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Table A.7:

Dereddened line intensity ratios with respect to I(H$\beta $) = 100 for regions analyzed in IRAS 08208+2816. The slit positions that we used for each knot are: PA 345$^{\circ }$ for C, PA 355$^{\circ }$ for #8 and #10, and PA 10$^{\circ }$ for #3 y #5.
Line $f(\lambda)$ C #3 #5 #8 #10
3728.00 [O II] 0.256 146.8 $\pm$ 9.8 279 $\pm$ 20 251 $\pm$ 24 164 $\pm$ 22 324 $\pm$ 64
3750.15 H I 0.253 1.74 $\pm$ 0.51 ... ... ... ...
3770.63 H I 0.249 1.55 $\pm$ 0.49 ... ... ... ...
3797.90 H I 0.244 2.86 $\pm$ 0.60 3.17: ... ... ...
3835.39 H I 0.237 5.53 $\pm$ 0.79 ... ...... ...  
3868.75 [Ne III] 0.230 32.8 $\pm$ 2.2 15.1 $\pm$ 3.4 26.3 $\pm$ 7.0 5.27: ...
3889.05 H I 0.226 15.1 $\pm$ 1.7 13.5 $\pm$ 3.2 12.9 $\pm$ 5.0 6.36: ...
3967.46 [NeIII]H7 0.210 22.1 $\pm$ 1.9 15.9 $\pm$ 2.9 17.0 $\pm$ 5.3 22.0 $\pm$ 5.7 26.23:
4026.21 He I 0.198 0.92: ... ... ... ...
4068.60 [S II] 0.189 1.14 $\pm$ 0.45 ... ... ... ...
4101.74 H I 0.182 26.1 $\pm$ 2.1 26.1 $\pm$ 2.9 24.1 $\pm$ 5.1 26.1 $\pm$ 5.7 26.23:
4340.47 H I 0.127 46.7 $\pm$ 2.7 46.8 $\pm$ 4.6 43.8 $\pm$ 6.8 43.5 $\pm$ 7.4 46 $\pm$ 15
4363.21 [O III] 0.121 3.12 $\pm$ 0.48 1.66: 2.26: ... ...
4471.48 He I 0.095 4.00 $\pm$ 0.67 3.7 $\pm$ 1.3 ... ... ...
4658.10 [Fe III] 0.050 1.68 $\pm$ 0.58 1.72: ... ... ...
4861.33 H I 0.000 100.0 $\pm$ 5.7 100.0 $\pm$ 8.4 100 $\pm$ 11 100 $\pm$ 12 100 $\pm$ 22
4958.91 [O III] -0.024 152.6 $\pm$ 8.3 76.6 $\pm$ 5.8 104 $\pm$ 10 44.7 $\pm$ 8.9 54 $\pm$ 15
5006.84 [O III] -0.036 470 $\pm$ 24 228 $\pm$ 14 305 $\pm$ 24 89 $\pm$ 13 151 $\pm$ 30
5197.90 [N I] -0.082 1.09 $\pm$ 0.42 ... 2.46: ... ...
5875.64 He I -0.215 12.8 $\pm$ 1.2 12.4 $\pm$ 1.9 14.6 $\pm$ 2.9 12.3 $\pm$ 3.4 11.28:
6300.30 [O I] -0.282 4.74 $\pm$ 0.62 5.6 $\pm$ 1.1 9.8 $\pm$ 2.3 10.1 $\pm$ 3.1 9.00:
6312.10 [S III] -0.283 1.46 $\pm$ 0.42 1.13: ... ... ...
6363.78 [O I] -0.291 1.70 $\pm$ 0.46 ... 3.21: 2.24: ...
6548.03 [N II] -0.318 14.2 $\pm$ 1.1 16.0 $\pm$ 2.4 16.2 $\pm$ 3.9 30.2 $\pm$ 5.3 14.95:
6562.82 H I -0.320 285 $\pm$ 15 283 $\pm$ 20 281 $\pm$ 25 288 $\pm$ 33 286 $\pm$ 51
6583.41 [N II] -0.323 36.9 $\pm$ 2.6 39.2 $\pm$ 4.2 37.8 $\pm$ 5.3 75.3 $\pm$ 9.3 42 $\pm$ 11
6678.15 He I -0.336 3.26 $\pm$ 0.63 3.04 $\pm$ 0.93 ... 2.93: 3.65:
6716.47 [S II] -0.342 22.0 $\pm$ 1.5 40.2 $\pm$ 4.2 52.9 $\pm$ 6.8 66.4 $\pm$ 9.6 50 $\pm$ 13
6730.85 [S II] -0.344 16.6 $\pm$ 1.3 28.5 $\pm$ 3.3 34.5 $\pm$ 5.2 46.7 $\pm$ 7.5 36 $\pm$ 10
7065.28 He I -0.387 2.42 $\pm$ 0.57 ... ... ... ...
7135.78 [Ar III] -0.396 6.37 $\pm$ 0.78 11.8 $\pm$ 3.0 ... ... ...
Aperture size (arcsec)   $1.4 \times 1$ $2.8 \times 1$ $4.0 \times 1$ $6.4 \times 1$ $4.0 \times 1$
Distance (arcsec)b   - 12.6 6.8 8.8 16
F(H$\beta $)a   12.9 $\pm$ 0.5 5.97 $\pm$ 0.28 2.98 $\pm$ 0.19 4.05 $\pm$ 0.34 1.36 $\pm$ 0.18
C(H$\beta $)   0.11 $\pm$ 0.02 0.47 $\pm$ 0.04 0.41 $\pm$ 0.04 0.17 $\pm$ 0.03 0.12 $\pm$ 0.02
$W_{\rm abs}$ (Å)   3.2 $\pm$ 0.1 1.6 $\pm$ 0.2 1.4 $\pm$ 0.2 4.9 $\pm$ 0.1 1.9 $\pm$ 0.1
-W(H$\alpha $) (Å)   331 $\pm$ 18 202 $\pm$ 15 346 $\pm$ 32 89 $\pm$ 10 98 $\pm$ 18
-W(H$\beta $) (Å)   80 $\pm$ 5 56 $\pm$ 5 62 $\pm$ 7 24 $\pm$ 3 17 $\pm$ 4
-W(H$\gamma$) (Å)   30 $\pm$ 2 20 $\pm$ 2 27 $\pm$ 4 10 $\pm$ 2 9 $\pm$ 3
-W([O III]) (Å)   370 $\pm$ 19 130 $\pm$ 8 200 $\pm$ 16 $18 \pm 3$ 19 $\pm$ 4

a In units of 10-15 erg s-1 cm-2 and not corrected for extinction; b relative distance with respect to the center of IRAS 08208+2816.


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