{"title":"类锗离子中最低奇宇称组态的研究","authors":"A. Wajid, S. Jabeen","doi":"10.26713/JAMCNP.V3I1.344","DOIUrl":null,"url":null,"abstract":"Fine structure energy levels, transition probabilities and oscillator strength for terms belonging to the ground configuration, \\(\\rm 4s^{2}4p^{2}\\) and the first exited odd parity configurations \\(\\rm 4s4p^{3}\\), \\(\\rm 4s^24p5s\\) and \\(\\rm 4s^{2}4p4d\\) of Ge-I like ions have been calculated using Hartree-Fock method with relativistic correction incorporating large number of interacting configurations \\(\\rm[4s^{2}4p(4f+5p+5g), 4s4p^{2}(4d+5s), 4p^{3}(4d+5s)]\\). Experimentally reported levels have been compared with theoretical results establishing energy parameters in the first eleven members of the sequence (Ge I-Mo XI). The configuration \\(\\rm 4s^{2}4p4d\\) in Rb VI, Sr VII, and \\(\\rm 4s4p^3\\) except \\(\\rm 4s4p^{3}\\) \\(\\rm^{5}S_2\\) level in Ge-I, are not observed yet. A systematic study of Slater parameters in the isoelectronic sequence enabled us to make precise predictions of the missing energy levels belonging to these configurations.","PeriodicalId":239838,"journal":{"name":"Journal of Atomic, Molecular, Condensate and Nano Physics","volume":"10 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2016-01-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Study of Lowest Odd Parity Configurations in Ge-I Like Ions\",\"authors\":\"A. Wajid, S. Jabeen\",\"doi\":\"10.26713/JAMCNP.V3I1.344\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Fine structure energy levels, transition probabilities and oscillator strength for terms belonging to the ground configuration, \\\\(\\\\rm 4s^{2}4p^{2}\\\\) and the first exited odd parity configurations \\\\(\\\\rm 4s4p^{3}\\\\), \\\\(\\\\rm 4s^24p5s\\\\) and \\\\(\\\\rm 4s^{2}4p4d\\\\) of Ge-I like ions have been calculated using Hartree-Fock method with relativistic correction incorporating large number of interacting configurations \\\\(\\\\rm[4s^{2}4p(4f+5p+5g), 4s4p^{2}(4d+5s), 4p^{3}(4d+5s)]\\\\). Experimentally reported levels have been compared with theoretical results establishing energy parameters in the first eleven members of the sequence (Ge I-Mo XI). The configuration \\\\(\\\\rm 4s^{2}4p4d\\\\) in Rb VI, Sr VII, and \\\\(\\\\rm 4s4p^3\\\\) except \\\\(\\\\rm 4s4p^{3}\\\\) \\\\(\\\\rm^{5}S_2\\\\) level in Ge-I, are not observed yet. A systematic study of Slater parameters in the isoelectronic sequence enabled us to make precise predictions of the missing energy levels belonging to these configurations.\",\"PeriodicalId\":239838,\"journal\":{\"name\":\"Journal of Atomic, Molecular, Condensate and Nano Physics\",\"volume\":\"10 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2016-01-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Atomic, Molecular, Condensate and Nano Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.26713/JAMCNP.V3I1.344\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Atomic, Molecular, Condensate and Nano Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.26713/JAMCNP.V3I1.344","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Study of Lowest Odd Parity Configurations in Ge-I Like Ions
Fine structure energy levels, transition probabilities and oscillator strength for terms belonging to the ground configuration, \(\rm 4s^{2}4p^{2}\) and the first exited odd parity configurations \(\rm 4s4p^{3}\), \(\rm 4s^24p5s\) and \(\rm 4s^{2}4p4d\) of Ge-I like ions have been calculated using Hartree-Fock method with relativistic correction incorporating large number of interacting configurations \(\rm[4s^{2}4p(4f+5p+5g), 4s4p^{2}(4d+5s), 4p^{3}(4d+5s)]\). Experimentally reported levels have been compared with theoretical results establishing energy parameters in the first eleven members of the sequence (Ge I-Mo XI). The configuration \(\rm 4s^{2}4p4d\) in Rb VI, Sr VII, and \(\rm 4s4p^3\) except \(\rm 4s4p^{3}\) \(\rm^{5}S_2\) level in Ge-I, are not observed yet. A systematic study of Slater parameters in the isoelectronic sequence enabled us to make precise predictions of the missing energy levels belonging to these configurations.