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Table 2

N2H+ (3–2) observational parameters, distances, and virial masses.

IRDC IR-darka Positionb TMB ΔV vLSR Dc Mvird Ncle Me
clump 8/24 RA Dec
(J2000) (J2000) (K) (km s-1) (km s-1) (kpc) (M) (M)

G329P1 N/N 16:00:17.3 −53:09:18 (0.25) 22 209
G329P2 Y/N 16:00:32.2 −53:12:39 3.20(0.19) 6.69(0.19) −43.42(0.08) 3.0 2444/1466 1 2692
G329P3 Y/Y 16:00:38.5 −53:13:41 (0.23) 12 211
G329P4 Y/Y 16:00:47.7 −53:15:01 (0.25) 37 56
G329P5 N/N 16:01:10.1 −53:16:02 3.26(0.32) 5.83(0.17) −42.00(0.08) 2.9 1642/985 3 867
G331P1 Y/Y 16:10:08.7 −51:22:52 0.86(0.17) 1.79(0.50) −45.10(0.18) 3.1 135/81 6 168
G331P2 N/N 16:10:26.9 −51:22:42 1.26(0.25) 5.60(0.49) −45.31(0.25) 3.1 1976/1185 1 553
G335P1 N/N 16:29:22.2 −49:12:24 3.88(0.33) 4.14(0.14) −39.83(0.05) 3.0 612/367 1 1002
G335P2 Y/N 16:29:27.4 −48:56:51 (0.25) 32 89
G335P3 N/N 16:29:37.8 −48:58:58 (0.24) 13 488
G335P4 N/N 16:30:05.3 −48:48:37 2.29(0.27) 5.53(0.26) −44.40(0.12) 3.2 1477/886 2 664
G337P1 N/N 16:37:35.8 −47:39:27 0.78(0.11) 2.49(0.59) −39.56(0.24) 3.0 234/140 12 85
G337P2 N/N 16:37:47.4 −47:38:59 0.94(0.26) 3.61(0.72) −40.85(0.30) 3.1 1095/657 3 937
G343P1 N/N 17:00:20.7 −42:49:08 (0.23) 4 281
G343P2 N/N 17:00:39.6 −42:51:28 1.27(0.14) 1.59(0.50) −27.42(0.14) 2.7 122/73 13 104
G343P3 Y/Y 17:01:00.4 −42:48:05 (0.23) 6 252
G345P1 N/N 17:05:10.5 −41:29:01 3.44(0.33) 5.85(0.15) −26.32(0.07) 2.8 1150/690 1 2630
G345P2 Y/Y 17:05:16.5 −41:26:14 0.80(0.17) 5.26(0.76) −26.04(0.37) 2.8 3137/1882 7 1520

Notes.Parameters are obtained from Gaussian fits. For non-detections, the values given in parenthesis represent the spectra 1σrms noise level.

(a)

“Y” means the clump is 8 μm- or 24 μm-dark and “N” means the clump is 8 μm- or 24 μm-bright.

(b)

Units of right ascension are hours, minutes, and seconds and units of declination are degrees, arcminutes, and arcseconds.

(c)

Derived (near) kinematic distances by using the N2H+ (3–2) line (see Sect. 4.1).

(d)

Virial mass of clumps estimated using two density distributions. The first value corresponds to a constant density distribution while the second value corresponds to a density distribution that varies as ρ ∝ 1/r2.

(e)

Associated Gaussclumps running number and gas mass (see Sect. 4.2 and Table 3).

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