A. N. Oraevsky, T.V. Sarkissian, D. J. Jones, D. K. Bandy
{"title":"单速度原子束脉泽动力学","authors":"A. N. Oraevsky, T.V. Sarkissian, D. J. Jones, D. K. Bandy","doi":"10.1364/nldos.1992.mb6","DOIUrl":null,"url":null,"abstract":"The dynamics of a beam maser, the first device in quantum electronics, was the subject of attention more than thirty years ago[1-4]. However, the interest in a beam masers has increased recently due to their applications in the study of fine quantum effects of atom interaction with the cavity field[5-6]. One of the most important feature of the presently used maser is a monovelocity atomic beam. A theory of a monovelocity beam maser was developed by Filipowicz et al.[7] and Guzman et al[8].","PeriodicalId":441335,"journal":{"name":"Nonlinear Dynamics in Optical Systems","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Dynamics of Monovelocity Atomic Beam Maser\",\"authors\":\"A. N. Oraevsky, T.V. Sarkissian, D. J. Jones, D. K. Bandy\",\"doi\":\"10.1364/nldos.1992.mb6\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The dynamics of a beam maser, the first device in quantum electronics, was the subject of attention more than thirty years ago[1-4]. However, the interest in a beam masers has increased recently due to their applications in the study of fine quantum effects of atom interaction with the cavity field[5-6]. One of the most important feature of the presently used maser is a monovelocity atomic beam. A theory of a monovelocity beam maser was developed by Filipowicz et al.[7] and Guzman et al[8].\",\"PeriodicalId\":441335,\"journal\":{\"name\":\"Nonlinear Dynamics in Optical Systems\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nonlinear Dynamics in Optical Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/nldos.1992.mb6\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nonlinear Dynamics in Optical Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/nldos.1992.mb6","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The dynamics of a beam maser, the first device in quantum electronics, was the subject of attention more than thirty years ago[1-4]. However, the interest in a beam masers has increased recently due to their applications in the study of fine quantum effects of atom interaction with the cavity field[5-6]. One of the most important feature of the presently used maser is a monovelocity atomic beam. A theory of a monovelocity beam maser was developed by Filipowicz et al.[7] and Guzman et al[8].
求助内容：
应助结果提醒方式：
京公网安备 11010802042870号
