{"title":"基本自旋性质和布洛赫方程","authors":"Hongyu An, Weili Lin","doi":"10.1002/0471142719.mib0300s13","DOIUrl":null,"url":null,"abstract":"In reality, spins are not isolated; instead, they interact with each other and their environment. The interaction of the spins with their surroundings leads to important modifications in their behavior. The experimentally determined spin-lattice relaxation time, T1, characterizes how quickly the longitudinal magnetization can grow back to its maximum value along the magnetic field direction. In contrast, T2 and T ∗ 2 are experimentally determined characteristic times describing the vanishing rate of the transverse magnetization. The T2 decay of signal is time-dependent and cannot be recovered, whereas part of the time-independent T ∗ 2 effect can be reversed by spin echo experiments.","PeriodicalId":100347,"journal":{"name":"Current Protocols in Magnetic Resonance Imaging","volume":"13 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2005-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1002/0471142719.mib0300s13","citationCount":"0","resultStr":"{\"title\":\"Basic Spin Properties and the Bloch Equations\",\"authors\":\"Hongyu An, Weili Lin\",\"doi\":\"10.1002/0471142719.mib0300s13\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In reality, spins are not isolated; instead, they interact with each other and their environment. The interaction of the spins with their surroundings leads to important modifications in their behavior. The experimentally determined spin-lattice relaxation time, T1, characterizes how quickly the longitudinal magnetization can grow back to its maximum value along the magnetic field direction. In contrast, T2 and T ∗ 2 are experimentally determined characteristic times describing the vanishing rate of the transverse magnetization. The T2 decay of signal is time-dependent and cannot be recovered, whereas part of the time-independent T ∗ 2 effect can be reversed by spin echo experiments.\",\"PeriodicalId\":100347,\"journal\":{\"name\":\"Current Protocols in Magnetic Resonance Imaging\",\"volume\":\"13 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2005-05-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1002/0471142719.mib0300s13\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Current Protocols in Magnetic Resonance Imaging\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/0471142719.mib0300s13\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Current Protocols in Magnetic Resonance Imaging","FirstCategoryId":"1085","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/0471142719.mib0300s13","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
In reality, spins are not isolated; instead, they interact with each other and their environment. The interaction of the spins with their surroundings leads to important modifications in their behavior. The experimentally determined spin-lattice relaxation time, T1, characterizes how quickly the longitudinal magnetization can grow back to its maximum value along the magnetic field direction. In contrast, T2 and T ∗ 2 are experimentally determined characteristic times describing the vanishing rate of the transverse magnetization. The T2 decay of signal is time-dependent and cannot be recovered, whereas part of the time-independent T ∗ 2 effect can be reversed by spin echo experiments.