Table 1. Rotational Parameters for the 2-Naphthalenethiol Dimer and Computational Predictions.
Experiment |
Theory |
|||||||
---|---|---|---|---|---|---|---|---|
Isomer 1 | Isomer 2 | CC-1 | CC-2 | CT-1 | CT-2 | TT-1 | CT-3 | |
A/MHza | 308.38853(21)e | 299.45856(51) | 318.10 | 304.23 | 294.60 | 307.2 | 300.3 | 390.1 |
B/MHz | 231.75029(16) | 246.9652(12) | 233.40 | 250.65 | 245.68 | 249.6 | 242.1 | 228.2 |
C/MHz | 226.78483(18) | 221.5793(15) | 231.34 | 225.72 | 240.89 | 225.6 | 239.4 | 175.3 |
DJ/kHz | 0.01761(44) | 0.1328(56) | 0.016 | 0.012 | 0.024 | 0.012 | 0.022 | 0.010 |
DJK/kHz | [0.0]f | –0.242(14) | –0.003 | 0.028 | –0.037 | 0.032 | –0.024 | 0.005 |
DK/kHz | 0.0234(12) | 0.164(10) | 0.023 | 0.005 | 0.055 | 0.001 | 0.044 | 0.065 |
d1/kHz | [0.0] | 0.0434(28) | –0.002 | 0.000 | –0.007 | 0.000 | –0.009 | –0.001 |
d2/kHz | [0.0] | [0.0] | 0.001 | –0.001 | 0.002 | –0.001 | 0.001 | –0.001 |
|μa|/D | - | - | 0.0 | 0.2 | 1.0 | –0.7 | 0.0 | –1.1 |
|μb|/D | - | ++ | 0.0 | 0.6 | 1.1 | 1.3 | 0.0 | 1.2 |
|μc|/D | +++g | ++ | 1.3 | 0.6 | 0.6 | 1.2 | –2.1 | 0.0 |
Nb | 173 | 86 | ||||||
σ/kHz | 10.6 | 10.6 | ||||||
ΔEZPE/kJ mol–1c | 0.0 | 0.2 | 0.5 | 0.7 | 0.9 | 1.1 | ||
ΔG/kJ mol–1 | 1.4 | 1.8 | 0.0 | 0.2 | –1.1 | 1.3 | ||
EC/kJ mol–1 | –48.7 | –47.4 | –47.2 | –47.2 | –46.9 | –46.9 | ||
ΔESCS-MP2/kJ mol–1d | 1.1 | 0.0 | 0.4 | 0.4 | 1.1 | 1.3 | ||
ΔEDLPNO-CCSD(T)/kJ mol–1 | 0.7 | 0.0 | 0.6 | 0.8 | 1.1 | 2.4 |
Rotational constants (A, B, C), centrifugal distortion constants (DJ, DJK, DK, d1, d2) according to Watson’s S-reduction (Ir-representation) and electric dipole moments (μα, α = a, b, c).
Number of measured transitions (N) and standard deviation of the fit (σ).
Relative energy with zero-point corrections (ΔE), Gibbs energy (ΔG, 298 K, 1 atm), and complexation energy (ΔEC including BSSE corrections) using B3LYP-D3(BJ)/def2-TZVP.
Electronic energy using SCS-MP2 and DLPNO-CCSD(T), uncorrected for zero-point vibrational energy.
Standard errors in parentheses in units of the last digit.
Parameters in square brackets fixed to zero.
The plus signs denote qualitatively the observation of the corresponding rotational transitions.