Table 1: Results of the excitation temperatures of Si II, corresponding total number of Si II (=$n_{\rm e}$), and abundance ratios of N/O, H/O under the hot component condition.

$T_{\rm ex}$ of Si II[K]
Si II(=$n_{\rm e}$) [ ${\rm cm}^{-3}$] N / O H / O

10 000a
$1.0\pm0.3 \times 10^{18}$ $\rm 18.7^{+36.9}_{-18.7}$ $\rm0.59^{+0.75}_{-0.59}$
$\mid$      

14 000
$3.7\pm0.9 \times 10^{16}$ $\rm 18.8^{+36.8}_{-18.8}$ $\rm0.59^{+0.74}_{-0.59}$

15 000
$2.1\pm0.5 \times 10^{16}$ $\rm 18.8^{+36.6}_{-18.8}$ $\rm0.59^{+0.74}_{-0.59}$

16 000
$1.3\pm0.3 \times 10^{16}$ $\rm 18.9^{+36.5}_{-18.9}$ $\rm0.59^{+0.74}_{-0.59}$

17 000
$8.7\pm2.1 \times 10^{15}$ $\rm 18.9^{+36.3}_{-18.9}$ $\rm0.60^{+0.73}_{-0.60}$

18 000
$6.0\pm1.5 \times 10^{15}$ $\rm 19.0^{+36.0}_{-19.0}$ $\rm0.60^{+0.73}_{-0.60}$
$\mid$      
20 000 $3.3\pm0.8 \times 10^{15}$ $\rm 19.2^{+35.5}_{-19.2}$ $\rm0.60^{+0.72}_{-0.60}$

a Borovicka (1994).

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