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Table A.2

Physical parameters and radio continuum emission of the identified cores.

Source Tex NH2 Rcore Fcm IR emission
(K) (1022 cm-2) (pc) (mJy)
(1) (2) (3) (4) (5) (6)

G008.68-0.37 24.1(1.7) 07.77(02.33) 2.2 < 2.3m p, d
G010.47+0.03 16.8(1.2) 02.15(00.65) 1.8 65.52m d
G010.62-0.38 29.3(2.1) 03.05(00.92) 1.2 1899.45m d
G012.03-0.04 17.5(1.2) 01.91(00.57) 1.6 < 2.3m p
G012.79-0.19 25.2(1.7) 29.16(08.73) 1.6 727.65m p, d
G014.33-0.64(1) 22.3(1.6) 04.21(01.26) 0.7 < 2.3m p
G014.33(2) 20.3(1.4) 09.28(02.76) 0.7 < 2.3m d
G014.33(3) 18.5(1.3) 08.34(02.49) 0.7 < 2.3m none
G014.33(4) 18.5(1.3) 10.70(03.21) 0.9 < 2.3m none
G015.03-0.68 46.6(3.2) 40.69(12.18) 0.8 1622.92m d
G029.86-0.05(1) 20.2(1.4) 17.52(05.25) 3.0 869m p
G029.86(2) 25.2(1.7) 10.23(03.06) 2.3 543m d
G029.86(3) 25.5(1.7) 22.46(06.72) 2.2 < 2.3m d
G030.82-0.05(1) 26.7(1.9) 05.04(01.51) 2.5 < 2.3m d
G030.82(2) 22.3(1.5) 11.39(03.39) 1.9 103.91m d
G030.82(3) 14.4(1.0) 23.64(07.08) 2.9 195.44m d
G031.41+0.31 17.5(1.2) 02.33(00.70) 7.4 755.83m d
G035.19-0.74(1) 23.5(1.6) 09.05(02.70) 0.8 144.45m p, d
G035.19(2) 33.5(2.3) 11.98(03.57) 1.5 < 2.3m none
G035.20-1.73(1) 18.5(1.3) 09.52(02.85) 1.4 < 2.3m d
G035.20(2) 18.5(1.3) 05.39(01.59) 1.0 < 2.3m d
G045.44+0.07 16.8(1.1) 06.34(01.89) 3.8 146.97m p, d
G059.78+0.06(1) 21.8(1.5) 03.39(00.99) 1.3 < 2.3m p, d
G059.78(2) 18.5(1.3) 04.93(01.47) 1.3 19.40m p
G059.84+0.66(1) 14.4(1.0) 02.18(00.65) 1.1 < 2.3m p, d
G059.84(2) 10.1(0.7) 00.82(00.24) 1.6 < 2.3m none
G069.52-0.97 22.5(1.6) 02.50(00.75) 0.5 98g p
G080.85+0.43(1) 18.1(1.3) 03.21(00.96) 0.7 16.26g p, d
G080.85(2) 20.5(1.4) 02.82(00.84) 0.7 < 6g p, d
G080.85(3) 16.5(1.1) 02.93(00.87) 0.7 < 6g none
G080.85(4) 16.5(1.1) 04.34(01.29) 0.8 < 6g none
G094.58-1.79 22.8(1.6) 00.88(00.26) 2.0 8r p, d
G136.84+1.12(1) 23.5(1.6) 02.11(00.63) 2.9 < 6g p
G136.84(2) 21.8(1.5) 05.28(01.56) 3.6 < 6g p
G173.49+2.42 44.5(3.1) 03.09(00.93) 0.8 < 6g p
G173.69+2.87 28.5(2.0) 03.52(01.05) 0.8 < 6g d
G173.71+2.35(1) 09.1(0.6) 00.70(00.21) 0.4 < 6g none
G173.71+2.35(2) 10.1(0.7) 00.46(00.12) 0.4 < 6g none
G173.71(3) 09.1(0.6) 00.69(00.18) 0.7 < 6g none
G174.19-0.09 19.0(1.3) 03.48(01.04) 0.7 p
G183.34+0.59 18.5(1.3) 03.52(01.05) 1.0 70g p
G188.79+1.02 21.3(1.5) 01.96(00.59) 0.9 0.6k p, d
G188.95+0.89 23.1(1.6) 02.24(00.67) 1.0 1.5k p, d
G189.03+0.76 26.8(1.8) 05.98(01.77) 0.3 0.7k p
G189.78+0.34 28.5(2.0) 14.23(04.26) 1.2 < 6g d
G192.60-0.05 53.0(3.7) 05.09(01.53) 1.0 22.3k d
G196.45-1.68(1) 24.2(1.6) 03.75(01.11) 1.1 715g d
G196.45(2) 23.4(1.6) 04.00(01.20) 1.1 < 6g none
G203.05-14.5 37.4(2.6) 18.34(05.49) 0.2 < 6g d
G213.70-12.6 28.1(1.9) 06.34(01.89) 1.0 180w d
G232.62+0.99 20.5(1.4) 01.98(00.57) 1.0 1w p, d

Notes. Col. (1) source names, which are also its Galactic coordinates. If one region has multiple cores, they are given suffix numbers “(1), (2), (3)...”.Col. (2) excitation tempearture of the 12CO (1 − 0) at the emission peak of the core.Col. (3) H2 column density at the emission peak of the core.Col. (4) effective radius of the core, which is calculated from using where Acore is the area encircled by the 50% contour in the 13CO (1 − 0) map (in unit of pc2). Col. (5) flux of the radio continuum emission associated with the core. The values are extracted from several works, including the 6 cm (m) MAGPIS survey (Helfand et al. 2006), and the observations of (g) Gregory & Condon (1991), (r) Rodriguez et al. (1981), (k) Kurtz et al. (1994), and (w) Walsh et al. (1998). The observational wavelength is λ = 6.1 cm for Gregory & Condon (1991) and Rodriguez et al. (1981), λ = 3.5 cm for Kurtz et al. (1994), and λ = 3.5 cm for Walsh et al. (1998). The detection limit is σ ≃ 2.3 mJy for MAGPIS and σ ≃ 6 mJy for Gregory & Condon (1991). Col. (6) infrared emission feature associated with the 13CO cores as shown in Fig. A.1. For the cores associated with the IR emission, the emission features are classified as “point-like” (p) and “diffused” (d).

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