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Table 4.

Dust and molecular gas properties of the galaxy sample.

Target znebular(a) SFRIR(b) Mmolgas(c) Mdust(d) tdepl(e,f) fmolgas(f) ϵSF(f)
(M yr−1) (1010M) (107M) (Myr) (%)
J1322+0423 2.0800 < 26 < 0.76 < 1.09 < 42 < 0.69 > 31
J0146–0220 2.1595 81 ± 29 1.28 ± 0.09 3.32 ± 1.78 61 ± 23 0.79 ± 0.11 21 ± 3
J1415+2036 2.2435 < 34 < 1.11 ± 0.23 < 1.38 < 50 ± 11 < 0.86 ± 0.20 > 14 ± 3
J1249+1550 2.2928 85 ± 30. 0.73 ± 0.05 3.42 ± 1.79 36 ± 13 0.63 ± 0.09 37 ± 5
J0006+2452 2.3796 283 ± 98 3.67 ± 0.21 11.1 ± 5.7 71 ± 25 0.92 ± 0.11 8 ± 0.9
J0850+1549 2.4235 59 ± 20 < 0.75 2.30 ± 1.18 < 30 < 0.80 > 20
J1220–0051 2.4269 96 ± 33 1.01 ± 0.10 3.73 ± 1.90 42 ± 15 0.87 ± 0.13 13 ± 2
J0950+0523 2.4548 185 ± 63 2.01 ± 0.12 7.15 ± 3.63 55 ± 19 0.91 ± 0.15 9 ± 1
J1220+0842 2.4698 < 57 < 1.12 < 2.20 < 31 < 0.76 > 24
J1157+0113 2.5450 141 ± 48 1.08 ± 0.10 8.97 ± 2.68 44 ± 16 0.85 ± 0.31 15 ± 6
J0121+0025 3.2445 71 ± 22 < 1.11 ± 0.32 3.75 ± 1.08 < 32 ± 14 < 0.71 ± 0.25 > 29 ± 10
J1316+2614 3.6122 74 ± 21 < 0.63 3.53 ± 1.01 < 13 < 0.60 > 40

Notes.

(a)

Redshifts derived from optical nebular emission lines.

(b)

Obscured SFRs derived from the IR luminosities (Table 3) following the calibration of Kennicutt (1998) for the Chabrier (2003) IMF, SFRIR = LIR/1010. For SFRIR non-detections, we considered the LIR 4σ upper limits.

(c)

Molecular gas masses computed from the CO(3–2) or CO(4–3) luminosities (Table 2) following Eq. (1) and assuming here the CO-to-H2 conversion factor derived for nearby starbursts, α CO SB = 1 M ( K km s 1 pc 2 ) 1 $ \alpha_{\mathrm{CO}}^{\mathrm{SB}} = 1\,M_{\odot}\,\rm (K\,km\,s^{-1}\,pc^2)^{-1} $ (Sect. 3.2).

(d)

Dust masses derived from the FIR fluxes (Table 3) following Eq. (2) (Sect. 3.3).

(e)

Molecular gas depletion timescales derived using the total SFRUV+IR.

(f)

Molecular gas depletion timescales, molecular gas mass fractions, and star-formation efficiencies defined in Sects. 4.2 and 4.3, and all computed here with α CO SB $ \alpha_{\mathrm{CO}}^{\mathrm{SB}} $.

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