Table 1.

A summary of ALMA 2 mm detected sources.

SourceRADec.zphotzspec|$S_{\rm 2~mm, aperture}^{a}$||$S_{\rm 2~mm, imfit}^{a}$||$S_{\rm 1.2~mm, aperture}^{a,b}$||$S_{\rm 1.2~mm, imfit}^{a,b}$|
(deg)(deg)(mJy)(mJy)
Q2343-BX610356.5393212.822022.052.2107 ± 0.00010.234 ± 0.0100.205 ± 0.0091.72 ± 0.061.48 ± 0.04
G1356.5341912.819792.092.2093 ± 0.0001c0.119 ± 0.0200.125 ± 0.021
G2356.5374412.817310.173 ± 0.0180.166 ± 0.017
G3356.5429212.823630.077 ± 0.0140.072 ± 0.0160.50 ± 0.110.50 ± 0.15
G4356.542812.820732.13d0.037 ± 0.0130.040 ± 0.0090.13 ± 0.100.17 ± 0.09
G5356.5456912.819980.173.01?0.141 ± 0.0290.175 ± 0.061
SourceRADec.zphotzspec|$S_{\rm 2~mm, aperture}^{a}$||$S_{\rm 2~mm, imfit}^{a}$||$S_{\rm 1.2~mm, aperture}^{a,b}$||$S_{\rm 1.2~mm, imfit}^{a,b}$|
(deg)(deg)(mJy)(mJy)
Q2343-BX610356.5393212.822022.052.2107 ± 0.00010.234 ± 0.0100.205 ± 0.0091.72 ± 0.061.48 ± 0.04
G1356.5341912.819792.092.2093 ± 0.0001c0.119 ± 0.0200.125 ± 0.021
G2356.5374412.817310.173 ± 0.0180.166 ± 0.017
G3356.5429212.823630.077 ± 0.0140.072 ± 0.0160.50 ± 0.110.50 ± 0.15
G4356.542812.820732.13d0.037 ± 0.0130.040 ± 0.0090.13 ± 0.100.17 ± 0.09
G5356.5456912.819980.173.01?0.141 ± 0.0290.175 ± 0.061

aThe continuum flux is measured using the aperture of 1.00 arcsec in the natural weighting map either based on the aperture photometry and 2D Gaussian fitting using imfit function in casa.

bFor 1.2 mm, we used the ALMA archival data (project code: 2015.1.00250.S) with 0.32 arcsec × 0.29 arcsec resolution for G4 and G3. For Q2343-BX610, we used a tapered map at 0.40 arcsec × 0.37 arcsec based on the investigation of the growth curve.

cG1’s redshift is based on CO (4−3) and [C i], detections and more details of line emitting sources will be presented in Lee et al. (in preparation).

dThe z = 2.21 solution is not rejected. See Section 3.2 and Fig. 3.

Table 1.

A summary of ALMA 2 mm detected sources.

SourceRADec.zphotzspec|$S_{\rm 2~mm, aperture}^{a}$||$S_{\rm 2~mm, imfit}^{a}$||$S_{\rm 1.2~mm, aperture}^{a,b}$||$S_{\rm 1.2~mm, imfit}^{a,b}$|
(deg)(deg)(mJy)(mJy)
Q2343-BX610356.5393212.822022.052.2107 ± 0.00010.234 ± 0.0100.205 ± 0.0091.72 ± 0.061.48 ± 0.04
G1356.5341912.819792.092.2093 ± 0.0001c0.119 ± 0.0200.125 ± 0.021
G2356.5374412.817310.173 ± 0.0180.166 ± 0.017
G3356.5429212.823630.077 ± 0.0140.072 ± 0.0160.50 ± 0.110.50 ± 0.15
G4356.542812.820732.13d0.037 ± 0.0130.040 ± 0.0090.13 ± 0.100.17 ± 0.09
G5356.5456912.819980.173.01?0.141 ± 0.0290.175 ± 0.061
SourceRADec.zphotzspec|$S_{\rm 2~mm, aperture}^{a}$||$S_{\rm 2~mm, imfit}^{a}$||$S_{\rm 1.2~mm, aperture}^{a,b}$||$S_{\rm 1.2~mm, imfit}^{a,b}$|
(deg)(deg)(mJy)(mJy)
Q2343-BX610356.5393212.822022.052.2107 ± 0.00010.234 ± 0.0100.205 ± 0.0091.72 ± 0.061.48 ± 0.04
G1356.5341912.819792.092.2093 ± 0.0001c0.119 ± 0.0200.125 ± 0.021
G2356.5374412.817310.173 ± 0.0180.166 ± 0.017
G3356.5429212.823630.077 ± 0.0140.072 ± 0.0160.50 ± 0.110.50 ± 0.15
G4356.542812.820732.13d0.037 ± 0.0130.040 ± 0.0090.13 ± 0.100.17 ± 0.09
G5356.5456912.819980.173.01?0.141 ± 0.0290.175 ± 0.061

aThe continuum flux is measured using the aperture of 1.00 arcsec in the natural weighting map either based on the aperture photometry and 2D Gaussian fitting using imfit function in casa.

bFor 1.2 mm, we used the ALMA archival data (project code: 2015.1.00250.S) with 0.32 arcsec × 0.29 arcsec resolution for G4 and G3. For Q2343-BX610, we used a tapered map at 0.40 arcsec × 0.37 arcsec based on the investigation of the growth curve.

cG1’s redshift is based on CO (4−3) and [C i], detections and more details of line emitting sources will be presented in Lee et al. (in preparation).

dThe z = 2.21 solution is not rejected. See Section 3.2 and Fig. 3.

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