Unveiling the substructure of the massive clump AGAL G035.1330−00.7450

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Table 5

Gaussian fitting parameters (see Fig. 6) for the K projections of the CH₃CN J = 13–12 transition toward cores C1 and C2.

Proj.	Peak Int.	Δv	W
K	(Jy beam⁻¹)	(km s⁻¹)	(Jy beam⁻¹ km s⁻¹)
		Core C1 (blue)

0	−	−	−
1	0.26	3.89	1.29
2	0.23	3.53	1.16
3	0.25	3.85	1.21
4	0.16	3.34	0.73

		Core C1 (red)

0	0.26	4.11	1.24
1	−	−	−
2	0.22	4.29	1.07
3	0.24	4.19	1.17
4	0.14	3.91	0.60

		Core C2

0	0.13	6.1	0.96
1	0.12	4.0	0.83
2	0.11	4.9	0.61
3	0.12	5.4	0.70
4	0.06	4.6	0.28

Notes. Core C1 is separated into blue and red components. The blue component of the K = 0 projection and the red component of the K = 1 projection for the core C1 are not fit.

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