James Anna H, Kaledin Martina, Kaledin Alexey L
Department of Chemistry & Biochemistry, Kennesaw State University, 370 Paulding Ave NW, Box # 1203, Kennesaw, Georgia 30144, United States.
Cherry L. Emerson Center for Scientific Computation and Department of Chemistry, Emory University, 1515 Dickey Drive, Atlanta, Georgia 30322, United States.
J Phys Chem A. 2025 Mar 6;129(9):2238-2246. doi: 10.1021/acs.jpca.4c08620. Epub 2025 Feb 24.
There has been renewed interest in carbon nanoscale structures. Experimental measurements at 4.7 K and subsequent first-principles-based vibrational diffusion Monte Carlo simulations at 0 K recently showed that the aromatic cyclo[10]carbon prefers a pentagon-like structure to a regular decagon. This symmetry breaking is due to the second-order Jahn-Teller effect (JTE) and has been amply described in the literature for the cumulenic cyclo[4 + 2]carbon clusters. Yet temperature dependence of the JTE in cyclo[4 + 2]carbon clusters in general and the cyclo[10]carbon in particular has not been studied systematically. In this work, we employ path integral Monte Carlo simulations on a first-principles-derived permutationally invariant potential energy surface (PES) to examine the JTE in cyclo[10]carbon as a function of temperature. The PES was trained on a set of τHCTH/cc-pVQZ energies sampled up to ∼7.7 eV above the global minimum and locally adjusted to a high-level benchmark (reported by others) of the 812 cm electronic energy difference between the global minimum and the transition state. The calculations show a strong JTE at lower temperatures with a dominant composition at 100 K and a gradually diminishing JTE at higher temperatures with a washed-out pentagonal structure above 300 K.
人们对碳纳米结构重新产生了兴趣。最近在4.7 K下进行的实验测量以及随后在0 K下基于第一性原理的振动扩散蒙特卡罗模拟表明,芳香族环[10]碳更倾向于类似五边形的结构而非规则的十边形。这种对称性破缺是由于二阶 Jahn-Teller 效应(JTE),并且在文献中已经对累积环[4 + 2]碳簇进行了充分描述。然而,一般来说,环[4 + 2]碳簇尤其是环[10]碳中JTE的温度依赖性尚未得到系统研究。在这项工作中,我们在基于第一性原理推导的置换不变势能面(PES)上采用路径积分蒙特卡罗模拟,以研究环[10]碳中JTE随温度的变化。该PES是根据一组在比全局最小值高约7.7 eV处采样的τHCTH/cc-pVQZ能量进行训练的,并在局部调整到全局最小值与过渡态之间812 cm电子能量差的高水平基准(由其他人报告)。计算结果表明,在较低温度下存在强烈的JTE,在100 K时占主导成分,而在较高温度下JTE逐渐减弱,在300 K以上五边形结构消失。