首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Search for Lowest-Energy Fullerenes 2:C38 to C80 and C112 to C120
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Search for Lowest-Energy Fullerenes 2:C38 to C80 and C112 to C120

机译:搜索最低能量富勒烯2:C38至C80和C112至C120

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An efficient computational approach that combines semiempirical density-functional based tight-binding method(DFTB)for geometry optimization and density-functional theory for single-point energy calculation is employed to search for the lowest-energy structures of higher fullerenes C110 to C120.In addition,a systematic study of low-lying structures of lower fullerenes C38 to C80 is undertaken.For the latter study,the targeted isomers amount to 131 164,including 17 IPR(isolated pentagon rule)isomers and all non-IPR isomers.Non-IPR isomers dominate the low-lying population of C72 but are gradually phased out of the low-lying population when the fullerene size increases toward C80.An unexpected manner of pentagonal adjacency was observed,that is,for fullerenes containing an adjacent-pentagon chain with less than five pentagons,the longer chain incurs less energy penalty than the shorter chain when the top-two lowest-energy fullerene cages(for all C38-C70)have the same number of adjacent pentagons.For higher fullerenes C112 to C120,a full set of total 32 795 IPR isomers were optimized using the DFTB method.An energy cutoff value of 6.3 kcal/mol was used to collect low-lying candidate isomers for the second-stage single-point energy calculation at the DFT level.Multiple candidates for the lowest-energy structure were identified for C112,C118,and C120.Among them,C112:3299 and C118:7308 exhibit a large HOMO-LUMO gap.For C116,a sole candidate for the lowest-energy structure was identified,namely,C116:6061 which has a high T_h symmetry and a large HOMO-LUMO gap and is 12.5 kcal/mol lower in energy than the second lowest-energy isomer.Thus,C116:6061 is most likely to be isolated first in the laboratory among the five large fullerenes.~(13)C NMR spectra of the ten lowest-energy isomers of C112 to C120 were calculated for comparison with the experiment.
机译:一种有效的计算方法结合了基于半经验的基于密度泛函的紧密结合方法(DFTB)进行几何优化,并采用密度泛函理论进行单点能量计算,以寻找高碳富勒烯C110至C120的最低能级结构。此外,还对低级富勒烯C38至C80的低位结构进行了系统研究。在后者的研究中,目标异构体为131164,包括17种IPR(孤立的五边形规则)异构体和所有非IPR异构体。 IPR异构体在C72的低洼人群中占主导地位,但当富勒烯的尺寸向C80增大时逐渐从低洼人群中逐步淘汰。观察到了一种意外的五边形邻接方式,即含有相邻五边形链的富勒烯与少于五个五边形,当前两个最低能量的富勒烯笼(对于所有C38-C70)具有相同数量的相邻p时,较长的链比较短的链产生的能量损失少对于较高的富勒烯C112至C120,使用DFTB方法对全套32 795种IPR异构体进行了优化。能量截断值6.3 kcal / mol用于收集第二阶段单分子筛的低位候选异构体。在DFT级别上进行点能量计算。确定了C112,C118和C120的多个最低能量结构的候选对象,其中C112:3299和C118:7308的HOMO-LUMO间隙较大。对于C116,唯一的候选对象确定了最低能级结构的C116:6061,它具有高T_h对称性和较大的HOMO-LUMO间隙,并且比第二低能级异构体的能量低12.5 kcal / mol。在五个大富勒烯中最有可能最先被分离出来。计算出C112至C120的十种最低能级异构体的〜(13)C NMR光谱,与实验进行比较。

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