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Table 2

Molecular parameters in cm−1 of CH3CSNH2 obtained with the RAM36 program.

ntr (a) Parameter (b) Operator (c) Value (d) Value (this study)
220 F 5.650542416 (e) 5.45339(10)(f)
220 V3 108.860(66) 110.71340(94)
211 ρ Jzpα 0.042368(54) 0.0437894(17)
202 ARAM 0.270791(38) 0.2696379(20)
202 BRAM 0.2207334(66) 0.22085611(92)
202 CRAM 0.11213403(48) 0.112127546(92)
202 Dzx {Jz, Jx} −0.0749884(24) −0.07505330(80)
440 V6 −14.66262(38)
422 FJ − 0.456(12) × 10−6
422 FK − 0.484(13) × 10−5
422 Fzx − 0.507(93) × 10−6
422 V3J J2(1 − cos3α) 0.2781(80) × 10−3 0.14296(43) × 10−3
422 V3K 0.149(12) × 10−2 − 0.14891(40) × 10−2
422 V3zx 0.1820(14) × 10−2 0.20727(28) × 10−2
422 V3xy 0.2311(85) × 10−3 0.9789(38) × 10−4
422 D3zy 0.9823(63) × 10−3
422 D3xy 0.450(32) × 10−4
413 ρJ J2Jzpα − 0.229(15) × 10−5 − 0.3828(59) × 10−6
413 ρK 0.1761(49) × 10−4 0.2695(19) × 10−5
413 ρzx − 0.982(24) × 10−6
404 DzxJ − 0.433(44) × 10−7
404 DzxK 0.6597(45) × 10−6
404 ΔJ J4 0.1137(12) × 10−6
404 ΔJK − 0.3446(24) × 10−6
404 ΔK 0.6353(49) × 10−6
404 δJ 0.1024(12) × 10−6
404 δK 0.6668(99) × 10−7
642 V6J J2 (1 − cos 6α) 0.1254(10) × 10−4
642 V6K − 0.1634(44) × 10−3
642 V6zx − 0.752(33) × 10−4
633 ρ3xy 0.427(12) × 10−5
624 V3JJ J4 (1 − cos 3α) − 0.632(57) × 10−10
624 V3JK − 0.506(34) × 10−8
624 FFJK − 0.1344(47) × 10−8
624 FKK 0.1582(46) × 10−8
624 D3xyK − 0.967(40) × 10−7
615 ρJK 0.382(32) × 10−10
606 ΦJK 0.1475(33) × 10−11
606 ΦKJ − 0.337(17) × 10−11
606 ϕJK 0.820(27) × 10−12

Number of parameters 17 40
Number of lines vt = 0, vt = 1 286, 0 1428, 321
Fmax in GHz 110 650
Jmax, Ka,max 15, 10 95, 20
rms in kHz 107 43.4
wrms unitless 0.71 0.90

Notes. (a)n = t + r, where n is the total order of the operator, t is the order of the torsional part and r is the order of the rotational part, respectively. (b)Parameter nomenclature based on the subscript procedures of Xu et al. (2008). (c){A, B, C} = ABC + CBA, {A, B} = AB + BA. The product of the operator in the third column of a given row and the parameter in the second column of that row gives the term actually used in the torsion-rotation Hamiltonian of the program, except for F, ρ and ARAM, which occur in the Hamiltonianin the form . (d)The parameters obtain with a refit of the data from Maris et al. (2019). (e)Fixed to the value from XIAM fit (see Table 1) in Maris et al. (2019). (f)All values are incm−1 (except ρ which is unitless). Statistical uncertainties are shown as one standard uncertainty in the units of the last two digits.

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