Table 1.
Observational details.
(1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | (10) | (11) | (12) |
---|---|---|---|---|---|---|---|---|---|---|---|
Observation | Antennas | Bandwidth | Spectral | Source | Restoring | Position | Peak | rms (a) | σs.−n.(b) | Pl(c) | Polarization |
date | channels | name | beam size | angle | intensity (I) | angle | |||||
(MHz) | (mas × mas) | (°) | (![]() |
(![]() |
(![]() |
(%) | (°) | ||||
17 June 2014 | Ef, On, Nt, Tr, Ys, Mh | 4 | 2048 | W75N(B) | 1.1 × 0.8 | −60.02 | – (d) | 13 | 25 | – (d) | – (d) |
J2040+4527 (e) | 1.1 × 0.7 | −62.40 | 0.029 | 0.6 | – | – | – | ||||
J2202+4216 (f) | 1.5 × 0.8 | −52.68 | 1.868 | 2.5 | – | 7.0 | −64 ± 8 (g) | ||||
12 June 2016 | Ef, Jb, Mc, Nt, Sr, Ys, | 4 | 2048 | W75N(B) | 1.9 × 1.2 | −86.02 | – (h) | 11 | 73 | – (h) | – (h) |
Mh | J2040+4527 (e) | 1.0 × 0.7 | −86.84 | 0.026 | 0.7 | – | – | – | |||
J2202+4216 (f) | 1.5 × 1.0 | +74.56 | 0.685 | 1.5 | – | 3.1 | −61 ± 12 (i) | ||||
3C48 (j) | 1.5 × 0.9 | −59.93 | 0.016 | 1.1 | – | < 21 (k) | − | ||||
09 June 2018 | Ef, Jb, Mc, On, Nt, Tr, | 8 | 4096 | W75N(B) | 1.2 × 1.0 | +86.92 | – (l) | 14 | 28 | – (l) | – (l) |
Sr, Ys, Mh | J2040+4527 (e) | 1.1 × 0.8 | −79.82 | 0.021 | 0.4 | – | – | – | |||
J2202+4216 (f) | 1.2 × 0.8 | −61.91 | 0.765 | 1.7 | – | 4.0 | +5 ± 1 (m) | ||||
3C48 (j) | 1.8 × 0.7 | −42.47 | 0.125 | 0.5 | – | 4.2 | −70 ± 1 | ||||
25 Oct. 2020 | Ef, Jb, Mc, On, Tr, Sr, | 8 | 4096 | W75N(B) | 1.4 × 1.0 | −53.96 | – (n) | 13 | 12 | – (n) | – (n) |
Ys, Mh | J2040+4527 (e) | 1.3 × 0.9 | −56.63 | 0.034 | 0.6 | – | – | – | |||
J2202+4216 (f) | 1.6 × 1.0 | −75.93 | 1.011 | 2.2 | – | 3.8 | +15 ± 1 (m) | ||||
3C48 (j) | 2.2 × 1.1 | −38.84 | 0.027 | 0.3 | – | 6.4 | −70 ± 1 |
Notes.
The spectral rms (in italics) is measured in channels with no line emission. The rms of the radio continuum (in boldface) is obtained by averaging all the channels.
Self-noise in the maser emission channels (e.g., Sault 2012). When more than one maser feature shows circularly polarized emission, we present here the self-noise of the weakest feature. When no circularly polarized emission is detected, we consider the self-noise of the brightest maser feature.
Phase-reference calibrator at 2.856° from W75N(B). The errors of α2000 and δ2000 are 0.68 mas and 0.80 mas, respectively (Petrov et al. 2011).
Calibrated using the maser feature VLA1.1.05, see Sect. 2.
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