Open Access
Table A.3.
Derived ne and Te for both high- and low-excitation regions from fully iterative extinction correction/plasma diagnostics with original-to-revised ratios.
| M1687 | Ratio | M2068 | Ratio | M2538 | Ratio | |
|---|---|---|---|---|---|---|
| Te([O III]) | 12940±420 | 0.983 | 11250±310 | 0.945 | 12870±550 | 0.942 |
| ne([Ar IV]) | 22340±3510 | 1.386 | 18020±2530 | 1.970 | 4430±1230 | 1.563 |
| Te([N II]) | 25650±1690 | 0.842 | 13020±1110 | 0.795 | 12600±580 | 0.947 |
| ne([S II]) | 4720±1320 | 0.977 | 11010±5120 | 1.771 | 3340±880 | 1.002 |
| M50 | Ratio | M1596 | Ratio | M2471 | Ratio | |
| Te([O III]) | 11670±320 | 0.984 | 12030±340 | 0.992 | 12380±380 | 0.954 |
| ne([Ar IV]) | 9780±1690 | 1.364 | 5410±1100 | 1.116 | 3640±930 | 1.312 |
| Te([N II]) | 13030±670 | 0.979 | 11770±450 | 0.994 | 11390±420 | 0.959 |
| ne([S II]) | 5980±2120 | 1.081 | 3460±1030 | 1.019 | 3220±870 | 1.000 |
| M2860 | Ratio | M1074 | Ratio | M1675 | Ratio | |
| Te([O III]) | 10660±310 | 0.939 | 12110±340 | 0.976 | 11000±270 | 0.959 |
| ne([Ar IV]) | 6000±1070 | 1.527 | 15590±2480 | 1.438 | 5170±1050 | 1.720 |
| Te([N II]) | 13780±560 | 0.910 | 13120±480 | 0.977 | 11380±860 | 1.002 |
| ne([S II]) | 3440±890 | 0.994 | 2750±710 | 1.006 | 10330±4680 | 2.351 |
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