Table 1.
HI properties of CGCG 137-068.
| Beam | zHI | W50 | W10 | Fint | log(L′HI) | log(MHI) |
|---|---|---|---|---|---|---|
| (″) | (km s−1) | (km s−1) | (Jy km s−1) | (K km s−1 pc2) | (M⊙) | |
| (1) | (2) | (3) | (4) | (5) | (6) | (7) |
| 28 | 0.013972 ± 0.000014 | 50 ± 30 | 127 ± 9 | 0.94 ± 0.09 | 10.738 ± 0.038 | 8.909 ± 0.038 |
| 19 | 0.013976 ± 0.000014 | 48 ± 22 | 127 ± 18 | 1.02 ± 0.12 | 10.772 ± 0.048 | 8.944 ± 0.048 |
| 13 | 0.013983 ± 0.000017 | 47 ± 22 | 126 ± 26 | 1.17 ± 0.15 | 10.832 ± 0.051 | 9.004 ± 0.051 |
| 5 | 0.013988 ± 0.000022 | 33 ± 14 | 126 ± 34 | 1.49 ± 0.23 | 10.939 ± 0.063 | 9.111 ± 0.063 |
Notes. (1) Beam size of the HI cube (the global estimates are the most reliable for the coarsest resolution). (2) Redshift determined from the emission-weighted frequency of the HI line. (3) HI line width at the 50% of the maximum. (4) Width at the 10% of the maximum. (5) Integrated flux within the dotted lines in Fig. 1. (6) HI line luminosity using Eq. (3) in Solomon et al. (1997). (7) Neutral hydrogen mass using Eq. (2) in Devereux & Young (1990).
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