J/A+A/692/A205        The putative center in NGC 1052            (Baczko+, 2024)

The putative center in NGC 1052. Baczko A.-K., Kadler M., Ros E., Fromm M. C., Wielgus M., Perucho M., Krichbaum P. T., Balokovic M., Blackburn L., Chan C., Issaoun S., Janssen M., Ricci L., Event Horizon Telescope Collaboration <Astron. Astrophys. 692, A205 (2024)> =2024A&A...692A.205B 2024A&A...692A.205B (SIMBAD/NED BibCode)
ADC_Keywords: Galaxies ; Radio continuum Keywords: methods: observational - techniques: high angular resolution - techniques: interferometric - galaxies: active - galaxies: jets - galaxies: Seyfert Abstract: Many active galaxies harbor powerful relativistic jets. The detailed mechanisms of their formation and acceleration remain poorly understood. To investigate the area of jet acceleration and collimation with the highest available angular resolution we have studied the innermost region of the bipolar jet in the nearby LINER galaxy NGC 1052. We combined observations of NGC 1052 taken with the VLBA, the GMVA and the EHT during one week in spring 2017. Our study focuses on the size and continuum spectrum of the innermost region containing the central engine and the footpoints of both jets. We employ a synchrotron-self absorption model to fit the continuum radio spectrum and combine size measurements from close to the central engine out to ∼1pc to study jet collimation. For the first time NGC 1052 was detected with the EHT, providing a size of the central region in-between both jet bases of 43uas perpendicular to the jet axes, corresponding to just around 250 RS (Schwarzschild radii). This size estimate supports previous studies of the jets expansion profile which suggest two breaks of the profile at around 3x103RS and 1x104RS distances to the core. Furthermore, we estimate the magnetic field to be 1.25 Gauss at a distance of 22uas from the central engine by fitting a synchrotron-self absorption spectrum to the innermost emission feature, which shows a spectral turn-over at ∼130GHz. Assuming a purely poloidal magnetic field this implies an upper limit on the magnetic field strength at the event horizon of 2.6x104Gauss, which is consistent with previous measurements. The complex and low brightness, double-sided jet structure in NGC 1052 makes it challenging to detect the source at millimeter wavelength. However, our first EHT observations demonstrated that detection is possible up to at least 230GHz. This enabled us to glimpse through the dense surrounding torus into the innermost central region where the jets are formed, to finally resolve this region and to give improved constraints on its expansion and magnetic field strength. Description: We provide here fits images and tables of model fit components from VLBI observations of NGC 1052: Fig. 2, the clean radio image of NGC 1052 at 86GHz observed with the GMVA. Table B contains the model fit parameters and uncertainties of 1.6, 5.0, 8.4, 15.3, 22.2, and 43.1GHz VLBA and 86 GHz GMVA observations. Objects: -------------------------------------------------------- RA (2000) DE Designation(s) -------------------------------------------------------- 02 41 04.79 -08 15 20.7 NGC 1052 = MCG-01-07-034 -------------------------------------------------------- File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tableb.dat 84 92 Fit parameters and uncertainties of 1.6, 5.0, 8.4, 15.3, 22.2, and 43.1GHz VLBA and 86 GHz GMVA observations list.dat 105 1 Information on fits image fits/* . 1 fits image -------------------------------------------------------------------------------- Byte-by-byte Description of file: tableb.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 7 A7 --- ID ID of component 9- 13 F5.2 GHz Freq Observing Frequency (1.55, 4.98, 8.42, 15.26, 22.22, 43.12 and 86.25) 15- 20 F6.2 mJy SFreq Flux density at Freq 22- 27 F6.2 mas oRA Offset in right ascension (1) 29- 32 F4.2 mas e_oRA oRA error 34- 39 F6.2 mas oDE Offset in declination (1) 41- 44 F4.2 mas e_oDE oDE error 46- 50 F5.2 mas Major Major axis 52- 55 F4.2 mas e_Major Major axis error 57- 62 F6.2 --- Ratio ? Ratio major to minor axis 64- 69 F6.2 mas Dist Component angular distance 71- 76 F6.2 mas e_Dist ? Angular distance error 79 A1 --- l_logTb Limit flag on logTb 80- 84 F5.2 [K] logTb Logarithm of brightness temperature -------------------------------------------------------------------------------- Note (1): Offsets from the 43 GHz map reference position RA = 02:41:04.799, DE = -08:15:20.752 -------------------------------------------------------------------------------- Byte-by-byte Description of file: list.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 F9.5 deg RAdeg Right Ascension of center (J2000) 10- 18 F9.5 deg DEdeg Declination of center (J2000) 20- 22 I3 --- Nx Number of pixels along X-axis 24- 26 I3 --- Ny Number of pixels along Y-axis 28- 37 A10 "datime" Obs.date Observation date 39- 45 F7.4 GHz Freq Observed frequency 47- 50 I4 Kibyte size Size of FITS file 52- 64 A13 --- FileName Name of FITS file, in subdirectory fits 66-105 A40 --- Title Title of the FITS file -------------------------------------------------------------------------------- Acknowledgements: Anne-Kathrin Baczko, baczko(at)chalmers.se
(End) Anne-Kathrin Baczko [Chalmers, Sweden], Patricia Vannier [CDS] 02-Oct-2024
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