Table 7
Spectroscopic constants of C2H5C≡C–C≡N.
Parameter | Experimental | Theory |
|
||
A (MHz) | 21750(21) | 21878.28 |
B(MHz) | 1344.8187(30) | 1338.41 |
C(MHz) | 1285.4798(29) | 1281.19 |
Δ(amu Å2) | –5.889(23) | –6.22 |
DJ(kHz) | 0.16287(68) | 0.14348 |
DJK(kHz) | –13.6967(90) | –12.6100 |
HJ(Hz) | 0.00029(20) | 0.00015 |
HJK(Hz) | –0.0086(32) | –0.1359 |
HKJ(Hz) | –0.528(39) | 14.30 |
rms | 1.1597 | |
N | 342 |
Notes.The spectroscopic constants are in the S-reduction form. The uncertainties represent one standard deviation. rms is the root-mean-square deviation defined by rms2 = Σ [(νobs − νcalc)/u] 2/(N − P), where νobs and νcalc are the observed and calculated frequencies, u is the uncertainty of the observed frequency, N is the number of transitions used in the least-squares fit, and P is the number spectroscopic constants used in the fit. The theoretical rotational constants were obtained in the CCSD/cc-pVTZ calculations and the centrifugal distortion constants were obtained in the B3LYP/cc-pVTZ calculations. Δ is defined by Δ = Ic − Ia − Ib.
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