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Table 2.

Obtained properties for detected sources.

Galaxy 5 GHz peak flux 5 GHz integrated flux Right ascension/declination Uncertainties Tb Putative
(mJy beam−1) (mJy) (mas/mas) (K) core
First obs || Second obs First obs || Second obs
Mrk 0001 1.30 ± 0.09 || 1.05 ± 0.05 8.6 ± 0.8 || 8.9±0.3 0.018/0.017 0.39 ± 0.03 6.5 × 106 NW
Mrk 1210 0.92 ± 0.07 || 3.10 ± 0.07 15.05 ± 0.8 || 17.9 ± 0.7 0.0008/0.002 0.40 ± 0.01 1.3 × 107 CN
Mrk 1419 0.94 ± 0.06 || 0.66 ± 0.03 1.7 ± 0.2 || 0.7 ± 0.3 0.001/0.001 0.31 ± 0.09 >2.6 × 106
NGC 2273 1.6 ± 0.03 || … 3.3 ± 0.1 || … 0.0005/0.0006 0.11 ± 0.06 9.1 × 106
UGC 3193 0.7 ± 0.06 || 1.3 ± 0.03 2.0 ± 0.1 || 3.0 ± 0.9 0.0004/0.001 −0.14 ± 0.04 1.3 × 107 N

Notes. Column 1: name of galaxy. The sources in bold hold clean maser disks (see Sect. 2). Column 2: 5 GHz peak flux density of the brightest component. Column 3: 5 GHz integrated flux. For detected sources with multiple components the reported flux is the sum of the fluxes from all the components. Column 4: J2000 right ascension and declination obtained (except for NGC 2273) from the second observations for the peak position of the brightest component. Column 5: right ascension and declination uncertainties. Column 6: spectral index obtained from 33 GHz VLA observation and 5 GHz VLBA observations assuming a power law dependence of S ∝ να. Column 7: brightness temperatures. If the source is unresolved, a lower limit is given. Column 8: putative core of the AGN, corresponding to the component with highest brightness temperature. NW stands for northwestern, CN for central, and N for northern.

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