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Table 2.

Observed lines of deuterated species and related species.

Line Rest freq. Redshifted freq. (△) μ(‡) α(⋆)
(GHz) (GHz) (D) (cm−2 km−1 s)
Observed on 2019 April 11

HDO (JKa,Kc = 10, 1–00, 0) 464.924520 246.537 1.73 1.9 × 1013
o-NH2D (JKa,Kc = 11, 0–00, 0, F = 2–1) 470.271911 (†) 249.373 1.46 5.6 × 1013(♢), (°)
p-NH2 (NKa,Kc = 11, 0–10, 1, J = 1/2–1/2, F = 3/2–3/2) 469.440621 (†) 248.932 (†) 1.82 1.8 × 1014(♢), (°)
p-NH2 (NKa,Kc = 11, 0–10, 1, J = 1/2–3/2, F = 3/2–5/2) 470.409052 (†) 249.445 (†) 1.82 1.8 × 1014(♢), (°)
7LiH (J = 1–0) 443.952930 235.416 5.88 2.5 × 1011

Observed on 2019 July 28

ND (N = 1–0, J = 2–1) 522.077372 (†) 276.844 (†) 1.39 7.7 × 1013(♢)
ND (N = 1–0, J = 1–1) 546.127619 (†) 289.597 (†) 1.39 7.7 × 1013(♢)
(JKa,Kc = 11, 0–10, 1) 547.676440 290.418 1.85 6.3 × 1012(°)

Notes. (△)For a redshift z = 0.88582, in heliocentric frame; (‡)electric dipole moment; (⋆)coefficients to convert line integrated opacity into column density Ncol = ατdv, calculated in the case of pure radiative coupling with CMB photons, i.e., taking Tex = TCMB = 5.14 K; (†)frequency of the strongest hyperfine transition; (♢)for a hyperfine component with equivalent line strength Sul = 1; (°)the coefficient converts directly to the total (ortho+para) column density, assuming the OPR = 3. Spectroscopy parameters are taken from the Cologne Database for Molecular Spectroscopy (Müller et al. 2001, 2005; Endres et al. 2016) and the Jet Propulsion Laboratory Molecular Spectroscopy catalog (Pickett et al. 1998) and references therein.

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