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Table A.3

Results of the Gaussian fit obtained from the averaged CN(1-0) emission for each clump.

Source Transition Hyperfine CN(1-0)
component V LSR FWHM
(km s-1) (km s-1) (K)
G22.35+0.41 – – – – –
G23.60+0.00A – – – – –
G23.60+0.00B – – – – –
G34.43+0.24A J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 58.82(0.26) 3.94(0.55) 0.10(0.03)
F = 3/2−1/2 66.41(0.35) 4.46(0.99) 0.08(0.03)
J = 1/2−1/2 F = 3/2−3/2 849.9(0.44) 4.64(0.97) 0.06(0.03)
F = 3/2−1/2 905.2(0.24) 3.48(0.56) 0.09(0.03)
F = 1/2−3/2 – – –
G34.43+0.24B J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 57.90(0.30) 5.87(0.76) 0.13(0.03)
F = 3/2−1/2 65.81(0.26) 5.22(1.03) 0.13(0.03)
J = 1/2−1/2 F = 3/2−3/2 849.3(0.17) 3.62(0.36) 0.12(0.03)
F = 3/2−1/2 904.1(0.19) 5.12(0.42) 0.12(0.03)
F = 1/2−3/2 973.5(0.21) 3.48(0.44) 0.09(0.03)
I18151−1208A J = 3/2−1/2 F = 3/2−3/2 −16.01(0.27) 4.95(0.67) 0.10(0.03)
F = 1/2−1/2 8.001(0.29) 4.81(0.71) 0.09(0.03)
F = 5/2−3/2 31.29(0.06) 3.75(0.14) 0.35(0.03)
F = 3/2−1/2 38.49(0.15) 3.81(0.32) 0.15(0.03)
J = 1/2−1/2 F = 3/2−3/2 822.9(0.17) 3.84(0.38) 0.12(0.03)
F = 3/2−1/2 878.0(0.19) 3.64(0.43) 0.11(0.03)
F = 1/2−3/2 947.7(0.19) 3.56(0.41) 0.11(0.03)
I18151−1208B J = 3/2−1/2 F = 3/2−3/2 −14.25(0.16) 3.63(0.65) 0.14(0.03)
F = 1/2−1/2 10.40(0.13) 2.76(0.27) 0.15(0.03)
F = 5/2−3/2 33.06(0.04) 2.60(0.09) 0.51(0.03)
F = 3/2−1/2 40.45(0.10) 2.65(0.27) 0.20(0.03)
J = 1/2−1/2 F = 3/2−3/2 824.7(0.09) 2.63(0.24) 0.18(0.03)
F = 3/2−1/2 879.4(0.10) 2.67(0.23) 0.17(0.03)
F = 1/2−3/2 949.2(0.10) 2.47(0.22) 0.16(0.03)
I18223-1243A J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 28.34(0.07) 0.50(0.16) 0.14(0.03)
F = 5/2−3/2 44.81(0.10) 2.79(0.28) 0.20(0.03)
F = 3/2−1/2 52.45(0.22) 3.68(0.63) 0.11(0.03)
J = 1/2−1/2 F = 3/2−3/2 837.0(0.14) 2.60(0.26) 0.11(0.03)
F = 3/2−1/2 891.8(0.14) 2.15(0.35) 0.10(0.03)
F = 1/2−3/2 961.0(0.25) 2.22(0.41) 0.07(0.03)
I18223-1243B J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 45.01(0.09) 3.25(0.23) 0.27(0.03)
F = 3/2−1/2 52.56(0.17) 2.94(0.47) 0.14(0.03)
J = 1/2−1/2 F = 3/2−3/2 836.9(0.15) 2.74(0.31) 0.13(0.03)
F = 3/2−1/2 892.1(0.20) 3.63(0.65) 0.12(0.03)
F = 1/2−3/2 – – –
I18306-0835 J = 3/2−1/2 F = 3/2−1/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 77.88(0.19) 2.46(0.48) 0.13(0.04)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 – – –
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –
I18310-0825A J = 3/2−1/2 F = 3/2−1/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 85.46(0.35) 3.96(0.59) 0.07(0.03)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 – – –
