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Table 1.

GJ 436 observations collected in 2016 with Narval.

Date UT HJD ncyc texp S/N σLSD Bl
[hh:mm:ss] [−2457464.4967] [s] [10−4Ic] [G]
Mar. 16 23:49:19 0.00 0.00 4×700 201 5.7 −12.3±7.0
Mar. 18 00:36:58 1.03 0.03 4×700 202 5.6 −8.0±6.8
Mar. 20 23:25:14 3.98 0.10 4×700 271 4.0 −4.0±5.0
Apr. 18 21:33:54 32.91 0.82 4×700 231 4.6 −0.9±6.0
May 2 23:10:51 46.97 1.17 4×700 265 4.0 −14.8±5.0
May 3 23:32:45 47.99 1.20 4×700 220 5.7 −11.5±6.6
May 4 21:30:12 48.90 1.22 4×700 229 4.8 −14.8±6.0
May 11 20:34:43 55.86 1.39 4×700 190 6.5 −12.3±7.4
May 16 20:45:50 60.87 1.52 4×700 270 3.9 −23.1±5.0
May 17 20:46:53 61.87 1.54 4×700 188 5.8 −19.6±7.4
May 20 21:13:31 64.89 1.62 4×700 210 5.9 −21.9±6.7
May 23 20:54:26 67.88 1.69 4×700 228 5.1 −17.4±6.1
Jun. 2 20:58:28 77.88 1.94 4×700 214 5.2 −9.1±6.5
Jun. 4 21:10:44 79.89 1.99 4×700 204 5.6 −2.7±6.8
Jun. 7 20:59:19 82.88 2.07 4×700 265 3.9 −11.3±5.1
Jun. 8 21:04:34 83.88 2.09 4×700 278 3.8 −6.5±4.7

Notes. The columns are: (1) and (2) date and universal time of the observations, (3) heliocentric Julian date normalised to the first collected observation, (4) rotational cycle of the observations found using Eq. (1), (5) exposure time of a polarimetric sequence, (6) signal-to-noise ratio at 1650 nm per polarimetric sequence, (7) rms noise level of the Stokes V signal in units of an unpolarised continuum, and (8) longitudinal magnetic field with a formal error bar.

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