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Table 1

Observational details.

Source Program Observation Calibrator Polarization Beam size Position rms σ s.−n. b Estimated absolute position using FRMAP
code date angle Angle α 2000 δ 2000 Δα a Δδ a
(°) (mas × mas) (°) () () (h:m:s) () (mas) (mas)

G24.78+0.08 ES072 30 May 2013 J2202+4216 − 31 ± 4 10.4 × 4.0 –36.14 4 8 +18:36:12.563 –07:12:10.787 0.4 3.7
G25.65+1.05 ES072 31 May 2013 J2202+4216 − 31 ± 4 11.9 × 3.5 –39.94 2 35 +18:34:20.900 –05:59:42.098 2.3 18.3
G29.86-0.04 ES072 01 June 2013 J2202+4216 − 31 ± 4 9.0 × 3.6 –40.71 4 6 +18:45:59.572 –02:45:01.573 8.3 172.5
G35.03+0.35 ES069 04 Nov. 2012 J2202+4216 − 30 ± 2 6.3 × 4.8 –34.53 4 6 +18:54:00.660 +02:01:18.551 7.2 167.7
G37.43+1.51 ES072 02 June 2013 J2202+4216 − 31 ± 4 8.3 × 3.8 –52.43 3 22 +18:54:14.229 +04:41:41.138 7.0 81.2
G174.20-0.08 ES069 04 Nov. 2012 J0555+3948 − 73 ± 5 7.7 × 4.3 –28.78 4 5 +05:30:48.020 +33:47:54.611 0.7 1.0
G213.70-12.6 ES069 03 Nov. 2012 J0555+3948 − 73 ± 5 7.4 × 5.4 –3.13 4 10 +06:07:47.860 –06:22:56.626 2.1 17.9

Notes.

(a)

Formal errors of the fringe rate mapping.

(b)

Self-noise in the maser emission channels (e.g., Sault 2012).

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