Open Access

Table A.1

List and properties of the sample of prestellar core (PSC) candidates.

Region Source RA DEC Mass [range] (1) FWHMdec nH2 tff (2) Location (3)
[deg] [deg] [M] [au] [×106 cm−3] [kyr]
G008.67 #4 271.580761 -21.6237093 7.8 [6.6 – 8.9] 3870 4.1 ± 0.6 15.7 ± 1.2 C
G008.67 #7 271.5800126 -21.6251966 13.7 [11.2 – 16.2] 2780 19.3 ± 3.5 7.2 ± 0.7 C
G008.67 #10 271.5774356 -21.6271193 7.4 [5.9 – 8.9] 4120 3.2 ± 0.6 17.7 ± 1.8 I

G010.62 #4 272.6216933 -19.9291438 11.7 [8.7 – 14.7] 1840 56.7 ± 14.6 4.2 ± 0.6 I

G012.80 #5 273.5482204 -17.9458195 7.4 [6.8 – 8.1] 1450 73.6 ± 6.6 3.7 ± 0.2 I

G327.29 #11 238.2800319 -54.6194279 8.6 [6.6 – 10.6] 3480 6.2 ± 1.4 12.7 ± 1.5 C

G333.60 (4)#1A 245.5468839 -50.0987477 54.0 [35.7 – 72.3] 2640 88.8 ± 30.1 3.4 ± 0.6 C
G333.60 (4)#1B 245.5466503 -50.0988518 40.5 [26.9 – 54.2] 2020 148.8 ± 50.2 2.6 ± 0.5 C
G333.60 #8 245.5282954 -50.1068134 6.7 [5.4 – 8.0] 2510 12.8 ± 2.5 8.8 ± 0.9 C
G333.60 #26 245.535353 -50.1041745 7.0 [4.9 – 9.1] 2310 17.3 ± 5.1 7.6 ± 1.2 I
G333.60 #45 245.549303 -50.0984873 6.4 [4.5 – 8.2] 4370 2.3 ± 0.7 20.8 ± 3.2 C

G337.92 #3 250.2949021 -47.1343006 12.0 [9.2 – 14.8] 2750 17.4 ± 4.1 7.6 ± 0.9 C
G337.92 #5 250.295556 -47.134715 11.2 [8.7 – 13.7] 3450 8.3 ± 1.9 11.0 ± 1.3 C

G338.93 #5 250.1417392 -45.7025004 24.9 [17.4 – 32.4] 1750 140.5 ± 42.4 2.7 ± 0.4 C
G338.93 #7 250.1378537 -45.7040233 10.0 [8.2 – 11.8] 1470 95.4 ± 16.8 3.2 ± 0.3 C
G338.93 #13 250.1423231 -45.6931039 11.1 [9.5 – 12.7] 3090 11.4 ± 1.7 9.4 ± 0.7 I
G338.93 #16 250.1418854 -45.701708 6.5 [4.8 – 8.2] 2930 7.8 ± 2.1 11.3 ± 1.6 C

G353.41 #5 262.6101515 -34.6960014 12.7 [9.9 – 15.6] 2630 21.2 ± 4.7 6.9 ± 0.8 C

W43-MM1 #6 281.9423152 -1.909246 40.5 [37.3 – 43.6] 2030 146.5 ± 11.4 2.6 ± 0.1 I
W43-MM1 #8 281.938703 -1.9102889 8.3 [7.5 – 9.0] 1350 101.6 ± 8.9 3.1 ± 0.1 C
W43-MM1 #14 281.944974 -1.9044595 9.1 [8.4 – 9.7] 1350 111.6 ± 8.2 3.0 ± 0.1 I
W43-MM1 #18 281.9462451 -1.9075171 18.7 [17.9 – 19.4] 1930 78.6 ± 3.0 3.6 ± 0.1 I
W43-MM1 #21 281.9453834 -1.9082357 21.1 [20.3 – 21.9] 2390 46.8 ± 1.7 4.6 ± 0.1 C
W43-MM1 #30 281.9456971 -1.9082389 12.2 [11.8 – 12.6] 1350 150.0 ± 5.4 2.6 ± 0.0 C
W43-MM1 #32 281.9455609 -1.9075139 19.5 [18.8 – 20.1] 2180 56.9 ± 1.9 4.2 ± 0.1 C

W43-MM2 #2 281.9001273 -2.0224281 13.0 [11.7 – 14.3] 2020 47.7 ± 4.8 4.6 ± 0.2 C
W43-MM2 #9 281.9034863 -2.0173945 7.8 [6.7 – 8.8] 2160 23.3 ± 3.3 6.6 ± 0.5 I
W43-MM2 #12 281.9027193 -2.014794 16.0 [14.0 – 18.1] 3390 12.4 ± 1.6 9.0 ± 0.6 I

W43-MM3 #3 281.9207197 -2.0057611 10.8 [9.4 – 12.2] 2420 23.1 ± 3.0 6.6 ± 0.4 C

W51-E #14 290.9326071 14.510126 35.6 [28.8 – 42.3] 2080 119.7 ± 22.7 2.9 ± 0.3 I
W51-E #28 290.9319946 14.5089561 7.5 [6.7 – 8.2] 1600 55.1 ± 5.8 4.3 ± 0.2 C
W51-E #31 290.9288221 14.5159753 9.5 [9.3 – 9.7] 4170 3.9 ± 0.1 15.9 ± 0.2 C

W51-IRS2 #8 290.9091553 14.5185781 17.4 [14.0 – 20.9] 1930 73.4 ± 14.5 3.7 ± 0.4 I
W51-IRS2 #9 290.9103723 14.5113251 16.5 [13.0 – 19.9] 2510 31.5 ± 6.7 5.6 ± 0.6 I
W51-IRS2 #11 290.9187587 14.5177443 23.9 [17.8 – 30.0] 2950 28.2 ± 7.2 6.0 ± 0.8 C
W51-IRS2 #17 290.9245968 14.5197752 11.5 [9.4 – 13.5] 3950 5.6 ± 1.0 13.3 ± 1.2 I
W51-IRS2 #22 290.9255723 14.5112676 7.6 [6.1 – 9.1] 1350 93.5 ± 18.6 3.3 ± 0.3 I
W51-IRS2 #24 290.9114738 14.5186878 7.7 [6.4 – 9.1] 3120 7.7 ± 1.4 11.4 ± 1.0 I
W51-IRS2 #28 290.9052888 14.5184717 10.1 [8.7 – 11.5] 3910 5.1 ± 0.7 14.0 ± 1.0 I
W51-IRS2 #32 290.9069467 14.5064897 9.7 [8.3 – 11.2] 1900 43.0 ± 6.4 4.8 ± 0.4 I
W51-IRS2 #38 290.9262262 14.515357 7.7 [6.1 – 9.4] 1800 40.1 ± 8.6 5.0 ± 0.6 I
W51-IRS2 #42 290.9180791 14.5179626 11.5 [8.7 – 14.2] 2820 15.5 ± 3.7 8.0 ± 1.0 I

Bold font is used to present the robust sample of PSC candidates with M > 16M.

1 Mean masses of the candidates with their range using the non-corrected PPMAP dust temperature (see Dell’Ova et al. 2024) and 20 K as upper and lower limits in temperature.

2 Volume density and free-fall time (see section 4.5).

3 Location of the source with C meaning clustered and I meaning isolated, based on the criteria described in Sect. 4.5.

4 This source contains two continuum peaks that can be seen in the GExt2D second derivative map. We then use the flux density and size of each GExt2D source to compute the masses and densities of the two peaks (see section 4.4).

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