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Table 2

Millimetre properties of LBQS0109, 2QZJ0028 and HB8903.

LBQS0109 2QZJ0028 HB8903

σ3mm [μJy/beam] 12 12 18
S3mm [μJy] 160 ± 16 168 ± 14 5692 ± 12
Major-axis3mm [′′]a 0.5 ± 0.1 0.102 ± 0.006
Axis-ratio3mma 0.5 ± 0.4 1.00 ± 0.06
PA3mm[°]a 85 ± 11 − 90 ± 60
Mdust [109M]b 0.5–0.8 0.6–0.9 20–30
λCO(3 − 2) [mm] 2.9094 ± 0.0004
z CO(3 − 2) 2.3558 ± 0.0005
FWHMCO(3−2) [km s-1] 400 ± 60
SCO(3 − 2)Δv [Jy km s-1]c 0.34 ± 0.03 <0.09 <0.08
[1010 K km s-1 pc2]c 1.04 ± 0.33 <0.3 <0.3
LCO(3 − 2) [107L]c 1.4 ± 0.2 <0.4 <0.3
Mgas(αCO = 0.8) [1010M]c,d 0.8 ± 0.5 <0.2 <0.2
Mgas(αCO = 4) [1010M]c,d 4.0 ± 2.4 <1.2 <1.0

Notes.

(a)

Beam-deconvolved size estimated in the UV-plane by using the UVMODELFIT task.

(b)

Under the assumption that the continuum emission at 3 mm is completely associated to thermal dust continuum emission. We assume a Td = 40–60 K and a β = 2.0.

(c)

For 2QZJ0028 and HB8903, we assume a line width of 400 km s-1 and the upper limits correspond to a 3σ level.

(d)

Assuming a r31 = 1.0 ± 0.5. The statistical errors associated to the molecular gas include r31 uncertainties.

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