Table 3: Observed fluxes, for type 1 objects, in units of $\rm 10^{-15}~ erg ~ cm^{-2} ~ s^{-1}$.

Ion		 $\rm\lambda_{lab}~(\AA)$ NGC 4748 Mrk 279 NGC 5548 PG 1415+451 Mrk 684 Mrk 478 PG 1448+273 Mrk 291 Mrk 493 PG 1519+226

O I		 8446 - $32.16\pm7.67$$^{\xi}$ $12.52\pm1.46 $ - - - $17.17\pm0.80 $ $1.74\pm0.26$ $20.69\pm1.18 $ $14.58\pm1.58$
Ca II 8498 - - $11.45\pm1.62 $ - - - $9.27\pm1.53 $ - $12.51\pm1.64 $ $9.14\pm2.10 $
$\lbrack$S III$\rbrack$ 9069 $30.67\pm1.50$ $7.24\pm0.85$ $12.60\pm0.51 $ - - $5.22\pm0.37$ $4.15\pm0.40 $ $6.43\pm1.04$ $4.84\pm0.60 $ -
Fe II 9127 - - - - - - - $3.65\pm0.79$   -
Fe II 9177 $2.57\pm0.61$k - - - - - $1.95\pm0.23 $ $1.98\pm0.40$   -
Fe II 9202 - - - - - - $1.58\pm0.26 $ $1.57\pm0.28$   -
H I 9230 - - - - - - $2.78\pm0.29 $ - - -
H I 9230(b) $38.41\pm8.92$a - - - $19.23\pm3.06$ah $11.52\pm1.84$ah $9.77\pm0.88 $ - $21.84~\pm~2.45$ah $11.00\pm1.85$ah
$\lbrack$S III$\rbrack$ 9531 $90.23\pm0.67$ $39.98\pm0.55$ $33.69\pm0.81 $ - $10.58\pm2.14 $ $27.25\pm0.68$ $18.58\pm0.66 $ $6.83\pm0.40$ $16.70\pm1.10 $ $8.84\pm1.73$d
$\lbrack$C I$\rbrack$ 9824 - - - - - - $2.07\pm0.20$ - - $0.35\pm0.07$d
$\lbrack$C I$\rbrack$ 9850 - $2.47\pm0.24$ - - - - $1.00\pm0.09$ - - $0.86\pm0.17$
$\lbrack$S VIII$\rbrack$ 9910 $8.23\pm2.52$ - $5.99\pm0.44 $ - - - $0.66\pm0.06$ - - $0.67\pm0.12$
Fe II 9999 $9.15\pm1.45$ $5.16\pm0.29$d - - $8.34\pm1.02 $ $2.74\pm0.42$ $3.08\pm0.50 $ - $4.33\pm0.74 $ -
H I 10049 - - $ 1.19\pm0.21 $ - - $6.31\pm0.55$ $6.60\pm0.40 $ - $6.86\pm0.69$ -
H I 10049(b) $45.61\pm2.69$a - $35.30\pm3.13$ - $12.08\pm1.31$a $35.54\pm2.02$ $18.13\pm2.16 $ - $5.47\pm2.25 $ $5.81\pm0.85$a
He II 10122 - - - - - - $1.08\pm0.28 $ - - -
He II 10122(b) $13.98\pm1.47$a - $4.00\pm0.37$a - - - $0.57\pm0.20 $ - - -
Fe II 10171 - - - - - - $3.11\pm0.39 $ - $1.68\pm0.08 $ -
$\lbrack$S II$\rbrack$ 10286 - - $ 1.18\pm0.14 $ - - - - - - -
$\lbrack$S II$\rbrack$ 10320 - - $1.72\pm0.14$ - - - - - - -
$\lbrack$S II$\rbrack$ 10336 - - $0.83\pm0.14$ - - - - - - -
$\lbrack$S II$\rbrack$ 10370 - - $0.23\pm0.14$ - - - - - - -
$\lbrack$N I$\rbrack$ 10404 - - $1.04\pm0.21$ - - $2.26\pm0.17$ - - - -
Fe II 10500 - - - $1.36\pm0.21$ $7.18\pm1.77 $ $7.96\pm0.56$ $3.11\pm0.39 $ - $2.78\pm0.27 $ $2.90\pm0.87$
He I 10830 $46.22\pm1.17$ - $69.88\pm1.56 $ - - $44.38\pm1.71$ $16.87\pm0.19 $ $3.96\pm0.32$ $10.87\pm0.28 $ $12.61\pm0.44$
He I 10830(b) $101.76\pm4.81$ $134.83\pm5.24$a $131.51\pm11.66$ $31.77\pm1.60$a $39.46\pm2.40$a $60.57\pm5.11$ $26.74\pm0.55 $ $5.63\pm2.40$ $27.31\pm0.84 $ $26.34\pm1.34$
H I 10938 $20.90\pm2.22$ - - - - $18.67\pm1.57$ $12.01\pm0.22 $ - $7.41\pm0.28 $ $4.91\pm0.39$
H I 10938(b) $19.89\pm2.52$ $27.05\pm3.98$a $5.57\pm1.76$a $10.19\pm1.21$a $24.96\pm2.36 $ $22.72\pm3.76$ $15.57\pm0.79 $ $2.34\pm0.38$a $14.58\pm0.95 $ $9.65\pm1.06$
