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Table 3:

Relative line fluxes.
  Area SI Area SII Area EI Area EII
Line (Å) Fa S/Nb F S/N F S/N F S/N
H$\beta$ 4861 <6   <6   <4   <4  
[O I] 6300 43.5 (23) 31.3 (16) 31.7 (33) 67.0 (18)
6548 50.5 (25) 54.5 (25) 48.6 (44) 29.4 (9)
H$\alpha $ 6563 100 (45) 100 (45) 100 (83) 100 (26)
6584 167.6 (64) 167.1 (67) 135.0 (101) 98.8 (25)
6716 97.1 (42) 93.8 (41) 88.1 (70) 109.8 (27)
6731 74.8 (32) 73.9 (32) 66.4 (58) 74.4 (19)
Absolute H$\alpha $ fluxc 2.5 1.9 4.6 1.8
/H$\alpha $ 1.72 $\pm$ 0.05 1.68 $\pm$ 0.05 1.54 $\pm$ 0.03 1.84 $\pm$ 0.09
F(6716)/F(6731) 1.30 $\pm$ 0.05 1.27 $\pm$ 0.05 1.33 $\pm$ 0.03 1.48 $\pm$ 0.09
[N II]/H$\alpha $ 2.18 $\pm$ 0.06 2.22 $\pm$ 0.06 1.84 $\pm$0.03 1.28 $\pm$ 0.07
c(H$\beta$)d >2.2 >2.2 >2.7 >2.7
a Observed fluxes normalized to F(H$\alpha $) = 100 and uncorrected for interstellar extinction.
b Numbers in parentheses represent the signal to noise ratio of the quoted fluxes.
c In units of 10-17 erg s-1 cm-2 arcsec-2.
d The logarithmic extinction is derived by c = 1/0.348 $\times$ log((H$\alpha $/H$\beta$) $_{\rm obs}$/2.85).
Listed fluxes are a signal to noise weighted average of two fluxes for area S.
The errors of the emission line ratios are calculated through standard error propagation.


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