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –
I18310-0825B J = 3/2−1/2 F = 3/2−3/2 37.01(0.32) 3.02(0.63) 0.18(0.08)
F = 1/2−1/2 63.16(2.06) 5.55(3.20) 0.03(0.08)
F = 5/2−3/2 84.20(0.21) 4.01(0.48) 0.30(0.08)
F = 3/2−1/2 91.69(0.22) 2.86(0.55) 0.25(0.08)
J = 1/2−1/2 F = 3/2−3/2 875.9(0.18) 1.91(0.42) 0.22(0.07)
F = 3/2−1/2 931.3(0.37) 3.84(0.81) 0.15(0.07)
F = 1/2−3/2 1000.(0.30) 3.06(0.77) 0.17(0.07)
I18337-0743 J = 3/2−1/2 F = 3/2−1/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 58.14(0.22) 2.14(0.41) 0.13(0.04)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 – – –
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –
I18530+0215 J = 3/2−1/2 F = 3/2−1/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 76.74(0.14) 3.25(0.31) 0.16(0.03)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 868.8(0.28) 2.80(0.75) 0.07(0.03)
F = 3/2−1/2 923.5(0.29) 3.93(0.66) 0.07(0.03)
F = 1/2−3/2 993.6(0.45) 3.97(1.38) 0.05(0.03)
I05358+3543 J = 3/2−1/2 F = 3/2−3/2 −64.17(0.24) 3.35(0.54) 0.09(0.03)
F = 1/2−1/2 −40.33(0.27) 3.01(0.60) 0.08(0.03)
F = 5/2−3/2 −17.05(0.09) 3.56(0.22) 0.27(0.03)
F = 3/2−1/2 −9.762(0.14) 2.63(0.35) 0.14(0.03)
J = 1/2−1/2 F = 3/2−3/2 774.8(0.21) 3.18(0.58) 0.11(0.03)
F = 3/2−1/2 829.4(0.16) 2.54(0.33) 0.12(0.03)
F = 1/2−3/2 899.1(0.19) 3.09(0.52) 0.10(0.03)
I18445-0222 J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 87.38(0.13) 3.54(0.30) 0.16(0.03)
F = 3/2−1/2 94.37(0.27) 3.08(0.76) 0.09(0.03)
J = 1/2−1/2 F = 3/2−3/2 878.4(0.18) 1.52(0.41) 0.09(0.03)
F = 3/2−1/2 933.9(0.24) 2.40(0.50) 0.07(0.03)
F = 1/2−3/2 1003.(0.17) 1.73(0.40) 0.09(0.03)
I18517+0437 J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 21.43(0.10) 0.98(0.27) 0.14(0.03)
F = 5/2−3/2 44.17(0.08) 2.80(0.19) 0.29(0.03)
F = 3/2−1/2 51.75(0.27) 3.05(0.58) 0.09(0.03)
J = 1/2−1/2 F = 3/2−3/2 835.6(0.18) 3.39(0.43) 0.13(0.03)
F = 3/2−1/2 890.4(0.15) 2.47(0.35) 0.13(0.03)
F = 1/2−3/2 960.5(0.16) 2.02(0.51) 0.11(0.03)
I20126+4104 J = 3/2−1/2 F = 3/2−3/2 −51.20(0.09) 2.77(0.28) 0.23(0.03)
F = 1/2−1/2 −26.80(0.14) 2.66(0.33) 0.15(0.03)
F = 5/2−3/2 −3.672(0.04) 2.72(0.10) 0.50(0.03)
F = 3/2−1/2 3.626(0.10) 2.62(0.26) 0.22(0.03)
J = 1/2−1/2 F = 3/2−3/2 788.0(0.08) 2.58(0.25) 0.23(0.03)
F = 3/2−1/2 842.9(0.08) 2.57(0.23) 0.22(0.03)
F = 1/2−3/2 912.3(0.10) 2.47(0.26) 0.17(0.03)
I20293+3952 J = 3/2−1/2 F = 3/2−3/2 −41.34(0.13) 2.21(0.30) 0.14(0.03)
F = 1/2−1/2 −17.25(0.23) 2.12(0.46) 0.08(0.03)
F = 5/2−3/2 6.091(0.06) 2.41(0.14) 0.33(0.03)
F = 1/2−1/2 13.74(0.21) 2.66(0.36) 0.10(0.03)
J = 1/2−1/2 F = 3/2−3/2 797.5(0.10) 2.16(0.23) 0.16(0.03)
F = 3/2−1/2 852.8(0.12) 2.42(0.25) 0.13(0.03)
F = 1/2−3/2 922.7(0.12) 1.73(0.32) 0.13(0.03)
