Notes. Columns: (1) Source names corresponding to those in Figs. 1 and 2. (2) Epoch label corresponding to those specified in Table 1. Note that epoch EM and V5 are quasi-simultaneous. (3–4) Coordinates given with respect to α(J2000) = 13^h20^m000 and . Position uncertainties in mas, within parentheses, are given in terms of the full width at half maximum (FWHM) by FWHM/(2 × S/N), where S/N is the signal-to-noise ratio, and FWHM was taken as the projection of the beam major axis on both α and δ axes. (5) Peak intensity. We estimated the uncertainties by adding in quadrature the rms noise in the map (Col. 10 in Table 1) to a 5% uncertainty in the point-source flux density calibration. (6) Flux density. (7) Monochromatic luminosity at the observed frequency (Col. 5 in Table 1). (8) Deconvolved major and minor axes, obtained by fitting a Gaussian to each source. (9) Brightness temperature. When no deconvolved sizes could be obtained, we instead used the solid angle subtended by the synthesised beam for calculating lower limits of T_B, i.e., , where FWHM_M and FWHM_m are the major and minor synthesised beam-fitted FWHM (Col. 9 in Table 1), respectively.