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}
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.