I20343+4129 J = 3/2−1/2 F = 3/2−3/2 −35.65(0.09) 2.49(0.22) 0.18(0.03)
F = 1/2−1/2 −11.10(0.09) 1.57(0.19) 0.15(0.03)
F = 5/2−3/2 11.95(0.04) 2.42(0.09) 0.47(0.03)
F = 3/2−1/2 19.31(0.09) 2.70(0.24) 0.21(0.03)
J = 1/2−1/2 F = 3/2−3/2 803.7(0.09) 2.68(0.22) 0.19(0.03)
F = 3/2−1/2 858.4(0.10) 2.36(0.19) 0.16(0.03)
F = 1/2−3/2 928.0(0.10) 1.96(0.26) 0.15(0.03)
I22134+5834 J = 3/2−1/2 F = 3/2−1/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 −18.54(0.22) 4.06(0.65) 0.11(0.03)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 – – –
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –
I22551+6221 J = 3/2−1/2 F = 3/2−3/2 −59.97(0.22) 2.93(0.50) 0.07(0.02)
F = 1/2−1/2 – – –
F = 5/2−3/2 −12.76(0.07) 2.58(0.16) 0.23(0.02)
F = 3/2−1/2 −5.114(0.12) 1.98(0.30) 0.12(0.02)
J = 1/2−1/2 F = 3/2−3/2 778.7(0.13) 2.57(0.33) 0.11(0.02)
F = 3/2−1/2 834.2(0.20) 2.54(0.42) 0.08(0.02)
F = 1/2−3/2 903.1(0.30) 5.17(1.03) 0.07(0.02)
I22570+5912 J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 −46.40(0.11) 2.56(0.26) 0.13(0.02)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 – – –
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –
I23033+5951 J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 −52.72(0.11) 3.78(0.31) 0.12(0.02)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 – – –
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –
I23139+5939 J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 −44.00(0.10) 2.15(0.26) 0.12(0.02)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 747.7(0.25) 2.71(0.39) 0.05(0.02)
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –
I01202+6133 J = 3/2−1/2 F = 3/2−3/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 −14.20(0.10) 2.99(0.26) 0.20(0.03)
F = 3/2−1/2 −6.625(0.22) 4.04(0.56) 0.10(0.03)
J = 1/2−1/2 F = 3/2−3/2 777.4(0.18) 2.55(0.36) 0.09(0.03)
F = 3/2−1/2 832.7(0.22) 2.76(0.45) 0.08(0.03)
F = 1/2−3/2 901.6(0.23) 2.15(0.42) 0.07(0.03)
I03035+5819 J = 3/2−1/2 F = 3/2−3/2 −87.21(0.35) 4.66(1.05) 0.08(0.03)
F = 1/2−1/2 – – –
F = 5/2−3/2 −39.82(0.09) 2.90(0.22) 0.21(0.03)
F = 3/2−1/2 −32.31(0.06) 1.01(0.17) 0.20(0.03)
J = 1/2−1/2 F = 3/2−3/2 751.9(0.14) 2.69(0.62) 0.14(0.03)
F = 3/2−1/2 – – –
F = 1/2−3/2 876.7(0.13) 2.56(0.32) 0.13(0.03)
19078+0901 J = 3/2−1/2 F = 3/2−3/2 −37.98(0.23) 12.97(0.53) 0.14(0.02)
F = 1/2−1/2 −13.57(0.27) 14.19(0.74) 0.13(0.02)
F = 5/2−3/2 8.680(0.10) 14.11(0.33) 0.36(0.02)
F = 3/2−1/2 20.82(0.19) 4.38(0.39) 0.12(0.02)
J = 1/2−1/2 F = 3/2−3/2 801.2(0.25) 12.91(0.55) 0.13(0.02)
F = 3/2−1/2 856.7(0.27) 11.58(0.70) 0.12(0.02)
F = 1/2−3/2 926.3(0.29) 10.08(0.69) 0.11(0.02)
