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Table 2.

Observation log for the VLT/FORS2 long-slit spectroscopic observations of damped absorbing galaxies.

Quasar field RA (J2000) Dec (J2000) Obs. date Nexp. × texp. (s) GRISM Slit PA (deg) Airmass Seeing (arcsec) Δλsyst. (Å)
HE 1122–1649 11:24:42.87 –17:05:17.50 2015-04-19 2 × 1800 600RI –12.90 1.105 0.86–0.93 0.33
Q 0153+0009 01:53:18.19 +00:09:11.44 2015-09-(08:09) 4 × 1800 600z 73.40 1.172 0.73–0.84 –0.93
Q 1209+107 PA1 12:11:40.59 +10:30:02.04 2015-04-19 2 × 1300 600RI 96.70 1.323 1.12–1.27 –1.04
Q 1209+107 PA2 12:11:40.59 +10:30:02.04 2015-04-19 2 × 1300 600RI 43.30 1.236 1.24–1.32 –0.44
Q 1323–0021 13:23:23.78 –00:21:55.28 2015-04-(17:18) 4 × 1100 600RI 42.00 1.158 1.03–1.17 –0.64
Q 1436–0051 14:36:45.05 –00:51:50.59 2015-04-(13:14) 4 × 1800 600z 29.40 1.097 0.68–0.77 –0.72
Q 2328+0022 23:28:20.38 +00:22:38.24 2015-07-11 2 × 800 600RI 45.00 1.147 0.78–0.85 –0.38
Q 2335+1501 23:35:44.19 +15:01:18.37 2015-05-30 2 × 800 600RI 4.80 1.673 0.83–0.93 0.43
Q 2353–0028 23:53:21.62 –00:28:40.67 2015-07-11 4 × 1800 600RI –2.30 1.143 0.90–0.95 0.35

Notes. RA and Dec refer to the coordinates of the quasar. The slit position angle (PA) was selected to match the candidate host galaxy from imaging data (Rao et al. 2011), and is defined so that N = 0, E = 90°. All observations were taken with a slit-width of 1.31 arcsec. The tabulated airmass corresponds to the mean value calculated from the nominal header-values at start and end for each exposure. The seeing, as the FWHM of a summed profile in ten pixels along the dispersion direction, was measured in the combined spectrum of the quasar. As the seeing-measurements varied temporally and in wavelength non-trivially, we report the observed ranges. We define the systematic offset in the wavelength-solution as Δλsyst. = λcalib.λUVES.

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