of f2-10 interval 118-125 E8.3 mW/m2 B_f2-10 ?=- Upper value of f2-10 interval -------------------------------------------------------------------------------- Note (1): The spectral indices alpha are defined as in Eq. (1). -------------------------------------------------------------------------------- Byte-by-byte Description of file: table2.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 18 A18 --- Source Source name (SWIFT JHHMM.m+DDMM) 20- 24 F5.2 --- CD Compton dominance ratio 26- 33 E8.3 10-7W nuLS Synchrotron peak luminosity in nuL(nu) 35- 38 F4.2 --- a1 a1 power-law slope 40- 43 F4.2 --- a2 a2 power-law slope 45- 48 F4.2 --- a3 a3 power-law slope 50- 56 E7.2 Hz nus Synchrotron peak frequency 58- 64 E7.2 Hz nuc Inverse-Compton peak frequency 66- 72 E7.2 Hz nucuts Cutoff frequency for low-energy spectra 74- 80 E7.2 Hz nucutc Cutoff frequency for high-energy spectra 82- 88 E7.2 Hz nuT Self-absorption frequency 90- 94 F5.2 --- ar Power-law slope for nu<nuT 96- 99 F4.2 Msun/yr dM/dt ?=- Accretion ratio 101-108 E8.3 Msun MBH ?=- Black hole mass (1) 110-113 F4.2 pc RT ?=- Obscuring torus radius (1) 115-118 F4.2 deg thetaT ?=- Obscuring torus covering angle (1) 120-124 F5.3 --- lEdd ?=- Accretion disk Eddington ratio (1) -------------------------------------------------------------------------------- Note (1): We only found the emission signature of an accretion disk in the first three objects. -------------------------------------------------------------------------------- Byte-by-byte Description of file: table3.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 18 A18 --- Source Source name (SWIFT JHHMM.m+DDMM) 20- 24 F5.2 Msun/yr dM/dt Accretion ratio 26- 33 E8.3 Msun M Black hole mass 35- 39 F5.3 --- lEdd Accretion disk Eddington ratio 41- 46 F6.2 pc RDB ?=- Dust belt radius 48- 51 F4.2 deg thetaDB ?=- Dust belt covering angle 53- 57 F5.2 pc RT Obscuring torus radius 59- 62 F4.2 deg thetaT Obscuring torus covering angle 64- 68 F5.3 --- f Intrinsic corona scattered component (as fraction of the total flux) 70- 77 E8.3 cm-2 NH Hydrogen column density 79- 86 E8.3 cm-2 NHgal Hydrogen column density from host galactic gas 88- 91 F4.2 --- gamma gamma X-ray corona power-law index 93- 97 F5.2 --- G G normalization coefficient for the galaxy emission template 99-103 F5.3 mag AB AB extinction at wavelength λB=0.44um -------------------------------------------------------------------------------- Byte-by-byte Description of file: table4.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 18 A18 --- Source Source name (SWIFT JHHMM.m+DDMM) 20- 37 A18 --- Class Classification -------------------------------------------------------------------------------- History: From electronic version of the journal
(End) Patricia Vannier [CDS] 31-May-2021
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