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Table A.2:

Sub-DLA N V measurements.
QSO0 Ins.1 $z_{\rm em}$ $z_{\rm abs}$2 log $N(H {\sc i})$ [Z/H]3 Z Line4 For.?5 v-, v+ $W_{\lambda}$(N V)6 log  $N(N {\sc v})^7$
        (N in cm-2)         (km s-1) (mÅ) (N in cm-2)
Detection                      
Q0237-2321 U 2.22 1.67234 19.65 $\pm$ 0.10 -0.26 $\pm$ 0.10 Si 1238 yes -50, 100 101.7 $\pm$ 2.3 13.88 $\pm$ 0.19
Q1037-2704 U 2.20 2.13906 19.70 $\pm$ 0.05 -0.02 $\pm$ 0.10 Si 1238 yes -340, -280 67.1 $\pm$ 2.0$\dagger$ 13.77 $\pm$ 0.01
Non-detection                      
HE0057-4126 U 2.05 1.72055 20.13 $\pm$ 0.07 -2.06 $\pm$ 0.08 Si 1238 yes -50, 50 <18.6 <12.94
HE0438-1638 U 1.97 1.69420 19.85 $\pm$ 0.10 -0.93 $\pm$ 0.10 Si 1238 yes -50, 50 <30.9 <13.16
J0953+5230 H 1.87 1.76780 20.10 $\pm$ 0.10 -0.05 $\pm$ 0.05 Si 1242 yes -100, 200 <58.0 <13.51
Q0049-2820 U 2.26 1.88615 20.20 $\pm$ 0.08 -1.03 $\pm$ 0.09 S 1238 yes -50, 50 <24.4 <13.06
Q0102-1902 U 3.04 2.92650 20.00 $\pm$ 0.10 -1.50 $\pm$ 0.10 Si 1238 yes -50, 50 <7.0 <12.51
Q0331-4505 U 2.67 2.41120 20.15 $\pm$ 0.07 <-1.41 Zn 1238 no -40, 50 <12.3 <12.76
Q0331-4505 U 2.67 2.65618 19.82 $\pm$ 0.05 -1.49 $\pm$ 0.05 Si 1238 yes -50, 50 <11.8 <12.74
Q1101-2629 U 2.14 1.83890 19.35 $\pm$ 0.04 -0.82 $\pm$ 0.14 S 1242 yes -65, 50 <16.2 <12.98
Q1220-1800 U 2.16 2.11285 20.12 $\pm$ 0.07 -0.93 $\pm$ 0.07 S 1238 no -60, 60 <11.3 <12.72
Q1337+1121 U 2.92 2.50792 20.12 $\pm$ 0.05 -1.81 $\pm$ 0.06 Si 1242 yes -50, 50 <25.1 <13.37
Q1340-1340 U 3.20 3.11835 20.05 $\pm$ 0.08 -1.42 $\pm$ 0.08 S 1242 yes -125, 250 <6.6 <12.79
Q1409+0930 U 2.85 2.66818 19.80 $\pm$ 0.08 -1.41 $\pm$ 0.09 S 1242 yes -200, 0 <37.8 <13.43
Q1444+0126 U 2.21 2.08679 20.25 $\pm$ 0.07 -0.80 $\pm$ 0.09 Zn 1242 yes 100, 190 <11.2 <13.02
Q2059-3604 U 3.09 2.50735 20.29 $\pm$ 0.07 -1.85 $\pm$ 0.20 S 1238 yes -50, 50 <56.0 <13.26
Q2153+1344 U 4.26 4.21225 19.70 $\pm$ 0.10 -1.81 $\pm$ 0.10 Si 1242 no -50, 50 <7.3 <12.83
Q2314-4057 U 2.45 1.87519 20.10 $\pm$ 0.20 <-1.19 Zn 1238 yes -20, 50 <11.0 <12.71
0 See footnote to Table A.1 for naming conventions.
1 Instrument that provided the data: U = UVES, H = HIRES, E = ESI.
2 Redshift defined by velocity of strongest low-ionization component.
3 Metallicity on log scale relative to solar. Z = S, Si, or Zn as listed in adjacent column. No ionization corrections have been applied.
4 N V line used for measurement.
5 Is the N V doublet in the Lyman-${\alpha }$ forest? If no, the system is within 5600 km s-1 of background QSO, so ``no'' implies ``proximate''.
6 N V rest-frame equivalent width, measured in the velocity range listed in the adjacent column. Upper limits are 3$\sigma$. In cases marked $\dagger$, the data are partly blended; the measurement listed here derives from the unblended velocity range, and the total  $W_{\lambda}$ could be higher.
7 For detections, $N_{\rm N {\sc v}}$ is the sum of the component column densities from VPFIT. For non-detections, 3$\sigma$ upper limits were calculated using $N_{\rm N {\sc v}}=1.13$ $\times$ $10^{17}W_{\lambda}^{\rm lim}/\lambda_0^2 f$, where $W_{\lambda}^{\rm lim}$ is the 3$\sigma$ upper limit on the equivalent width in mÅ, $\lambda_0$ is in Å, and $N_{\rm N {\sc v}}$ is in cm-2.
List of sub-DLAs with blended N V (QSO, $z_{\rm abs}$, instrument): Q0952-0115 3.47570 U; Q1108-0747 3.48179 U; Q2116-3537 1.99618 U; Q2153+1344 3.14198 U; Q2332-0924 2.28749 U.

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