\begin{table}%t1 \par \caption {\label{tab:obs}Basic properties of sources and log of observations } %\centerline { \begin{tabular}{lllllrlrlclllr} \hline \hline \noalign{\smallskip} Survey name & Other name & \multicolumn{1}{c}{$m_B^{{a}}$} &\multicolumn{1}{c}{$z^{{b}}$} & \multicolumn{1}{c}{$\Delta z^{{b}}$} & \multicolumn{1}{c}{Line$^{{c}}$} &\multicolumn{1}{c}{$M_{B}^ {{d}}$} & $\log R_K^{{\rm e}}$ & \multicolumn{1}{c}{Date$^{{f}}$} & \multicolumn{1}{c}{Band$^{{g}}$} & \multicolumn{1}{c}{DIT$^{{h}}$} & \multicolumn{1}{c}{$N_{\rm exp}^{{i}}$} & \multicolumn{1}{c}{Airmass$^{{j}}$} & \multicolumn{1}{c}{$S/N$$^{{k}}$} \\ % \multicolumn{1}{c}{} & \multicolumn{1}{c}{} & \multicolumn{1}{c}{\AA} & \multicolumn{1}{c}{\AA} % & \multicolumn{1}{c}{(1)} & \multicolumn{1}{c}{(2)} & \multicolumn{1}{c}{(3)} & \multicolumn{1}{c}{(4)} & \multicolumn{1}{c}{(5)} & \multicolumn{1}{c}{(6)} & \multicolumn{1}{c}{(7)} & \multicolumn{1}{c}{(8)} & \multicolumn{1}{c}{(9)} & \multicolumn{1}{c}{(10)} & \multicolumn{1}{c}{(11)} & \multicolumn{1}{c}{(12)} & \multicolumn{1}{c}{(13)} & \multicolumn{1}{c}{(14)}\\ \hline \object{HE~0035-2853} & & 17.03 & 1.6377 & 0.0012 & 1,2,3 & --28.10 & $<$0.21 & 2004/07/13 & $J$ & 180 & 20 & 1.12--1.03 & 20 \\ \object{HE~0043-2300} & & 17.06 & 1.5402 & 0.0014 & 1 & --27.89 & 2.03 & 2004/08/08 & $J$ & 180 & 20 & 1.01--1.08 & 40 \\ \object{HE~0058-3231} & Q 0058--3231 & 17.14 & 1.5821 & 0.0002 & 1, 2, 3 & --27.94 & $<$0.24 & 2004/07/11 & $J$ & 180 & 20 & 1.02--1.01 & 20 \\ \object{HE~0105-3006} & Q 0105--301 & 16.79 & 1.0900 & 0.0004 & 1.3 & --27.36 & $<$0.12 & 2004/07/28 & sZ & 180 & 16 & 1.00--1.01 & 10 \\ \object{HE~0109-3518} & Q 0109--3518 & 16.44 & 2.4057 & 0.0003 & 1, 2, 3 & --29.63 & $<$--0.04 & 2004/08/02 & sH & 180 & 20 & 1.49--1.23 & 20 \\ \object{HE~0119-3325} & Q 0119--3325 & 17.17 & 1.1422 & 0.0012 & 1 & --27.11 & 1.11 & 2004/08/02 & sZ & 180 & 20 & 1.11--1.03 & 12 \\ \object{HE~0142-4619} & & 17.20 & 1.1665 & 0.0017 & 1 & --27.12 & $<$0.55 & 2004/08/02 & sZ & 180 & 20 & 1.07--1.08 & 20 \\ \object{HE~0142-4619} & & & & & & & & 2004/08/03 & $J$ & 180 & 20 & 1.62--1.34 & 25 \\ \object{HE~0203-4627} & & 17.34 & 1.4381 & 0.0007 & 1, 2, 3 & --27.49 & 2.07 & 2004/08/03 & $J$ & 180 & 20 & 1.28--1.15 & 10--15 \\ HE~0203-4627 & & & & & & & & 2004/08/08 & sZ & 180 & 20 & 1.20--1.11 & 10 \\ \object{HE~0205-3756} & Q 0205-379 & 17.17 & 2.4335 & 0.0057 & 1 & --28.87 & 1.06 & 2004/08/03 & sH & 180 & 32 & 1.05--1.03 & 25 \\ \object{HE~0224-3826} & & 16.83 & 1.0763 & 0.0012 & 1 & --27.29 & $<$0.14 & 2004/08/04 & sZ & 180 & 16 & 1.06--1.03 & 15 \\ \object{HE~0229-5603} & & 17.07 & 1.1409 & 0.0015 & 1 & --27.22 & $<$--0.29 & 2004/08/18 & sZ & 180 & 16 & 1.52--1.36 & 20 \\ \object{HE~0239-4809} & & 17.12 & 1.1660 & 0.0009 & 1 & --27.27 & 0.84 & 2004/08/22 & sZ & 180 & 16 & 1.29--1.18 & 20 \\ \object{HE~0248-3628} & & 16.58 & 1.5355 & 0.0007 & 1 & --28.45 & 0.55 & 2004/08/22 & $J$ & 180 & 12 & 1.08--1.04 & 25 \\ \object{HE~0251-5550} & H25.01 & 16.59 & 2.3505 & 0.0011 & 1 & --29.56 & $<$0.23 & 2004/08/18 & sH & 180 & 20 & 1.31--1.21 & 35 \\ \object{HE~0349-5249} & H27.03 & 16.13 & 1.5409 & \ldots & 1 & --28.93 & 0.76 & 2004/08/22 & $J$ & 180 & 12 & 1.17--1.14 & 17.5 \\ \object{HE~0359-3959} & & 17.09 & 1.5209 & \ldots & 1 & --27.89 & 0.22 & 2004/08/28 & $J$ & 180 & 20 & 1.14--1.06 & 20 \\ \object{HE~0435-4312} & & 17.10 & 1.2321 & 0.0014 & 1 & --27.35 & $<$0.51 & 2004/09/17 & sZ & 180 & 16 & 1.47--1.28 & 10--5 \\ \object{HE~0436-3709} & & 16.84 & 1.4447 & 0.0023 & 1 & --27.93 & $<$0.38 & 2004/09/17 & $J$ & 180 & 16 & 1.10--1.04 & 10 \\ \object{HE~0940-1050} & & 16.96 & 3.0932 & \ldots & 1 & --29.82 & $<$0.10 & 2005/06/10 & sK & 180 & 24 & 1.18--1.50 & 10-45 \\ \object{HE~1039-0724} & & 17.16 & 1.4584 & 0.0002 & 1, 2, 3 & --27.86 & $<$0.20 & 2005/06/23 & $J$ & 180 & 20 & 1.19--1.44 & 20 \\ \object{HE~1120+0154} & UM 425 & 16.31 & 1.4720 & 0.0004 & 1, 2, 3 & --28.70 & --0.57 & 2005/06/24 & $J$ & 180 & 16 & 1.42--1.75 & 35 \\ \object{HE~1347-2457} & & 16.83 & 2.5986 & \ldots & 1 & --29.64 & --0.68 & 2005/04/15 & sH & 180 & 28 & 1.16--1.54 & 65--10 \\ \object{HE~1348+0118} & Q 1348+0118 & 17.08 & 1.0873 & 0.0012 & 1 & --27.05 & $<$0.24 & 2005/06/13 & sZ & 180 & 12 & 1.20--1.29 & 15 \\ \object{HE~1349+0007} & UM 617 & 16.83 & 1.4442 & 0.0010 & 1, 2, 3 & --28.00 & --0.18 & 2005/06/24 & $J$ & 180 & 20 & 1.25--1.52 & 15 \\ \object{HE~1409+0101} & & 16.92 & 1.6497 & 0.0039 & 1 & --28.30 & 0.40 & 2005/07/21 & $J$ & 180 & 20 & 1.18--1.38 & 55--25 \\ \object{HE~1430-0041} & Q 1430-0041 & 16.72 & 1.1216 & \ldots & 1 & --27.60 & --0.39 & 2005/07/21 & sZ & 180 & 16 & 1.43--1.78 & 20 \\ \object{HE~1505+0212} & & 17.06 & 1.0943 & \ldots & 1 & --27.28 & 0.51 & 2004/07/18 & sZ & 180 & 16 & 1.26--1.53 & 50 \\ HE~1505+0212 & & & 1.0930 & 0.0240 & 1 & & & 2005/05/21 & sZ & 180 & 20 & 1.28--1.57 & 30 \\ \object{HE~2147-3212} & & 16.84 & 1.5432 & \ldots & 1 & --28.15 & $<$0.14 & 2004/07/05 & $J$ & 180 & 20 & 1.06--1.19 & 15 \\ \object{HE~2156-4020} & & 17.39 & 2.5431 & 0.0010 & 1 & --28.75 & --0.09 & 2004/07/10 & sH & 180 & 32 & 1.05--1.20 & 15--5 \\ \object{HE~2335-3029} & & 16.96 & 1.1194 & 0.0016 & 1 & --27.21 & $<$0.20 & 2004/07/11 & sZ & 180 & 16 & 1.58--1.31 & 25 \\ \noalign{\smallskip} \noalign{\smallskip} \hline \end{tabular}} \par \smallskip $^{{a}}$ Apparent B Johnson magnitude corrected because of Galactic absorption. The value of HE 0436$-$3709 referes to the b Str\"omgren magnitude. $^{{b}}$ Redshift, with uncertainty in parentheses. $^{{c}}$ Lines used for redshift calculations: 1: \hb, 2: \oiii. 3: [\ion{O}{iii}]\l4959. $^{{d}}$ Absolute $B$~magnitude, computed for $H_0=70$~\kms~Mpc$^{-1}$, $\Omega_{\rm M} = 0.3$, $\Omega_{\Lambda} = 0.7$, and $k$-correction spectral index $a=0.6$. $^{{e}}$ Decimal logarithm of the specific flux ratio at 6~cm and 4400~\AA\ (effective wavelength of the $B$~band). Upper limits are from the NVSS ($\approx$2.5~mJy), and would place all undetected sources in the RQ domain. $^{{f}}$ Date refers to time at start of exposure. $^{{g}}$ Photometric band. $^{{h}}$ Detector Integration Time (DIT) of ISAAC, in seconds. $^{{i}}$ Number of exposures with integration time equal to DIT. $^{{j}}$ Airmass at start and end of exposure. $^{{k}}$ $S/N$\ at continuum level in the proximity of \hb. Two values are reported in case of different $S/N$\ on the blue and red side of \hb\ (blue side first). The $S/N$\ value is with $N$ estimated at a $2 \sigma$\ confidence level i.e., 2~times the rms. \end{table}