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Table 1:

The parsec-scale structure of Arp 299-A as imaged with the EVN.

Source
Source $\Delta~\alpha$a $\Delta~\delta$a Angular sizeb S1.7 ($\mu $Jy) c S5.0 ($\mu $Jy)c Spectral index
name type (J2000.0) (J2000.0) (milliarcsec)     $\alpha_{1.7}^{5.0}$
A0 SN 33.6213 46.707 $\leq$ $ 4.1\times4.0$ $\leq$75 $307 \pm 27$ $\geq$1.28
A1 AGN (core) 33.6199 46.699 $\leq$ $6.1\times 2.7$ $822 \pm 48$ $716 \pm 42$ - $0.13 \pm 0.11$
A1b AGN (jet) 33.6190 46.699 $\leq$ $10.1\times 5.1$ $314 \pm 30$ $\leq$66 $\leq$-1.42
A1c AGN (jet) 33.6183 46.695 $\leq$ $14.3 \times 6.2$ $267 \pm 28$ $\leq$66 $\leq$-1.27
A5 AGN (jet) 33.6176 46.694 $\leq$ $6.9 \times 5.0$ $246 \pm 28$ $183 \pm 24$ - $0.27 \pm 0.22$

Notes. (a) Coordinates are given with respect to $\alpha$ = 11:28:00.0000 and $\delta$ = 58:33:00.000, and the typical uncertainty is less than 1 mas; (b) upper limits to the deconvolved angular size (Major axis $\times$ Minor axis, in mas) as obtained using task IMFIT within AIPS, using our 5.0 GHz for all components but A1b and A1c, which were only detected at 1.7 GHz; (c) the uncertainty in the reported flux density (and derived spectral index) for the detected compact components corresponds to 1$\sigma$, where $\sigma$ was determined by adding in quadrature the off-source rms in each image and a 5% of the local maxima, to conservatively account for possible inaccuracies in the EVN calibration. Upper limits for undetected sources are three times the off-source rms.


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