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Table A.1:

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)
Secure ID                      
J1211+0422 H 2.54 2.37655 20.80 $\pm$ 0.10 -1.41 $\pm$ 0.08 Si 1238 yes -130, 25 76.7 $\pm$ 3.6 13.63 $\pm$ 0.22
Q0450-1310 U 2.25 2.06655 20.50 $\pm$ 0.07 -1.45 $\pm$ 0.05 Si 1238 yes -30, 115 65.6 $\pm$ 2.3 13.56 $\pm$ 0.02
Q0528-2505 U 2.77 2.81115 21.35 $\pm$ 0.07 -0.90 $\pm$ 0.11 Si 1238 no -115, 100 171.0 $\pm$ 2.2 14.01 $\pm$ 0.05
Q0551-3637 U 2.32 1.96221 20.70 $\pm$ 0.08 -0.44 $\pm$ 0.06 Si 1238 yes -220, 100 319.9 $\pm$ 9.7 14.28 $\pm$ 0.07
Q1242+0006 U 2.08 1.82452 20.45 $\pm$ 0.10 -1.04 $\pm$ 0.07 Si 1238 yes -865, -700 167.0 $\pm$ 7.3 14.05 $\pm$ 0.02
Q1331+1704 U 2.08 1.77635 21.15 $\pm$ 0.07 -1.40 $\pm$ 0.05 Si 1238 yes -200, 200 224.7 $\pm$ 3.1 14.08 $\pm$ 0.06
Q2243-6031 U 3.01 2.33061 20.65 $\pm$ 0.05 -0.85 $\pm$ 0.05 Si 1238 yes -380, -350 33.6 $\pm$ 2.0$\dagger$ 13.52 $\pm$ 0.01
Q2348-1444 U 2.94 2.27940 20.56 $\pm$ 0.08 -1.92 $\pm$ 0.02 Si 1242 yes -145, 25 214.3 $\pm$ 2.2$\dagger$ 14.61 $\pm$ 0.15
Marginal ID                      
J1014+4300 H 3.10 2.95880 20.50 $\pm$ 0.02 -0.71 $\pm$ 0.14 Si 1242 yes -60, 25 16.5 $\pm$ 2.3 13.20 $\pm$ 0.04
J1757+7539 H 3.05 2.62530 20.76 $\pm$ 0.02 -0.79 $\pm$ 0.01 Si 1242 yes -80, -55 14.8 $\pm$ 2.2 13.20 $\pm$ 0.03
J2100-0641 E 3.14 3.09240 21.05 $\pm$ 0.15 -0.72 $\pm$ 0.01 Si 1242 no -75, 100 52.7 $\pm$ 5.7 13.62 $\pm$ 0.05
Q0042-2930 U 2.39 1.80947 20.40 $\pm$ 0.10 -1.25 $\pm$ 0.15 Si 1242 yes -105, -75 32.2 $\pm$ 4.3 13.59 $\pm$ 0.04
Non-detection                      
HE0251-5550 U 2.37 2.33972 20.70 $\pm$ 0.08 -1.41 $\pm$ 0.08 S 1238 no -50, 50 <7.9 <12.57
HE0322-3213 U 3.30 2.24338 20.50 $\pm$ 0.10 -0.74 $\pm$ 0.10 S 1242 yes -50, 50 <88.3 <13.83
HE0414-2850 U 2.09 1.71903 21.20 $\pm$ 0.10 -0.75 $\pm$ 0.10 Zn 1242 yes -50, 50 <18.9 <13.25
HE2225-4025 U 2.41 1.96532 20.65 $\pm$ 0.10 -2.26 $\pm$ 0.10 Si 1242 yes -50, 50 <12.1 <13.05
HE2316-1012 U 1.95 1.92990 21.35 $\pm$ 0.10 -1.57 $\pm$ 0.12 Zn 1238 no -50, 50 <17.0 <12.90
J0255+0008 H 3.97 3.91460 21.30 $\pm$ 0.05 -1.78 $\pm$ 0.01 S 1242 no -20, 80 <14.7 <13.14
J0339-0133 H 3.20 3.06210 21.20 $\pm$ 0.10 -1.54 $\pm$ 0.01 S 1238 yes -70, 70 <27.3 <12.85
