Table C.1.
Energies, rotational constants, quadrupole coupling constants, dipole moment, and vibrational partition functions of the HC5N isomers evaluated at MP2/cc-pVTZ level of theory.
ΔE(a) | ΔEMP2(b) | A0(c) | B0(c) | C0(c) | 1.5χaa | 0.25(χbb − χcc) | μT | Qv(d) | Qv(d) | |
---|---|---|---|---|---|---|---|---|---|---|
(kJ mol−1) | (kJ mol−1) | (MHz) | (MHz) | (MHz) | (MHz) | (MHz) | (D) | 50 K | 300 K | |
HC5N (e) | 0.0 | 0.0 | 1320.046 | −5.77 | 4.36 | 1.09 | 22.89 | |||
HC4NC (f) | 134.7 | 133.8 | 1390.737 | 1.15 | 3.57 | 1.07 | 22.62 | |||
C3CHCN | 256.1 | 254.5 | 21076.776 | 1689.938 | 1564.496 | −2.73 | −0.41 | 3.09 | 1.10 | 14.18 |
C5NH | 269.2 | 267.7 | 1348.267 | 2.10 | 0.31 | 9.14 | 1.02 | 8.86 | ||
HC2NC3 | 294.1 | 292.2 | 1434.147 | 2.96 | 6.58 | 1.01 | 8.06 | |||
HC2C(C)CN | 289.3 | 284.2 | 10693.657 | 2526.651 | 2038.799 | −4.72 | −0.20 | 3.27 | 1.06 | 15.93 |
HC3NC2 | 320.8 | 316.2 | 1435.856 | 0.91 | 7.15 | 1.03 | 15.46 | |||
C2CHC2N | 365.5 | 361.3 | 11195.360 | 2552.013 | 2073.245 | −5.24 | −0.14 | 4.48 | 1.15 | 15.16 |
Notes.
Rotational constants at the ground state evaluated using the vibration-rotation interaction constants obtained using the anharmonic corrections. In the case of the quasi linear C5NH, the effective rotational constant, Beff, is provided.
Vibrational partition function calculated using the expression ∏i(1 − e−(hωi/KT))−di (Gordy & Cook 1984), where ωi and di represent the energy and the degeneracy of each i vibrational mode. The energies for the vibrational modes are taken from the results of ab initio calculations evaluated at MP2/cc-pVTZ level of theory, under the anharmonic correction. At the temperature of TMC1 (10 K), the vibrational partition function for isomers is equal to one.
The experimental value is B0 = 1331.33269 ± 0.00002 (Bizzocchi et al. 2004). The ratio B0(exp)/B0(Cal) is 1.0086.
The experimental value is B0 = 1401.18216 ± 0.00006 (this work, see Table A.3. The ratio B0(exp)/B0(Cal) is 1.0075.
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