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Table 8:

Estimated FMK pre-shock ionic abundances $n_{\rm ion}/n_{\rm O}$ computed assuming that the lines originate only in the pre-shock PIR. (See text for details).

Line
I/I(5007 Å) $T_{\rm e}$, K $n_{\rm e}$, cm-3 $\varepsilon$, cm3/s IP, eV $\Delta t$, s $n_{\rm ion}/n$(O) $n_{\rm element}$/n(O) **
[Ar II] 6.985 $\mu $m 0.5 $2.0 \times 10^4$ 100 $4 \times 10^{-8}$ 27.6 $5 \times 10^6$ 1.0* 0.005
[Ar V] 13.07 $\mu $m 0.003 7000 250 $8\times10^{-7}$ 75.1 $5\times10^7$ $8\times10^{-5}$ 0.005
[Ne II] 12.81 $\mu $m 0.10 $1.5\times10^4$ 150 $5\times10^{-8}$ 41.0 $1.4\times10^7$ 0.06 0.02
[Fe II] 17.94 $\mu $m 0.03 $2.0 \times 10^4$ 50 $1.1\times10^{-8}$ 16.2 $9\times10^5$ 5.5* 0.005
[S III] 33.48 $\mu $m 0.04 $1.5\times10^4$ 150 $3.0\times10^{-7}$ 34.8 $1\times10^7$ 0.015 0.05
[Si II] 34.81 $\mu $m 0.07 $2.0 \times 10^4$ 50 $1.5\times10^{-7}$ 16.4 $1\times10^6$ 0.7* 0.05
[O III] 88.36 $\mu $m 0.10 $1.0\times10^4$ 200 $4.0\times10^{-8}$ 54.9 $3\times10^7$ 1.1 1.0

* Shown to arises mostly in the post-shock photoionized region; see Sect. 5; ** atomic number densities with respect to oxygen, see Table 9.


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