J0747+2739 E 4.11 3.42330 20.85 $\pm$ 0.05 -1.66 $\pm$ 0.21 Si 1238 yes -180, 30 <26.6 <13.10
J0812+3208 H 2.70 2.62630 21.35 $\pm$ 0.10 -0.93 $\pm$ 0.05 Si 1242 yes -80, 210 <9.1 <12.93
J0836+1046 H 2.70 2.46530 20.58 $\pm$ 0.10 -1.15 $\pm$ 0.05 Si 1238 yes -100, 200 <86.2 <13.61
J0900+4204 H 3.29 3.24580 20.30 $\pm$ 0.10 -0.85 $\pm$ 0.02 S 1238 no -15, 60 <6.2 <12.47
J0929+2825 H 3.40 3.26270 21.10 $\pm$ 0.00 -1.62 $\pm$ 0.01 Si 1242 yes -50, 100 <7.0 <12.82
J0930+2803 H 3.42 3.23530 20.30 $\pm$ 0.10 -1.97 $\pm$ 0.02 Si 1242 yes -50, 0 <8.4 <12.89
J1021+3001 H 3.12 2.94890 20.70 $\pm$ 0.10 -1.94 $\pm$ 0.02 Si 1238 yes -25, 70 <11.7 <12.74
J1131+6044 H 2.92 2.87600 20.50 $\pm$ 0.15 -2.13 $\pm$ 0.15 Si 1238 no -100, 50 <15.2 <12.85
J1135+2227 H 2.88 2.78350 21.00 $\pm$ 0.07 -2.08 $\pm$ 0.14 Si 1242 yes -50, 50 <16.6 <12.92
J1310+5424 H 1.93 1.80070 21.45 $\pm$ 0.15 -0.45 $\pm$ 0.15 Zn 1242 yes -100, 100 <81.9 <13.88
J1357-1744 H 3.15 2.77990 20.30 $\pm$ 0.15 -1.86 $\pm$ 0.05 Si 1238 yes -50, 0 <53.6 <13.26
J1410+5111 H 3.21 2.96420 20.85 $\pm$ 0.20 -1.96 $\pm$ 0.15 Si 1238 yes 75, 200 <21.7 <13.01
J1435+5359 H 2.64 2.34270 21.05 $\pm$ 0.10 -1.48 $\pm$ 0.10 Si 1238 yes -50, 70 <9.5 <12.65
J1506+5220 H 4.18 3.22440 20.67 $\pm$ 0.07 -2.33 $\pm$ 0.02 Si 1238 yes -50, 30 <21.3 <13.00
J1558-0031 H 2.83 2.70260 20.67 $\pm$ 0.05 -1.99 $\pm$ 0.01 Si 1238 yes -20, 20 <38.4 <13.16
J2036-0552 H 2.58 2.28050 21.20 $\pm$ 0.15 -1.71 $\pm$ 0.17 Si 1238 yes -30, 50 <13.1 <12.79
J2241+1352 E 4.44 4.28240 21.15 $\pm$ 0.10 -1.76 $\pm$ 0.03 S 1242 yes -15, 150 <64.8 <13.53
J2323+2758 E 4.18 3.68450 20.95 $\pm$ 0.10 -2.59 $\pm$ 0.03 Si 1238 yes -50, 50 <79.1 <13.35
J2340-0053 H 2.09 2.05450 20.35 $\pm$ 0.15 -0.74 $\pm$ 0.04 Si 1238 no -50, 50 <22.5 <12.87
J2346+1245 H 2.79 2.53790 20.36 $\pm$ 0.10 -1.74 $\pm$ 0.01 Si 1242 yes -50, 10 <32.5 <13.32
Q0010-0012 U 2.15 2.02478 20.95 $\pm$ 0.10 -1.43 $\pm$ 0.11 Zn 1238 yes -50, 50 <21.9 <13.01
Q0039-3354 U 2.48 2.22400 20.60 $\pm$ 0.10 -1.31 $\pm$ 0.12 Si 1242 yes -50, 130 <47.8 <13.40
Q0042-2930 U 2.39 1.93560 20.50 $\pm$ 0.10 -1.27 $\pm$ 0.10 Si 1242 yes -50, 50 <32.4 <13.48
Q0049-2820 U 2.26 2.07125 20.45 $\pm$ 0.10 -1.31 $\pm$ 0.12 Si 1242 yes -20, 50 <11.0 <13.01
