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Table 2.

Parameters derived from best-fit of the image decomposition.

Species Model Centerx Centery nISM rs_x rs_y θ re_x re_y νSν_point νSν_ext Sν_point Sν_ext fpoint_all
(hh:mm:ss) (dd:mm:ss) (″) (″) (°) (kpc) (kpc) (Jy km s−1) (Jy km s−1) (mJy) (mJy) (%)
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12) (13) (14) (15)
[C II] S 23:10:38.8994 ± 0.0001s 18:55:19.7925 ±
CO (9–8) S 23:10:38.9016 ± 0.0001s 18:55:19.7781 ±
CO (9–8) P+S 23:10:38.9016 ± 0.0001s 18:55:19.7787 ±
[C II]con S 23:10:38.9003 ± 0.0001s 18:55:19.8033 ±
[C II]con P+S 23:10:38.9003 ± 0.0001s 18:55:19.8032 ±
CO (9–8) con S 23:10:38.9013 ± 0.0001s 18:55:19.7740 ±
CO (9–8) con P+S 23:10:38.9013 ± 0.0001s 18:55:19.7741 ±

Notes. Column 1: the name of the ISM tracer. Column 2: the best-fit model. “S” and “P” present the Sérsic and point component, respectively. Columns 3–4: source position – RA and Dec, respectively. Column 5: the Sérsic index of the ISM (the gas and the dust emission). Columns 6–7: the scale lengths along the major and minor axes, respectively. Column 8: the rotation angle defined in Appendix B. Columns 9–10: the half-light radii. The values in boldface are measurements near the kinematic major axes. Columns 11–12: the line flux for the point component and extended component, respectively. Columns 13–14: the dust continuum flux density for the point component and extended component, respectively. Column 15: the fraction of the nuclear component in the whole emission. Note that the errors of these parameters are all fitting-type errors. The complex correlated noise is not included. As claimed by the task reference of the CASA IMFIT, the correlated noise can bring 4% effect when 5σ detection of the emission for a 2D elliptical Gaussian fitting.

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