Feature |
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(km s-1) | (Jy beam-1) | (mas) | (mas) | (km s-1) | (mG) | |||||
RCP | LCP | RCP | LCP | |||||||
1 | 70.88 | 71.76 | 2.39 | 0.40 | 0 | 0 | -0.86 | -1.5 | ||
2 | 67.89 | ... | 2.02 | ... |
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... | ... | ||
3 | 66.84 | 66.84 | 1.36 | 0.84 |
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... | ... | ||
4 | 73.87 | 73.87 | 1.01 | 0.16 |
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... | ... | ||
5 | ... | 74.75 | ... | 0.97 |
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... | ... | ||
6 | ... | 70.57 | ... | 0.89 |
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... | ... | ||
7 | 68.07 | ... | 0.74 | ... |
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... | ... | ||
8 | 72.99 | 72.99 | 0.67 | 0.26 |
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... | ... | ||
9 | ... | 75.10 | ... | 0.60 |
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... | ... | ||
10 | 74.92 | ... | 0.55 | ... |
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... | ... | ||
11 | 70.35 | 69.82 | 0.52 | 0.23 |
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+0.62 | +1.0 | ||
12 | 67.19 | ... | 0.46 | ... |
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... | ... | ||
13 | 76.33 | 79.67 | 0.25 | 0.43 |
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-3.41 | -5.8 | ||
14 | ... | 76.33 | ... | 0.41 |
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... | ... | ||
15 | 68.77 | ... | 0.38 | ... |
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... | ... | ||
16 | ... | 63.50 | ... | 0.31 |
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... | ... | ||
17 | 64.90 | ... | 0.30 | ... |
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... | ... | ||
18 | 70.18 | ... | 0.25 | ... |
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... | ... | ||
19 | 79.32 | 77.21 | 0.25 | 0.17 |
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+2.11 | +3.6 | ||
20 | 64.55 | 65.08 | 0.23 | 0.13 |
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-0.49 | -0.8 | ||
21 | 66.84 | ... | 0.22 | ... |
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... | ... | ||
22 | 62.62 | 62.79 | 0.16 | 0.20 |
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... | ... | ||
23 | 69.65 | 69.30 | 0.18 | 0.19 |
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... | ... | ||
24 | 60.68 | 60.51 | 0.12 | 0.14 |
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... | ... | ||
Reference Feature: Absolute position | ||||||||||
Feature | RA(J2000) | Dec(J2000) | ||||||||
(h m s) | (![]() |
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1 | 18:34:40.28515
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-09:00:38.3783
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Notes. For each identified
feature, the label (given in Col. 1) increases with decreasing
brightness. Columns 2(3) and 4(5) report the LSR
velocity and brightness of the brightest spot for the right (left)
circular polarization. Columns 6 and 7 give the
position offset relative to the feature #1, in the
east and north directions, respectively. Columns 8
and 9 report the fit split of LSR velocity (RCP-LCP) between
co-spatial circular polarization components and the inferred l.o.s.
magnetic field strength, respectively. The absolute position of the
reference feature #1 is reported at the bottom of the table.
(a) A magnetic field
of 0.34 mG shifts the emission velocity of 1665 MHz
OH masers by 0.2 km s-1.
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