Table D.3.
Flux densities of LkCa 4 in Stokes I and V that were used in the light curve in Fig. 5.
Time | Stokes I | Stokes V | Pol. Fraction | Beam |
---|---|---|---|---|
(hrs) | (mJy) | (mJy) | (%) | |
0 - 0.5 | ≤4.38 | ≤3.21 | - |
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0.5 - 1.0 | ≤3.24 | ≤2.61 | - |
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1.0 - 1.5 | 4.99 ± 0.99 | 3.30 ± 0.70 |
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1.5 - 2.0 | 4.30 ± 0.76 | 3.76 ± 0.61 |
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2.0 - 2.5 | 2.76 ± 0.68 | 3.00 ± 0.56 |
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![]() |
2.5 - 3.0 | ≤1.89 | ≤1.47 | - |
![]() |
3.0 - 3.5 | ≤2.01 | ≤1.47 | - |
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3.5 - 4.0 | ≤1.89 | ≤1.44 | - |
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4.0 - 4.5 | ≤1.80 | ≤1.50 | - |
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4.5 - 5.0 | ≤1.74 | ≤1.44 | - |
![]() |
5.0 - 5.5 | ≤1.74 | ≤1.47 | - |
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5.5 - 6.0 | 2.28 ± 0.62 | ≤1.53 | ≤67 |
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6.0 - 6.5 | ≤1.83 | ≤1.53 | - |
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6.5 - 7.0 | 3.95 ± 0.60 | 2.40 ± 0.53 |
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7.0 - 7.5 | 4.46 ± 0.65 | 3.90 ± 0.56 |
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![]() |
7.5 - 8.0 | ≤2.25 | ≤1.86 | - |
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Notes. The time in the first column refers to the time in hours after the start of the observation (August 10, 2019, at 02:11:00). The polarisation fraction is shown for the times where both Stokes I and V are detected. When only Stokes I is detected, 3σ upper limits are given for the polarisation fraction. The dimensions and position angle of the synthesised beam in the image at each time are shown in the final column.
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