Fe II 11126 - - $1.84\pm0.42$ - - $3.52\pm0.46$ $1.64\pm0.17 $ $0.85\pm0.20$ $1.86\pm0.10 $ -
O I 11287 $23.17\pm2.13$ - - $4.31\pm0.96$ $9.16\pm1.83 $ $23.03\pm0.36$ $11.33\pm0.53 $ - $10.28\pm0.54 $ $7.04\pm0.62$d
$\lbrack$P II$\rbrack$ 11460 - - - - - - - - - -
$\lbrack$P II$\rbrack$ 11886 - - - - - - - - - -
$\lbrack$S IX$\rbrack$ 12520 - $1.84\pm0.48$ $2.79\pm0.37 $ - - - - - - -
$\lbrack$Fe II$\rbrack$ 12570 $7.39\pm0.37$c $7.22\pm0.46$c $1.71\pm0.26$c - - - - $0.91\pm0.24$c $1.96\pm0.34$c -
H I 12820 $7.73\pm0.62$ $1.43\pm0.26$ $ 5.34\pm0.30 $ - $14.61\pm0.49 $ - - $2.56\pm0.22$ $12.89\pm0.52 $ $10.16\pm0.50$
H I 12820(b) $60.12\pm2.20$ $55.87\pm2.51$ $49.30\pm2.91 $ $19.28\pm0.84$a $13.48\pm1.17 $ 82.70cd - $2.76\pm0.85$ $16.10\pm1.82 $ $13.06\pm1.21$
$\lbrack$Fe II$\rbrack$ 13201 $3.08\pm0.22$ - - - - - - - - -
$\lbrack$Si X$\rbrack$ 14300 - - $5.57\pm0.38 $ - - - - - - -
$\lbrack$Fe II$\rbrack$ 16436 $7.85\pm0.61$c $5.36\pm0.61$c $1.30\pm0.14$c - - - - $0.80\pm0.09$c $1.40\pm0.27$c -
H I 18750 $43.24\pm0.57$ - - - $24.76\pm0.46 $ $31.15\pm0.60$ $26.98\pm1.17 $ $9.44\pm0.20$ $23.83\pm0.51 $ $9.80\pm0.39$
H I 18750(b) $78.26\pm2.49$ $17.45\pm0.50$a 78.87ad $21.35\pm0.73$a $17.21\pm1.46 $ $55.63\pm1.70$ $2.40\pm0.10 $ $4.04\pm1.25$ $14.18\pm1.71 $ $17.79\pm1.06$
H I 19446 $2.24\pm0.30$ - - - - - - - - -
H I 19446(b) $8.90\pm0.99$ - - - - $7.63\pm0.63$a $2.40\pm0.10 $a - - -
$\rm H_2$ 19570 $1.90\pm0.42$c 0.67cd - - - $3.73\pm0.40$c $0.93\pm0.07$c $0.30\pm0.12$c - -
$\lbrack$Si VI$\rbrack$ 19641 $8.96\pm0.29$ - $9.97\pm0.86 $ - - - $1.00\pm0.07 $ - - -
$\rm H_2$ 20332 - $1.04\pm0.16$c - - - - $0.37\pm0.08$c $0.22\pm0.07$c $0.32\pm0.07$c -
He I 20580 - - - - - - - - - -
He I 20580(b) $1.43\pm0.08$a - - - - - $0.42\pm0.10$a $0.47\pm0.05$a - -
$\rm H_2$ 21213 $1.59\pm0.20$c $1.89\pm0.23$c $0.80\pm0.11$c - - $1.26\pm0.15$c $0.45\pm0.08$c $0.47\pm0.10$c $1.04\pm0.20$c -
H I 21654 $1.41\pm0.11$ $0.63\pm0.36$ - - $1.68\pm0.36 $ $1.13\pm0.23$ $1.45\pm0.16 $ $0.36\pm0.04$ $0.85\pm0.12 $ -
H I 21654(b) $9.65\pm0.49$ $8.86\pm2.28$ $16.27\pm2.0$ca - $3.66\pm1.01 $ $6.29\pm0.62$ $2.63\pm0.38 $ $0.91\pm0.13$ $1.77\pm0.25 $ -
$\rm H_2$ 22230 - $0.62\pm0.15$c - - - - - - - -
$\rm H_2$ 22470 $0.40\pm0.13$c $0.56\pm0.15$c - - - - - - - -
$\lbrack$Ca VIII$\rbrack$ 23218 - - $1.66\pm0.38$ - - - - - - -
a Total Flux of the line.
b Broad Component of the line.
c Rodríguez-Ardila et al. (2004).
d Teluric absorption.
e Rodríguez-Ardila et al. (2005).
f Total flux. Line without broad component.
$\xi$ Blend 8446+8498.
h Blend with Fe II $\lambda$9177 $\AA$ and Fe II $\lambda$9202 $\AA$.
k Blend with Fe II$\lambda$ 9202 $\AA$.


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