posted on 2023-09-29, 21:14authored byBrian
J. Esselman, Maria A. Zdanovskaia, Andrew N. Owen, John F. Stanton, R. Claude Woods, Robert J. McMahon
Recent advances in gas-phase structure determination
afford outstanding
agreement between the CCSD(T)/cc-pCVTZ-corrected semi-experimental
(<i>r<sub>e</sub></i><sup>SE</sup>) equilibrium structures
and their corresponding best theoretical estimates (BTEs) of the equilibrium
structures (<i>r<sub>e</sub></i>) based upon corrections
to the CCSD(T)/cc-pCV5Z geometries for the aromatic heterocycles pyrimidine
and pyridazine. Herein, that same analysis is extended to the fundamental
aromatic molecule benzene, using published experimental spectroscopic
data for a total of 11 available isotopologues. The incorporation
of rotational constants from all of these isotopologues and CCSD(T)
corrections to address the impacts of both the vibration-rotation
interaction and electron-mass distribution results in a highly precise
and accurate <i>r<sub>e</sub></i><sup>SE</sup> structure.
The CCSD(T)/cc-pCV5Z optimized geometry has been further corrected
to address a finite basis set, untreated electron correlation, relativistic
effects, and a breakdown of the Born–Oppenheimer approximation.
This analysis achieves outstanding agreement between the <i>r<sub>e</sub></i> (BTE) and <i>r<sub>e</sub></i><sup>SE</sup> structural parameters of benzene to a highly satisfying level (0.0001
Å), an agreement that surpasses our recently published structures
of the aforementioned nitrogen-substituted benzene analogues. The <i>D</i><sub>6<i>h</i></sub> geometry of benzene is now
known to an unprecedented precision: <i>R</i><sub>C–C</sub> = 1.3913 (1) Å and <i>R</i><sub>C–H</sub> =
1.0809 (1) Å. The mutual agreement between theory and experiment
presented in this work validates both, substantially resolving all
discrepancies between the <i>r<sub>e</sub></i><sup>SE</sup> and theoretical <i>r<sub>e</sub></i> structures available
in the literature.