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Table A.1

Observed and de-reddened line fluxes relative to Hβ=100.

Line (Å) F(λ) I(λ)
Hβ 100 100
[O III] 4959 435.0±8.7 432.0±8.7
[O III] 5007 1314±26.4 1299.0±26.5
[N I] 5200 0.016±0.002 0.016±0.002
He II 5412 2.14±0.11 2.05±0.1
[Cl III] 5517 0.032±0.03 0.31±0.03
[Cl III] 5538 0.30±0.03 0.28±0.03
[N II] 5755 0.052±0.007 0.064±0.007
0.032±0.03 0.049±0.005
He I 5876 11.97±0.63 12.0±0.6
[O I] 6300 0.105±0.011 0.096±0.010
[S III] 6312 0.76±0.08 0.70±0.08
[O I] 6363 0.041±0.001 0.04±0.01
[N II] 6548 0.76±0.04 0.70±0.04
Hα 319.0±6.4 287.0±6.4
[N II] 6584 2.33±0.12 2.10±0.12
He I 6678 3.30±0.17 3.0±0.21
[S II] 6716 0.31±0.02 0.27±0.02
[S II] 6731 0.42±0.02 0.37±0.02
[Ar III] 7136 8.77±0.46 7.7±0.5
[O II] 7320 0.63±0.07 0.55±0.06
0.54±0.06 0.46±0.07
[O II] 7330 0.56±0.06 0.50±0.06
0.45±0.05 0.38±0.07
[C I] 8727 0.008±0.0001 0.0070±0.0001
[S III] 9069 7.6±0.4 6.3±0.5
F(Hβ)×10−14 140.0±1.4
c(Hβ) 0.14

Notes. The fluxes are integrated for a pseudo-slit that covers the whole PN (36.8″ × 42.6″ and centered at the center of the PN). (a)For [N II] λ5755, the flux was estimated from the raw map (b)F(Hβ) is the reddened Hβ flux in unit erg cm−2 s−1. (†) The second row represents the values after correction for recombination contribution.

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