I19097+0847 J = 3/2−1/2 F = 3/2−3/2 10.30(0.19) 2.96(0.49) 0.09(0.02)
F = 1/2−1/2 35.18(0.15) 0.96(0.33) 0.08(0.02)
F = 5/2−3/2 57.85(0.08) 4.22(0.20) 0.22(0.02)
F = 3/2−1/2 65.82(0.26) 3.13(0.74) 0.07(0.02)
J = 1/2−1/2 F = 3/2−3/2 849.3(0.16) 3.14(0.35) 0.10(0.02)
F = 3/2−1/2 904.1(0.28) 4.20(0.63) 0.07(0.02)
F = 1/2−3/2 974.7(0.26) 4.24(0.74) 0.07(0.02)
I19111+1048B J = 3/2−1/2 F = 3/2−3/2 11.54(0.40) 4.26(0.75) 0.07(0.03)
F = 1/2−1/2 35.62(0.56) 6.35(1.53) 0.06(0.03)
F = 5/2−3/2 58.99(0.18) 5.31(0.43) 0.16(0.03)
F = 3/2−1/2 68.62(0.32) 2.37(0.50) 0.06(0.03)
J = 1/2−1/2 F = 3/2−3/2 849.9(0.32) 4.82(0.72) 0.09(0.03)
F = 3/2−1/2 905.9(0.40) 5.97(1.18) 0.08(0.03)
F = 1/2−3/2 974.2(0.46) 4.27(0.86) 0.06(0.03)
I19111+1048A J = 3/2−1/2 F = 3/2−3/2 11.31(0.37) 5.65(0.90) 0.08(0.03)
F = 1/2−1/2 36.00(0.55) 4.85(1.41) 0.07(0.03)
F = 5/2−3/2 58.27(0.10) 4.35(0.49) 0.23(0.03)
F = 3/2−1/2 65.61(1.05) 13.33(2.65) 0.13(0.03)
J = 1/2−1/2 F = 3/2−3/2 850.6(0.23) 4.56(0.51) 0.10(0.03)
F = 3/2−1/2 905.5(0.22) 4.87(0.58) 0.11(0.03)
F = 1/2−3/2 974.7(0.23) 3.88(0.55) 0.09(0.03)
I19442+2427 J = 3/2−1/2 F = 3/2−3/2 –24.30(0.06) 3.42(0.12) 0.28(0.02)
F = 1/2−1/2 0.037(0.09) 3.47(0.22) 0.20(0.02)
F = 5/2−3/2 22.93(0.02) 3.54(0.05) 0.82(0.02)
F = 3/2−1/2 30.47(0.06) 3.59(0.13) 0.30(0.02)
J = 1/2−1/2 F = 3/2−3/2 814.5(0.32) 3.96(0.32) 0.32(0.03)
F = 3/2−1/2 869.5(0.32) 3.27(0.32) 0.30(0.03)
F = 1/2−3/2 939.2(0.32) 3.23(0.32) 0.26(0.03)
I20081+3122 J = 3/2−1/2 F = 3/2−1/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 11.22(0.28) 3.82(0.51) 0.16(0.06)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 858.1(0.35) 4.02(0.76) 0.11(0.05)
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –
I23116+6111 J = 3/2−1/2 F = 3/2−3/2 −104.1(0.13) 4.72(0.30) 0.14(0.02)
F = 1/2−1/2 −79.64(0.18) 6.47(0.69) 0.10(0.02)
F = 5/2−3/2 −57.09(0.05) 4.72(0.15) 0.40(0.02)
F = 3/2−1/2 −49.72(0.11) 4.93(0.29) 0.20(0.02)
J = 1/2−1/2 F = 3/2−3/2 734.7(0.09) 5.33(0.28) 0.17(0.02)
F = 3/2−1/2 789.7(0.09) 3.99(0.23) 0.15(0.02)
F = 1/2−3/2 859.3(0.11) 3.78(0.25) 0.12(0.02)
I23133+6050 J = 3/2−1/2 F = 3/2−3/2 −103.2(0.22) 2.48(0.47) 0.12(0.04)
F = 1/2−1/2 −78.84(0.22) 1.70(0.42) 0.10(0.04)
F = 5/2−3/2 −56.06(0.08) 3.09(0.19) 0.38(0.04)
F = 3/2−1/2 −48.43(0.22) 3.20(0.49) 0.14(0.04)
J = 1/2−1/2 F = 3/2−3/2 735.2(0.12) 1.85(1.52) 0.16(0.04)
F = 3/2−1/2 790.5(0.17) 2.36(0.41) 0.13(0.04)
F = 1/2−3/2 – – –
I23138+5945 J = 3/2−1/2 F = 3/2−3/2 −90.23(0.35) 5.05(0.90) 0.07(0.03)
F = 1/2−1/2 −65.82(0.25) 3.23(0.57) 0.08(0.03)
F = 5/2−3/2 −43.04(0.08) 3.75(0.18) 0.27(0.03)
F = 3/2−1/2 −35.64(0.17) 4.66(0.53) 0.14(0.03)
J = 1/2−1/2 F = 3/2−3/2 748.8(0.14) 2.66(0.34) 0.12(0.03)
