Esselman Brian J, Zdanovskaia Maria A, Owen Andrew N, Stanton John F, Woods R Claude, McMahon Robert J
Department of Chemistry, University of Wisconsin-Madison, 1101 University Avenue, Madison, Wisconsin 53706-1322, USA.
Quantum Theory Project, Departments of Physics and Chemistry, University of Florida, Gainesville, Florida 32611, USA.
J Chem Phys. 2021 Aug 7;155(5):054302. doi: 10.1063/5.0057221.
The pure rotational spectrum of thiazole (c-CHNS, C) has been studied in the millimeter-wave region from 130 to 375 GHz. Nearly 4800 newly measured rotational transitions for the ground vibrational state of the main isotopologue were combined with previously reported measurements and least-squares fit to a complete sextic Hamiltonian. Transitions for six singly substituted heavy-atom isotopologues (C, N, S, S) were observed at natural abundance and likewise fit. Several deuterium-enriched samples were prepared, which gave access to the rotational spectra of 16 additional isotopologues, 14 of which had not been previously studied. The rotational spectra of each isotopologue were fit to A- and S-reduced distorted-rotor Hamiltonians in the I representation. The experimental values of the ground-state rotational constants (A, B, and C) from each isotopologue were converted to determinable constants (A″, B″, and C″), which were corrected for effects of vibration-rotation interactions and electron-mass distributions using coupled-cluster singles, doubles, and perturbative triples calculations [CCSD(T)/cc-pCVTZ]. The moments of inertia from the resulting constants (A, B, and C) of 24 isotopologues were used to determine the precise semi-experimental equilibrium structure (r ) of thiazole. As a basis for comparison, a purely theoretical equilibrium structure was estimated by an electronic structure calculation [CCSD(T)/cc-pCV5Z] that was subsequently corrected for extrapolation to the complete basis set, electron correlation beyond CCSD(T), relativistic effects, and the diagonal Born-Oppenheimer correction. The precise r structure is compared to the resulting "best theoretical estimate" structure. Some, but not all, of the best theoretical r structural parameters fall within the narrow statistical limits (2σ) of the r results. The possible origin of the discrepancies between the best theoretical estimate r and semi-empirical r structures is discussed.
已在130至375吉赫兹的毫米波区域研究了噻唑(c-CHNS,C)的纯转动光谱。近4800个新测量的主要同位素分子基振动态的转动跃迁与先前报道的测量结果相结合,并通过最小二乘法拟合到一个完整的六次哈密顿量。在天然丰度下观测到了六种单取代重原子同位素分子(C、N、S、S)的跃迁,并同样进行了拟合。制备了几个氘富集样品,从而获得了另外16种同位素分子的转动光谱,其中14种此前未被研究过。每种同位素分子的转动光谱都在I表象下拟合到A-和S-简化畸变转子哈密顿量。将每种同位素分子基态转动常数(A、B和C)的实验值转换为可确定常数(A″、B″和C″),使用耦合簇单双激发和微扰三激发计算[CCSD(T)/cc-pCVTZ]对其进行振动-转动相互作用和电子质量分布效应的校正。利用24种同位素分子所得常数(A、B和C)的转动惯量来确定噻唑精确的半实验平衡结构(r )。作为比较基础,通过电子结构计算[CCSD(T)/cc-pCV5Z]估计了一个纯理论平衡结构,随后对其进行了外推到完整基组、CCSD(T)之外的电子关联、相对论效应以及对角波恩-奥本海默校正的校正。将精确的r 结构与所得的“最佳理论估计”结构进行比较。最佳理论r 结构参数中的一些(但不是全部)落在r 结果的狭窄统计极限(2σ)内。讨论了最佳理论估计r 与半经验r 结构之间差异的可能来源。