B3LYP/6-31G*//SAM1 C36富勒烯和准富勒烯笼的计算

Z. Slanina, F. Uhlík, Xiang Zhao, H. Ueno, E. Ōsawa
{"title":"B3LYP/6-31G*//SAM1 C36富勒烯和准富勒烯笼的计算","authors":"Z. Slanina, F. Uhlík, Xiang Zhao, H. Ueno, E. Ōsawa","doi":"10.1080/10641220009351423","DOIUrl":null,"url":null,"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.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"32 1","pages":"433 - 447"},"PeriodicalIF":0.0000,"publicationDate":"2000-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"B3LYP/6-31G*//SAM1 Calculations of C36 Fullerene and quasi-Fullerene Cages\",\"authors\":\"Z. Slanina, F. Uhlík, Xiang Zhao, H. Ueno, E. Ōsawa\",\"doi\":\"10.1080/10641220009351423\",\"DOIUrl\":null,\"url\":null,\"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.\",\"PeriodicalId\":12470,\"journal\":{\"name\":\"Fullerene Science and Technology\",\"volume\":\"32 1\",\"pages\":\"433 - 447\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2000-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Fullerene Science and Technology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1080/10641220009351423\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Fullerene Science and Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1080/10641220009351423","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1

摘要

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。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
B3LYP/6-31G*//SAM1 Calculations of C36 Fullerene and quasi-Fullerene Cages
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.
求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信