Table 1.
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Line parameters for C2D observations done by Yoshida et al. (2019).

FrequencyTransition∫Tmbdv
(GHz)|$(n_{1},j_{1},F) \rightarrow (n_{1}^{\prime },j_{1}^{\prime },F^{\prime })$|(K km s−1)
72.101715(1,1.5,1.5) → (0,0.5,1.5)0.147(16)a
72.107700(1,1.5,2.5) → (0,0.5,1.5)0.395(16)
72.109114(1,1.5,0.5) → (0,0.5,0.5)0.117(14)
72.112399(1,1.5,1.5) → (0,0.5,0.5)0.144(15)
72.187704(1,0.5,1.5) → (0,0.5,1.5)0.165(20)
72.189505(1,0.5,0.5) → (0,0.5,1.5)0.12(3)
72.198388(1,0.5,1.5) → (0,0.5,0.5)0.065(16)
FrequencyTransition∫Tmbdv
(GHz)|$(n_{1},j_{1},F) \rightarrow (n_{1}^{\prime },j_{1}^{\prime },F^{\prime })$|(K km s−1)
72.101715(1,1.5,1.5) → (0,0.5,1.5)0.147(16)a
72.107700(1,1.5,2.5) → (0,0.5,1.5)0.395(16)
72.109114(1,1.5,0.5) → (0,0.5,0.5)0.117(14)
72.112399(1,1.5,1.5) → (0,0.5,0.5)0.144(15)
72.187704(1,0.5,1.5) → (0,0.5,1.5)0.165(20)
72.189505(1,0.5,0.5) → (0,0.5,1.5)0.12(3)
72.198388(1,0.5,1.5) → (0,0.5,0.5)0.065(16)

Note. aParenthesis represent the errors of last significant digits.

Table 1.
Open in new tab

Line parameters for C2D observations done by Yoshida et al. (2019).

FrequencyTransition∫Tmbdv
(GHz)|$(n_{1},j_{1},F) \rightarrow (n_{1}^{\prime },j_{1}^{\prime },F^{\prime })$|(K km s−1)
72.101715(1,1.5,1.5) → (0,0.5,1.5)0.147(16)a
72.107700(1,1.5,2.5) → (0,0.5,1.5)0.395(16)
72.109114(1,1.5,0.5) → (0,0.5,0.5)0.117(14)
72.112399(1,1.5,1.5) → (0,0.5,0.5)0.144(15)
72.187704(1,0.5,1.5) → (0,0.5,1.5)0.165(20)
72.189505(1,0.5,0.5) → (0,0.5,1.5)0.12(3)
72.198388(1,0.5,1.5) → (0,0.5,0.5)0.065(16)
FrequencyTransition∫Tmbdv
(GHz)|$(n_{1},j_{1},F) \rightarrow (n_{1}^{\prime },j_{1}^{\prime },F^{\prime })$|(K km s−1)
72.101715(1,1.5,1.5) → (0,0.5,1.5)0.147(16)a
72.107700(1,1.5,2.5) → (0,0.5,1.5)0.395(16)
72.109114(1,1.5,0.5) → (0,0.5,0.5)0.117(14)
72.112399(1,1.5,1.5) → (0,0.5,0.5)0.144(15)
72.187704(1,0.5,1.5) → (0,0.5,1.5)0.165(20)
72.189505(1,0.5,0.5) → (0,0.5,1.5)0.12(3)
72.198388(1,0.5,1.5) → (0,0.5,0.5)0.065(16)

Note. aParenthesis represent the errors of last significant digits.

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