Q0100+1300 U 2.69 2.30904 21.35 $\pm$ 0.08 -1.46 $\pm$ 0.01 S 1242 yes -50, 50 <20.2 <13.08
Q0102-1902 U 3.04 2.36962 21.00 $\pm$ 0.08 -1.90 $\pm$ 0.08 S 1242 yes -50, 50 <10.3 <12.98
Q0112+0259 U 2.81 2.42310 20.90 $\pm$ 0.10 -1.31 $\pm$ 0.11 S 1238 yes -50, 100 <13.1 <12.79
Q0112-3030 U 2.99 2.41850 20.50 $\pm$ 0.08 -2.42 $\pm$ 0.08 Si 1238 yes -30, 30 <9.1 <12.63
Q0135-2722 U 3.21 2.10739 20.30 $\pm$ 0.15 -1.12 $\pm$ 0.16 S 1238 yes 0, 120 <24.0 <13.05
Q0135-2722 U 3.21 2.80003 21.00 $\pm$ 0.10 -1.40 $\pm$ 0.10 S 1242 yes -100, 50 <73.6 <13.73
Q0254-4025 U 2.28 2.04607 20.45 $\pm$ 0.08 -1.55 $\pm$ 0.09 S 1238 yes -50, 50 <12.7 <12.77
Q0300-3152 U 2.37 2.17905 20.80 $\pm$ 0.10 -1.80 $\pm$ 0.10 S 1238 yes -50, 50 <50.0 <13.21
Q0405-4418 U 3.02 1.91270 20.80 $\pm$ 0.10 -1.03 $\pm$ 0.10 Zn 1238 yes -100, 40 <68.9 <13.45
Q0405-4418 U 3.02 2.54990 21.15 $\pm$ 0.15 -1.36 $\pm$ 0.16 Zn 1242 yes 0, 150 <45.8 <13.52
Q0405-4418 U 3.02 2.59475 21.05 $\pm$ 0.10 -1.12 $\pm$ 0.10 Zn 1238 yes -50, 70 <58.1 <13.38
Q0405-4418 U 3.02 2.62140 20.45 $\pm$ 0.10 -2.04 $\pm$ 0.10 Si 1242 yes 70, 150 <27.9 <13.30
Q0421-2624 U 2.28 2.15680 20.65 $\pm$ 0.10 -1.86 $\pm$ 0.10 Si 1238 yes 0, 230 <24.0 <13.05
Q0425-5214 U 2.25 2.22430 20.30 $\pm$ 0.10 -1.43 $\pm$ 0.11 S 1238 no -75, 50 <9.9 <12.67
Q0432-4401 U 2.65 2.30197 20.95 $\pm$ 0.10 -1.23 $\pm$ 0.13 S 1238 yes -150, -70 <12.7 <12.78
Q0458-0203 U 2.29 2.03955 21.70 $\pm$ 0.10 -1.22 $\pm$ 0.10 Zn 1242 yes -150, 50 <79.3 <13.67
Q0642-5038 U 3.09 2.65860 20.95 $\pm$ 0.08 -1.05 $\pm$ 0.09 Zn 1242 yes -100, 100 <22.7 <13.33
Q0841+1256 U 2.50 1.86388 21.00 $\pm$ 0.10 -1.51 $\pm$ 0.11 S 1238 yes -100, 10 <38.0 <13.06
Q0841+1256 U 2.50 2.37452 21.05 $\pm$ 0.10 -1.27 $\pm$ 0.02 Si 1238 yes -50, 50 <14.1 <12.82
Q0841+1256 U 2.50 2.47621 20.80 $\pm$ 0.10 -1.39 $\pm$ 0.03 S 1238 no -50, 50 <9.2 <12.64
Q0933-3319 U 2.68 2.68227 20.50 $\pm$ 0.10 -1.27 $\pm$ 0.14 Si 1238 no -50, 50 <27.1 <13.10
Q1036-2257 U 3.13 2.77739 20.93 $\pm$ 0.05 -1.36 $\pm$ 0.05 S 1238 yes -15, 150 <21.8 <12.79
Q1055-3008 U 1.90 1.90350 21.54 $\pm$ 0.10 -1.30 $\pm$ 0.03 Zn 1238 no -50, 50 <31.6 <13.17
