{"title":"用极化中子测量贝里相","authors":"D. Dubbers","doi":"10.1016/0378-4363(88)90150-7","DOIUrl":null,"url":null,"abstract":"<div><p>When a quantum mechanical system is transported adiabatically around a closed circuit in parameter space, the system will, in addition to the usual dynamical phase, pick up a “topological”phase which depends only on the geometric history of the system. This phase, which is named after Berry who predicted it in 1984, has a number of exciting properties. We have measured these phases in neutron spin-rotation in helical magnetic fields.</p></div>","PeriodicalId":101023,"journal":{"name":"Physica B+C","volume":"151 1","pages":"Pages 93-95"},"PeriodicalIF":0.0000,"publicationDate":"1988-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0378-4363(88)90150-7","citationCount":"5","resultStr":"{\"title\":\"Measurement of the Berry phase with polarized neutrons\",\"authors\":\"D. Dubbers\",\"doi\":\"10.1016/0378-4363(88)90150-7\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>When a quantum mechanical system is transported adiabatically around a closed circuit in parameter space, the system will, in addition to the usual dynamical phase, pick up a “topological”phase which depends only on the geometric history of the system. This phase, which is named after Berry who predicted it in 1984, has a number of exciting properties. We have measured these phases in neutron spin-rotation in helical magnetic fields.</p></div>\",\"PeriodicalId\":101023,\"journal\":{\"name\":\"Physica B+C\",\"volume\":\"151 1\",\"pages\":\"Pages 93-95\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1988-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0378-4363(88)90150-7\",\"citationCount\":\"5\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physica B+C\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0378436388901507\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physica B+C","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0378436388901507","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Measurement of the Berry phase with polarized neutrons
When a quantum mechanical system is transported adiabatically around a closed circuit in parameter space, the system will, in addition to the usual dynamical phase, pick up a “topological”phase which depends only on the geometric history of the system. This phase, which is named after Berry who predicted it in 1984, has a number of exciting properties. We have measured these phases in neutron spin-rotation in helical magnetic fields.