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Table 2

Observed MIR and FIR fluxes for the line and broadband emission.

Flux ± uncertainty Ionization
Line Wavelength (× 10-16 W m-2) Critical density potential
(μm) Region I Region II (cm-3) (eV)

[S iv] 10.51 5.68 ± 0.21 8.40 ± 0.10 5 × 104 [e] 34.79
[Ne ii] 12.81 8.98 ± 0.22 4.13 ± 0.11 7 × 105 [e] 21.56
[Ne iii] 15.56 18.70 ± 0.14 14.25 ± 0.08 3 × 105 [e] 40.96
[S iii] 18.71 11.78 ± 0.20 6.85 ± 0.08 2 × 104 [e] 23.34
[S iii] 33.48 18.71 ± 0.27 8.20 ± 0.12 7 × 103 [e] 23.34
[O i] 63.18 10.11 ± 0.35 4.06 ± 0.21 5 × 105 [H]
[O iii] 88.36 31.86 ± 0.62 13.50 ± 0.40 5 × 102 [e] 35.12
[N ii] 121.90 0.44 ± 0.20 0.14 ± 0.08 3 × 102 [e] 14.53
[O i] 145.52 0.65 ± 0.09 0.32 ± 0.07 1 × 105 [H]
[C ii] 157.74 26.34 ± 0.33 10.05 ± 0.21 50 [e], 3 × 103 [H] 11.26
Flux density ± uncertainty
Broadband Wavelength (Jy)
( μm) Region I Region II

MIPS 24 0.67 ± 0.01 0.48 ± 0.01
PACS 70 7.36 ± 0.21 3.72 ± 0.12
PACS 100 7.91 ± 0.19 4.10 ± 0.11
PACS 160 6.07 ± 0.10 3.23 ± 0.06

LTIR (erg s-1) 3–1100 5.25 × 1041 3.02 × 1041

Notes. Uncertainties on the fluxes include data and line-fitting uncertainties, but not calibration uncertainties, which are on the order of 5% for the Spitzer lines and 15% for the Herschel lines. Critical density and ionization potential values are taken from Cormier et al. (2012). Critical densities are noted [e] for collisions with electrons and [H] for collisions with hydrogen atoms.

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