Q1108-0747 U 3.92 3.60760 20.37 $\pm$ 0.07 -1.59 $\pm$ 0.07 Si 1238 yes -130, -25 <12.2 <12.76
Q1111-1517 U 3.37 3.26548 21.30 $\pm$ 0.05 -1.65 $\pm$ 0.11 Zn 1242 yes 70, 170 <6.1 <12.76
Q1157+0128 U 1.99 1.94375 21.80 $\pm$ 0.10 -1.44 $\pm$ 0.10 Zn 1238 no -75, 50 <12.8 <12.78
Q1203+0218 U 2.13 1.74735 20.40 $\pm$ 0.10 -0.97 $\pm$ 0.11 Zn 1242 yes -100, 15 <72.7 <13.64
Q1210+1731 U 2.54 1.89177 20.70 $\pm$ 0.08 -0.93 $\pm$ 0.08 S 1242 yes -50, 50 <71.3 <13.77
Q1223+1753 U 2.94 2.46608 21.40 $\pm$ 0.10 -1.63 $\pm$ 0.10 Zn 1242 yes -85, 150 <54.6 <13.55
Q1337+1121 U 2.92 2.79583 21.00 $\pm$ 0.08 -1.86 $\pm$ 0.09 Si 1238 yes -80, 25 <13.8 <12.81
Q1354-1046 U 3.01 2.96680 20.80 $\pm$ 0.10 -1.39 $\pm$ 0.10 Si 1238 no -50, 50 <7.7 <12.56
Q1409+0930 U 2.85 2.01882 20.65 $\pm$ 0.10 -1.62 $\pm$ 0.16 Zn 1238 yes -50, 50 <8.5 <12.60
Q1409+0930 U 2.85 2.45595 20.53 $\pm$ 0.08 -2.06 $\pm$ 0.08 Si 1238 yes -50, 50 <29.0 <12.96
Q2059-3604 U 3.09 3.08291 20.98 $\pm$ 0.08 -1.77 $\pm$ 0.09 S 1242 no -25, 100 <16.0 <13.17
Q2138-4427 U 3.17 2.85235 20.98 $\pm$ 0.05 -1.74 $\pm$ 0.05 Zn 1242 yes -270, 120 <10.7 <13.00
Q2206-1958 U 2.56 2.07622 20.44 $\pm$ 0.05 -2.32 $\pm$ 0.05 Si 1242 yes -25, 50 <16.7 <12.99
Q2222-3939 U 2.18 2.15387 20.85 $\pm$ 0.10 -1.97 $\pm$ 0.10 S 1242 no -25, 25 <8.1 <12.88
Q2228-3954 U 2.21 2.09437 21.20 $\pm$ 0.10 -1.36 $\pm$ 0.12 Zn 1242 yes -35, 25 <18.6 <13.24
Q2230+0232 U 2.15 1.86377 20.90 $\pm$ 0.10 -0.81 $\pm$ 0.10 S 1238 yes -50, 50 <10.6 <12.70
Q2311-3721 U 2.48 2.18210 20.48 $\pm$ 0.13 <-1.33 Zn 1242 yes -100, 50 <10.8 <13.00
Q2314-4057 U 2.45 1.85733 20.90 $\pm$ 0.10 -1.02 $\pm$ 0.14 Zn 1238 yes -100, 50 <25.0 <13.07
Q2332-0924 U 3.32 3.05725 20.50 $\pm$ 0.07 -1.33 $\pm$ 0.08 S 1238 yes -130, 50 <11.4 <12.73
Q2341+0325 U 4.24 3.22030 21.35 $\pm$ 0.07 <-1.63 Zn 1238 yes -20, 70 <31.9 <13.00
Q2342+3417 U 3.01 2.90910 21.10 $\pm$ 0.10 -1.04 $\pm$ 0.02 Si 1238 yes -50, 50 <38.7 <13.12
Q2343+1232 U 2.76 2.43127 20.40 $\pm$ 0.07 -0.60 $\pm$ 0.06 Si 1242 yes -350, -50 <17.3 <12.92
Q2348-0108 U 3.01 2.61473 21.30 $\pm$ 0.08 -2.02 $\pm$ 0.08 Si 1242 yes -50, 50 <10.5 <12.99
Q2359-0216 U 2.81 2.09508 20.65 $\pm$ 0.10 -0.84 $\pm$ 0.13 Zn 1242 yes -180, 100 <44.8 <13.62
Q2359-0216 U 2.81 2.15390 20.30 $\pm$ 0.10 -1.62 $\pm$ 0.10 Si 1238 yes -150, 75 <52.3 <13.39
