Table B.1.
Theoretical values for the vibrational excited states of HC9N calculated at B3LYP/cc-pVTZ and MP2/cc-pVTZ levels of theory under the anharmonic approach.
αi (MHz) | Bν (MHz) (a) |
![]() |
Frequency (cm−1) | ||||||
---|---|---|---|---|---|---|---|---|---|
Vib. State | Sim. | B3LYP | MP2 | B3LYP | B3LYP | B3LYP | MP2 | B3LYP | MP2 |
ν1 | σ | 0.07761 | 0.07485 | 290.44071 | 290.44347 | – | – | 3336 | 3348 |
ν2 | σ | 0.40988 | 0.52794 | 290.10844 | 289.99038 | – | – | 2296 | 2142 |
ν3 | σ | 0.48562 | 0.47154 | 290.03270 | 290.04678 | – | – | 2253 | 2090 |
ν4 | σ | 0.62642 | 0.60274 | 289.89190 | 289.91558 | – | – | 2182 | 2023 |
ν5 | σ | 0.34994 | 0.33200 | 290.16838 | 290.18632 | – | – | 2173 | 2028 |
ν6 | σ | 0.29256 | 0.33625 | 290.22576 | 290.18207 | – | – | 2088 | 1956 |
ν7 | σ | 0.50556 | 0.47858 | 290.01276 | 290.03974 | – | – | 1406 | 1383 |
ν8 | σ | 0.31723 | 0.30450 | 290.20109 | 290.21382 | – | – | 1128 | 1098 |
ν9 | σ | 0.19501 | 0.18891 | 290.32331 | 290.32941 | – | – | 737 | 744 |
ν10 | σ | 0.08457 | 0.08156 | 290.43375 | 290.43676 | – | – | 377 | 365 |
ν11 | π | –0.03612 | –0.03210 | 290.55444 | 290.55042 | 0.0101 | 0.0103 | 653 | 601 |
ν12 | π | –0.22177 | –0.25210 | 290.74009 | 290.77042 | 0.0128 | 0.0134 | 545 | 459 |
ν13 | π | –0.18431 | –0.20526 | 290.70263 | 290.72358 | 0.0138 | 0.0139 | 535 | 491 |
ν14 | π | –0.19463 | –0.19918 | 290.71295 | 290.71750 | 0.0143 | 0.0145 | 510 | 477 |
ν15 | π | –0.21125 | –0.22289 | 290.72957 | 290.74121 | 0.0161 | 0.0160 | 450 | 430 |
ν16 | π | –0.27911 | –0.28303 | 290.79743 | 290.80135 | 0.0205 | 0.0208 | 309 | 285 |
ν17 | π | –0.27102 | –0.26584 | 290.78934 | 290.78416 | 0.0300 | 0.0298 | 208 | 198 |
ν18 | π | –0.29291 | –0.28753 | 290.81123 | 290.80585 | 0.0537 | 0.0530 | 122 | 110 |
ν19 | π | –0.35317 | –0.34513 | 290.87149 | 290.86345 | 0.1408 | 0.1378 | 55 | 47 |
Exp. (ν19) (b) | 290.884436 (345) | 0.146310(133) | 50 (d) | ||||||
Error (c) | 0.004% | 0.007% | 3.8% | 5.8% | 10.0% | 6.0% |
Notes. (a)Rotational constant B of the vibrational state ν calculated using the experimental value of the ground state from Iida et al. (1991). (b)Experimental values obtained form a fit to the frequencies observed in this work (see Table A.2). (c)Discrepancies between theoretical calculations and experimental values for the vibrational excited state ν19. Values calculated as follows: ((Exp − Theo) / Exp) × 100. (d)Calculated using the approximation , where ων is the frequency of the vibrational state ν and Bν and qνt are its rotational and l-doubling constants, respectively.
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