Table 3.
Object | (Te, log
Ne)
|
(Te, log Ne)other | Ref.* | ||
---|---|---|---|---|---|
(R1, R2) | (R1, R3) | (R1, R4) | |||
NGC 2440 | — | I, 3.4 | — | 11,750, 3.7 | 22 |
NGC 6537 | 7,500, 4.2 | — | — | 9,200, 4.3 | 24 |
NGC 6572† | 10,000, 4.2 | 14,000, 4.3 | 11,000, 4.2 | 11,000, 4.2 | 25 |
NGC 6572‡ | 12,500, 4.2 | I, 4.2 | 14,000, 4.2 | 11,000, 4.2 | 25 |
NGC 6741 | 12,000, 3.8 | — | I, 3.8 | 11,750, 3.7 | 26 |
NGC 6884 | I 3.9 | — | — | 11,750, 4.1 | 21 |
NGC 7009 | I, 3.6 | — | I, 3.6 | 11,500, 3.6 | 27 |
NGC 7027 | 12,500, 4.9 | 13,500, 4.9 | 11,000, 4.9 | 14,000, 4.8 | 14 |
NGC 7662 | — | — | I, 3.5 | 12,000, 3.7 | 28 |
IC 2165 | — | I, 3.4 | I, 3.4 | 9,750, 3.6 | 15 |
IC 4997† | I, 4.3 | I, 4.3 | I, 4.3 | 10,000, 4.2 | 29 |
IC 4997‡ | I, 4.1 | I, 4.1 | I, 4.1 | 10,000, 4.2 | 29 |
Hubble 12 | I, 4.3 | I, 4.3 | I, 4.3 | 12,500, 4.4 | 30 |
Te values are in K, Ne values are in cm−3. I indicates that Te was indeterminate due to the observed R2, R3, or R4 line ratio lying outside the range of values given in Fig. 1 or 2. In these instances, log Ne was deduced from R1 by adopting Te = 10,000 K.
*References for sources of (Te, log Ne)other.
†Observations taken in 1990.
‡Observations taken in 1991.