0 Our adopted QSO names follow one of three conventions, each based on the object coordinates. The UVES quasars are named either HEhhmm+ddmm (Hamburg-ESO survey, J2000) or Qhhmm+ddmm (J1950); the HIRES and ESI quasars are named Jhhmm+ddmm (J2000). We retain these (non-standardized) names to facilitate comparison with previous work. Absorbers are listed alphabetically within each category.
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. Most [Z/H] and log N(H I) measurements are from Ledoux et al. (2006), Prochaska et al. (2007), and Wolfe et al. (2008). Several others were taken from Lu et al. (1996), Ellison & Lopez (2001), Srianand & Petitjean (2001), Akerman et al. (2005), Heinmüller et al. (2006), Fox et al. (2007b), Noterdaeme et al. (2008), or Kaplan et al. (2009, in prep.).
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. The N V doublet has $\lambda_0$ = 1238.821, 1242.804 Å and f = 0.157, 0.07821 respectively (Morton 2003).
List of DLAs with blended N V (QSO, $z_{\rm abs}$, instrument): HE0242-2917 2.55956 U; J0022-1505 3.43890 H; J0127-0045 3.72740 E; J0133+0400 3.69260 H; J0134+3307 3.76090 E; J0203+1134 3.38690 H; J0209+0517 3.66670 H; J0209+0517 3.86430 H; J0349-3810 3.02470 H; J0426-2202 2.98310 E; J0747+2739 3.90000 E; J0808+5215 3.11320 E; J0826+3148 2.91220 H; J0956+4734 3.40360 E; J0956+4734 3.89100 E; J0956+4734 4.24420 E; J1057+4555 3.31720 H; J1155+0530 3.32680 H; J1248+3110 3.69700 E; J1253-0228 2.78280 E; J1410+5111 2.93440 H; J1432+3940 3.27250 E; J1502+4803 2.56960 E; J1723+2243 3.69470 E; J2225+2040 3.11920 H; Q0013-0029 1.97295 U; Q0027-1836 2.40186 U; Q0058-2914 2.67140 U; Q0112-3030 2.70230 U; Q0130+0345 3.77373 U; Q0216+0803 1.76875 U; Q0438-4338 2.34736 U; Q0528-2505 2.14105 U; Q0913+0715 2.61840 U; Q0951-0450 3.85670 H; Q0951-0450 4.20287 U; Q0952-0115 4.02270 U; Q1117-1329 3.35037 U; Q1209+0919 2.58440 U; Q1228-1122 2.19289 U; Q1232+0815 2.33771 U; Q1354-1046 2.50090 U; Q1441+2737 4.22371 U; Q1451+1223 2.25465 U; Q1451+1223 2.46921 U; Q2138-4427 2.38279 U; Q2153+1344 3.31600 U; Q2206-1958 1.91998 U; Q2318-1107 1.98888 U; Q2348-0108 2.42630 U.

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