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Table 3

Measured lines in all the integrated spectra.

I(λ)/I(Hβ)

Line λ   (Å) f(λ)a X1b X2b E1b E2b MB1 MB2 MB3 B1 B2

[OII] 3728 0.322 125.7  ±  13.1 181.0  ±  3.5 281.4  ±  36.1 217.0  ±  19.4 178.5  ±  13.2 274.1  ±  31.9 279.6  ±  35.1 234.4  ±  38.6 112.8  ±  12.9
H9 3835 0.298 10.0  ±  1.5 9.0  ±  3.2 25.0  ±  7.1 ... 10.8  ±  1.7 ... ... ... 9.6  ±  2.3
[NeIII] 3868 0.291 10.8  ±  2.8 31.1  ±  9.3 43.4  ±  16.3 ... 4.1  ±  1.1 29.8  ±  8.4 51.8  ±  15.1 ... 16.1  ±  1.5
H8+HeI 3889 0.286 29.7  ±  2.4 27.3  ±  3.5 6.9  ±  1.8 ... 23.7  ±  2.3 ... ... ... 30.4  ±  0.8
H7 3970 0.266 16.3  ±  0.8 16.0  ±  2.5 ... ... 16.5  ±  3.9 ... ... ... 21.0  ±  3.8
HeI+[NII] 4026 0.251 4.4  ±  0.4 3.5  ±  0.7 ... ... ... ... ... ... ...
Hδ 4101 0.229 29.2  ±  0.1 31.3  ±  0.4 27.6  ±  3.6 26.8  ±  4.0 28.1  ±  1.5 29.3  ±  3.2 26.8  ±  4.8 41.5  ±  7.4 30.0  ±  1.8
Hγ 4340 0.156 52.6  ±  0.2 57.8  ±  0.8 49.4  ±  1.2 47.9  ±  4.5 53.0  ±  1.6 54.4  ±  11.5 55.0  ±  12.7 57.0  ±  14.3 55.8  ±  1.9
[OIII] 4363 0.149 3.5  ±  0.3 18.8  ±  2.7 27.4  ±  14.8 ... ... ... ... ... ...
HeI 4471 0.115 10.1  ±  0.7 9.5  ±  0.6 5.5  ±  1.2 ... 7.7  ±  0.8 ... ... ... 9.0  ±  0.8
[OIII] 4959 –0.026 45.9  ±  0.2 101.0  ±  1.0 108.2  ±  2.9 39.9  ±  0.1 24.4  ±  0.6 111.5  ±  7.0 51.9  ±  4.7 39.3  ±  2.3 81.2  ±  1.0
[OIII] 5007 –0.038 138.1  ±  2.7 299.1  ±  0.4 328.9  ±  11.7 119.9  ±  1.6 74.1  ±  1.0 335.5  ±  8.7 148.5  ±  9.3 110.4  ±  13.3 242.7  ±  1.3
HeI 5015 –0.040 3.7  ±  0.3 1.2  ±  0.1 ... ... ... ... ... ... ...
[NI] 5200 –0.083 ... ... 12.4  ±  2.6 ... 4.1  ±  0.3 8.5  ±  1.7 12.1  ±  3.0 ... 1.9  ±  0.3
[NII] 5755 –0.185 3.0  ±  0.1 ... ... ... 3.3  ±  0.2 ... ... ... 1.2  ±  0.3
HeI 5876 –0.203 28.2  ±  1.4 31.6  ±  3.1 20.4  ±  5.9 ... 22.6  ±  1.0 19.9  ±  3.1 ... ... 23.5  ±  0.9
[SIII] 6312 –0.264 1.3  ±  0.1 ... ... ... ... ... ... ... ...
[NII] 6548 –0.296 135.8  ±  2.8 90.9  ±  2.6 29.2  ±  8.5 25.0  ±  6.7 199.2  ±  10.5 44.3  ±  7.2 27.2  ±  6.0 38.9  ±  6.2 48.3  ±  1.8
Hα 6563 –0.298 324.4  ±  0.3 351.6  ±  0.3 305.8  ±  16.0 295.0  ±  9.7 317.1  ±  16.3 330.8  ±  22.2 313.6  ±  20.4 293.2  ±  43.3 285.1  ±  4.2
[NII] 6584 –0.300 418.1  ±  2.2 274.3  ±  6.2 83.5  ±  11.9 77.5  ±  9.0 581.4  ±  29.4 133.1  ±  11.3 76.3  ±  5.6 111.0  ±  17.0 138.4  ±  2.8
HeI 6678 –0.313 7.0  ±  0.1 6.9  ±  0.3 ... ... 6.0  ±  0.4 ... ... 3.2  ±  0.6 6.2  ±  0.2
[SII] 6717 –0.318 16.9  ±  0.1 25.3  ±  0.5 43.2  ±  3.0 46.0  ±  2.9 34.0  ±  2.1 31.5  ±  2.8 36.5  ±  4.0 42.1  ±  6.9 9.8  ±  0.1
[SII] 6731 –0.320 13.9  ±  0.3 19.1  ±  0.1 28.5  ±  2.4 29.7  ±  2.4 33.2  ±  2.1 20.5  ±  2.5 23.8  ±  3.3 31.7  ±  5.6 7.4  ±  0.2
F(Hβ)c 195.7  ±  3.2 43.0  ±  0.8 3.4  ±  0.1 3.2  ±  0.2 39.1  ±  0.3 5.5  ±  0.2 3.5  ±  0.2 2.7  ±  0.2 31.3  ±  0.2
c(Hβ) 0.75  ±  0.01 0.77  ±  0.01 0.67  ±  0.04 0.66  ±  0.02 0.72  ±  0.07 0.60  ±  0.09 0.69  ±  0.09 0.73  ±  0.21 0.71  ±  0.02

Notes. The intensity values of each emission line (I(λ)/I(Hβ)) are normalized to F(Hβ) = 100 and reddening corrected.

(a)

Adopted reddening curve. Obtained using Cardelli et al. (1989) extintion law with RV = 3.1.

(b)

In these regions intensities are the mean weighted by errors of the different emission lines measured from high and low resolution gratings.

(c)

Hβ fluxes in units of  ×    10-15 erg cm-2 s-1 (not corrected for extinction).

(†)

Lines with bad measure. These lines are not used in determining physical parameters or abundances.

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