B3LYP/6-31G*//SAM1 Calculations of C36 Fullerene and quasi-Fullerene Cages

Z. Slanina, F. Uhlík, Xiang Zhao, H. Ueno, E. Ōsawa
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引用次数: 1

Abstract

Abstract The recently isolated fullerene C36 is computed by the SAM1 method with energetics refined at the B3LYP/6-31G* level. Twelve low-energy cages are considered in detail, exhibiting both fullerene (pentagons and hexagons) and quasi-fullerene (also squares and heptagons) pattern. In contrast to other fullerene systems, the SAM1 and B3LYP/6-31G* methods do produce somewhat different energetics. Consequently, the equilibrium isomeric composition at high temperatures is different, too. In the best affordable B3LYP/6-31G* approach the fullerene cage with the topological D 6d symmetry represents the most populated species at high temperatures. Hence, an agreement with the solid-state NMR experiment is achieved at the B3LYP/6-31G* theoretical level.
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B3LYP/6-31G*//SAM1 C36富勒烯和准富勒烯笼的计算
摘要采用SAM1方法计算了最近分离的富勒烯C36,能量学在B3LYP/6-31G*水平上进行了改进。对12个低能笼进行了详细的研究,显示了富勒烯(五角形和六角形)和准富勒烯(方形和七角形)的模式。与其他富勒烯体系相比,SAM1和B3LYP/6-31G*方法确实产生了一些不同的能量学。因此,高温下的平衡异构体组成也不同。在最经济的B3LYP/6-31G*方法中,具有拓扑D - 6d对称性的富勒烯笼在高温下代表了最多的物种。因此,在B3LYP/6-31G*理论水平上与固体核磁共振实验结果一致。
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