Table 1: The measured lines are given in Col. 3. The last column gives the ratio of the line intensity to H$\beta $(=100).
Ident. $\lambda $($\mu $m) Intensity$^\dagger$ I/H $\beta^\sharp$
? 9.98 6.52 0.96
[S IV] 10.51 1665 321
H I 9-7 11.30 4.27 0.806
[Cl IV] 11.76 4.50 0.844
H2 12.28 3.53 0.65
H I7-6(11-8) 12.37 10.2 1.89
[Ne II] 12.81 235 43.5
[Ar V] 13.10 3.41 0.63
[Ne V] 14.31 2.78 0.51
[Cl II] 14.36 7.68 1.41
[Ne III] 15.55 2708 497
H2 17.03 1.83 0.336
[S III] 18.70 994 184
[Cl IV] 20.31 10.47 1.07
[Ar III] 21.81 41.0 4.19
[Fe III] 22.92 3.68 0.376
[Ne V] 24.31 3.89 0.396
[O IV] 25.87 900 91.5
[Fe II] 25.98 2.51 0.255
Hi9-8 27.78 2.66 0.27
[S III] 33.46 1185 120
[Si II] 34.80 158 16.0
[Ne III] 35.99 424 42.8
$^\dagger$ The intensity is measured in units of 10-14 erg cm-2 s-1.
$^\sharp$ In the ratio of intensity to H$\beta $ the intensities below 19 $\mu $m are multiplied by a factor 1.8 to correct for part of the nebula being outside the diaphragm. A reddening correction is also made but it is very small.


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