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Table 5

Summary of gas-phase abundances in the Orion nebula.

A ϵ(A) Data Source Method Major uncertainties

C 8.40  ±  0.25 CEL: C iii]1907,09 Rubin et al. (1993) model dereddening, CII not fitted
8.37  ±  0.03 RL: C ii C++: E04 icf (own model)
N 7.92  ±  0.09 CEL: [N ii]6584 data: E04, N+: this paper icf (own model) icf
O 8.52  ± 0.01 CEL: [O iii]5007, [O ii]3727 data: E04, O+ & O++: this paper no icf needed
8.65  ±  0.03 RL: O iii O++: E04 icf (own model)
Ne 8.05  ±  0.03 CEL: [Ne iii]3869 data: E04, Ne++: this paper icf (own model)
7.84  ±  0.03 CEL: [Ne iii]3869 data: E04, Ne++: this paper icf (classical)
8.25  ±  0.35 RL: Ne ii Ne++: E04a icf (own model)
8.03  ±  0.26 RL: Ne ii Ne++: E04a icf (classical)
S 6.87  ±  0.06 CEL: [S iii]9069 data: E04, S++: this paper icf (own model)
Ar 6.39  ±  0.03 CEL: [Ar iii]7135 data: E04, S++: this paper icf (own model)
Mg 6.50 :: CEL: Mg ii 2798 Baldwin et al. (1991) model intensity, interstellar absorption
Si 6.50  ±  0.25 CEL: Si iii]1883,92 Rubin et al. (1993) model Si/C more accurate than Si/H
Fe 6.0  ±  0.3 CEL: [Fe ii], [Fe iii], [Fe iv] Rodríguez & Rubin (2005) model sum of observed ions gives
different result

Notes. 

(a)

The uncertainty for Ne++ was erroneaously given as 0.09 dex in E04, instead of 0.2 dex (García-Rojas, private communication).

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