{"title":"随时间漂移的哈密顿量","authors":"A. Boozer","doi":"10.1063/1.864525","DOIUrl":null,"url":null,"abstract":"The lowest‐order drift equations are given in a canonical magnetic coordinate form for time‐dependent magnetic and electric fields. The advantages of the canonical Hamiltonian form are also discussed.","PeriodicalId":22276,"journal":{"name":"The annual research report","volume":"51 1","pages":"2-13"},"PeriodicalIF":0.0000,"publicationDate":"1982-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"60","resultStr":"{\"title\":\"TIME DEPENDENT DRIFT HAMILTONIAN\",\"authors\":\"A. Boozer\",\"doi\":\"10.1063/1.864525\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The lowest‐order drift equations are given in a canonical magnetic coordinate form for time‐dependent magnetic and electric fields. The advantages of the canonical Hamiltonian form are also discussed.\",\"PeriodicalId\":22276,\"journal\":{\"name\":\"The annual research report\",\"volume\":\"51 1\",\"pages\":\"2-13\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1982-04-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"60\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The annual research report\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/1.864525\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The annual research report","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.864525","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The lowest‐order drift equations are given in a canonical magnetic coordinate form for time‐dependent magnetic and electric fields. The advantages of the canonical Hamiltonian form are also discussed.
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