Table 2.
Spectroscopic parameters of H2CCCH+ (in MHz) obtained by fitting Watson’s S-reduced Hamiltonian to the rotational transitions from Table 1.
Exp. | Calculated |
|||
---|---|---|---|---|
Parameter | This study | Huang et al. (2011) | This study (a) | This study, BE (b) |
A0 | 281 856.(247) | 281 911.9 | 283 318.43 | 282 182.6 |
B0 | 9675.841(1) | 9580.2 | 9670.18 | 9675.97 |
C0 | 9342.877(1) | 9251.9 | 9337.82 | 9343.14 |
DJ × 103 | 2.942(4) | 3. | 2.68 | 3.06 |
DJK | 0.4388(9) | 0.479 | 0.479 | 0.433 |
DK | 20.678 (c) | 20.862 | 20.678 | 20.678 |
d1 × 103 | −0.121(3) | 0. | −0.097 | −0.103 |
d2 × 103 | −0.051 (c) | 0. | −0.037 | −0.051 |
μA / Debye | ⋯ | 0.524 d) | 0.55 | ⋯ |
Notes. Western’s PGOPHER program (Western 2017) was used for the fit. The experimental uncertainties are given in parentheses.
From equilibrium structure and force field calculated at the ae-CCSD(T)/cc-pwCVQZ and fc-CCSD(T)/ANO1 levels, respectively.
Best estimate (BE) values, obtained through scaling of calculated values via isoelectronic propadienylidene, H2CCC (see text for details).
From Huang & Lee (2011).
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