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Table B.3.

Comparison between experimental and theoretical values, using the anharmonic approximation at MP2/cc-pVTZ level of theory, for the vibrationally excited states of HC5N and HC7N.

Vib. State Theo. Bν (a) Exp. Bν (b) Bν (c) Theo. (d) Exp. (e) (c)
HC5N

ν6 1330.229 1330.27109(88) (f) 0.003%
ν7 1331.651 1331.600997(28) (f) –0.004% 0.2017 0.213887(55) (f) –5.7%
ν8 1333.224 1333.051138(27) (f) –0.013% 0.2986 0.316154(59) (f) –5.6%
ν9 1332.841 1332.925330(20) (g) 0.006% 0.3094 0.328526(40) (g) –5.8%
ν10 1333.634 1333.784785(26) (g) 0.011% 0.4651 0.500190(52) (g) –7.0%
ν11 1333.959 1334.118237(24) (g) 0.012% 1.0892 1.162898(48) (g) –6.3%

HC7N

ν13 564.713 564.736752(39) (h) 0.004% 0.0809 0.085553(77) (h) –5.5%
ν14 564.705 564.743284(47) (h) 0.007% 0.1350 0.143602(94) (h) –6.0%
ν15 564.845 564.887305(34) (h) 0.007% 0.3392 0.359762(69) (h) –5.7%

Notes. (a)Rotational constant B of the vibrational state ν estimated using the theoretical vibration–rotation coupling constants αi calculated at the MP2/cc-pVTZ level of theory. (b)Experimental values of the B rotational constant. (c)Discrepancies between theoretical calculations and experimental values calculated as follows: ((Exp  −  Theo) / Exp)  ×  100. (d)l-doubling constant of the vibrational mode ν calculated at the MP2/cc-pVTZ level of theory. (e)Experimental value of the l-doubling constant qνt. (f)Experimental values are taken from Degli Esposti et al. (2005). (g)Experimental value are taken from Yamada et al. (2004). (h)Experimental values are taken from Bizzocchi & Degli (2004).

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