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Table 5.

Emission line observed fluxes (in units of 10−17 erg s−1 cm−2), emission line ratios, and main properties (ionization parameter U, and gas phase metallicity, in terms of oxygen abundance and relative to solar) of the LAEs and confirmed companions, from their integrated spectra reported in Figs. 9 and 11.

LAE1a LAE1b LAE2 C1 C2 C3 C4
Hα 15.8 ± 1.3 27.0 ± 0.9 4.9 ± 0.5 12.0 ± 1.1 2.1 ± 0.2 12.3 ± 0.7 1.35 ± 0.10
Hβ 16.4 ± 1.9a 21 ± 3a < 0.9 4 ± 2 < 0.4 5.7 ± 1.3 < 0.3
[Ne III] λ3869 Å 7.5 ± 1.4 7.7 ± 1.6 < 0.8 3.2 ± 1.9 < 1.1 < 2 < 0.5
[N II] λ6584 Å < 0.4 4.14 ± 0.15 2.54 ± 0.11 < 0.7 0.78 ± 0.14 9.4 ± 0.6 0.51 ± 0.06
[O II] λ3727,29 Å 36 ± 2 44 ± 2 < 1.6 11 ± 2 3.6 ± 0.7 19 ± 2 < 1.0
[O III] λ5007 Å 79 ± 4 70 ± 2 < 0.9 40 ± 3 6.8 ± 0.6 12.5 ± 1.2 4.2 ± 0.3

Hα/Hβ 3.0 ± 1.6 2.2 ± 0.5
log([N II]/Hα) <  − 1.6 −0.82 ± 0.02 −0.29 ± 0.05 < −1.2 −0.43 ± 0.09 –0.12 ± 0.04 –0.42 ± 0.06
log([O III]/Hβ) 0.68 ± 0.06 0.53 ± 0.07 1.0 ± 0.2 > 1.3 0.34 ± 0.11 > 1.2
log([O III]/[O II]) 0.34 ± 0.04 0.21 ± 0.03 0.57 ± 0.11 0.28 ± 0.10 −0.18 ± 0.07

log(U) −2.75 ± 0.03 −2.86 ± 0.02 –2.56 ± 0.09 −2.80 ± 0.08 −3.16 ± 0.05
12+log(O/H) 8.19 0.22 + 0.17 $ _{-0.22}^{+0.17} $ 8.35 0.14 + 0.12 $ _{-0.14}^{+0.12} $ 8.77 0.19 + 0.17 $ _{-0.19}^{+0.17} $ 8.08 0.25 + 0.19 $ _{-0.25}^{+0.19} $ 8.47 0.16 + 0.13 $ _{-0.16}^{+0.13} $ 8.58 0.07 + 0.06 $ _{-0.07}^{+0.06} $ 8.77 0.22 + 0.17 $ _{-0.22}^{+0.17} $
Z/Z b 0.31 0.12 + 0.15 $ _{-0.12}^{+0.15} $ 0.45 0.12 + 0.15 $ _{-0.12}^{+0.15} $ 1.2 0.4 + 0.6 $ _{-0.4}^{+0.6} $ 0.25 0.11 + 0.14 $ _{-0.11}^{+0.14} $ 0.60 0.18 + 0.21 $ _{-0.18}^{+0.21} $ 0.77 0.11 + 0.12 $ _{-0.11}^{+0.12} $ 1.2 0.5 + 0.6 $ _{-0.5}^{+0.6} $

Notes. aThese measurements should be taken with caution due to the presence of spikes at the wavelengths of Hβin the spectrum of LAE1 (see Fig. 9); for this reason, we have not used the ratios involving this line to estimate the metallicity of LAE1a and LAE1b. bAssuming a solar photospheric value of 12+log(O/H) = 8.69 (Asplund et al. 2009).

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