F = 3/2−1/2 803.8(0.17) 3.38(0.54) 0.12(0.03)
F = 1/2−3/2 873.4(0.20) 4.21(0.58) 0.11(0.03)
U49.49-0.37 J = 3/2−1/2 F = 3/2−3/2 12.82(0.38) 7.37(1.05) 0.14(0.05)
F = 1/2−1/2 37.32(0.57) 6.87(1.04) 0.09(0.05)
F = 5/2−3/2 59.73(0.13) 11.89(0.38) 0.59(0.05)
F = 3/2−1/2 71.08(0.60) 6.05(1.24) 0.14(0.05)
J = 1/2−1/2 F = 3/2−3/2 851.2(0.31) 12.57(0.77) 0.19(0.04)
F = 3/2−1/2 906.3(0.24) 12.60(0.66) 0.25(0.04)
F = 1/2−3/2 975.3(0.38) 15.53(0.86) 0.17(0.04)
C41.1-0.21 J = 3/2−1/2 F = 3/2−1/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 60.53(0.18) 3.44(0.52) 0.09(0.02)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 – – –
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –
C48.93-0.29 J = 3/2−1/2 F = 3/2−3/2 20.97(0.10) 5.05(0.24) 0.11(0.01)
F = 1/2−1/2 45.55(0.14) 4.43(0.32) 0.08(0.01)
F = 5/2−3/2 68.43(0.04) 5.24(0.11) 0.31(0.01)
F = 3/2−1/2 75.91(0.09) 4.44(0.22) 0.13(0.01)
J = 1/2−1/2 F = 3/2−3/2 859.8(0.09) 4.94(0.23) 0.13(0.01)
F = 3/2−1/2 914.7(0.10) 5.42(0.26) 0.12(0.01)
F = 1/2−3/2 984.7(0.12) 5.56(0.32) 0.10(0.01)
C49.00-0.30 J = 3/2−1/2 F = 3/2−3/2 20.46(0.14) 6.06(0.39) 0.11(0.02)
F = 1/2−1/2 45.15(0.15) 4.40(0.44) 0.09(0.02)
F = 5/2−3/2 67.63(0.10) 5.21(0.17) 0.35(0.02)
F = 3/2−1/2 74.12(0.24) 7.16(0.48) 0.19(0.02)
J = 1/2−1/2 F = 3/2−3/2 859.9(0.14) 7.65(0.32) 0.13(0.02)
F = 3/2−1/2 914.6(0.14) 7.85(0.32) 0.13(0.02)
F = 1/2−3/2 984.5(0.14) 6.49(0.36) 0.12(0.02)
C49.38-0.30 J = 3/2−1/2 F = 3/2−3/2 3.77(0.12) 4.40(0.32) 0.10(0.01)
F = 1/2−1/2 28.22(0.14) 3.40(0.30) 0.08(0.01)
F = 5/2−3/2 51.02(0.08) 4.03(0.17) 0.28(0.01)
F = 3/2−1/2 58.07(0.26) 8.19(1.08) 0.13(0.01)
J = 1/2−1/2 F = 3/2−3/2 842.9(0.11) 4.98(0.28) 0.13(0.02)
F = 3/2−1/2 897.8(0.12) 5.24(0.32) 0.12(0.02)
F = 1/2−3/2 967.6(0.15) 5.35(0.42) 0.11(0.02)
C51.36-0.00 J = 3/2−1/2 F = 3/2−3/2 7.36(0.21) 5.71(0.57) 0.08(0.02)
F = 1/2−1/2 31.55(0.38) 4.33(0.89) 0.05(0.02)
F = 5/2−3/2 54.31(0.08) 3.91(0.20) 0.18(0.02)
F = 3/2−1/2 61.75(0.16) 4.44(0.46) 0.09(0.02)
J = 1/2−1/2 F = 3/2−3/2 845.9(0.19) 3.78(0.52) 0.07(0.02)
F = 3/2−1/2 900.9(0.16) 3.74(0.45) 0.07(0.02)
F = 1/2−3/2 970.4(0.15) 2.84(0.36) 0.07(0.02)
C52.94-0.59 – – – – –
D53.64+0.24 J = 3/2−1/2 F = 3/2−1/2 – – –
F = 1/2−1/2 – – –
F = 5/2−3/2 36.68(0.29) 3.08(0.80) 0.06(0.02)
F = 3/2−1/2 – – –
J = 1/2−1/2 F = 3/2−3/2 – – –
F = 3/2−1/2 – – –
F = 1/2−3/2 – – –

Notes. The columns are (1) source name; (2) velocity of CN; (3) FWHM line width of CN; (4) intensity of CN. The − indicates that the averaged molecule emission of the clump is weak and that its signal-to-noise ratio is higher than 1, but lower than 3.

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