{"title":"低功率85Rb CPT原子钟","authors":"S. Goka, T. Okura, M. Moroyama, Y. Watanabe","doi":"10.1109/FREQ.2008.4622966","DOIUrl":null,"url":null,"abstract":"This paper outlines the features of the <sup>85</sup>Rb vapor cell atomic clock, the coherent population trapping (CPT) resonance in an <sup>85</sup>Rb/<sup>87</sup>Rb mixed vapor cell, and the results of the frequency stabilities of a pilot system. The experiments were performed with a sealed vapor cell containing a natural mixture of Rb isotopes and a buffer gas. Excitation of the CPT resonance was accomplished using a vertical-cavity surface-emitting laser modulated at 1.5, 3.0, 3.4 and 6.8 GHz, which corresponded to the full- and half-ground-state hyperfine frequencies of <sup>85</sup>Rb and <sup>87</sup>Rb. The results show that the CPT resonances at both <sup>85</sup>Rb and <sup>87</sup>Rb can be observed separately. The frequency stabilities of the output signals for each CPT resonance were <10x10<sup>-12</sup>/day for <sup>85</sup>Rb and <6x10<sup>-12</sup>/day for <sup>87</sup>Rb. In addition, the RF modulation signal power for <sup>85</sup>Rb was 1.1 dB less than that of <sup>87</sup>Rb, which was 3.4 GHz.","PeriodicalId":220442,"journal":{"name":"2008 IEEE International Frequency Control Symposium","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2008-05-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":"{\"title\":\"Low power 85Rb CPT atomic clock\",\"authors\":\"S. Goka, T. Okura, M. Moroyama, Y. Watanabe\",\"doi\":\"10.1109/FREQ.2008.4622966\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This paper outlines the features of the <sup>85</sup>Rb vapor cell atomic clock, the coherent population trapping (CPT) resonance in an <sup>85</sup>Rb/<sup>87</sup>Rb mixed vapor cell, and the results of the frequency stabilities of a pilot system. The experiments were performed with a sealed vapor cell containing a natural mixture of Rb isotopes and a buffer gas. Excitation of the CPT resonance was accomplished using a vertical-cavity surface-emitting laser modulated at 1.5, 3.0, 3.4 and 6.8 GHz, which corresponded to the full- and half-ground-state hyperfine frequencies of <sup>85</sup>Rb and <sup>87</sup>Rb. The results show that the CPT resonances at both <sup>85</sup>Rb and <sup>87</sup>Rb can be observed separately. The frequency stabilities of the output signals for each CPT resonance were <10x10<sup>-12</sup>/day for <sup>85</sup>Rb and <6x10<sup>-12</sup>/day for <sup>87</sup>Rb. In addition, the RF modulation signal power for <sup>85</sup>Rb was 1.1 dB less than that of <sup>87</sup>Rb, which was 3.4 GHz.\",\"PeriodicalId\":220442,\"journal\":{\"name\":\"2008 IEEE International Frequency Control Symposium\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2008-05-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2008 IEEE International Frequency Control Symposium\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/FREQ.2008.4622966\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2008 IEEE International Frequency Control Symposium","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/FREQ.2008.4622966","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
This paper outlines the features of the 85Rb vapor cell atomic clock, the coherent population trapping (CPT) resonance in an 85Rb/87Rb mixed vapor cell, and the results of the frequency stabilities of a pilot system. The experiments were performed with a sealed vapor cell containing a natural mixture of Rb isotopes and a buffer gas. Excitation of the CPT resonance was accomplished using a vertical-cavity surface-emitting laser modulated at 1.5, 3.0, 3.4 and 6.8 GHz, which corresponded to the full- and half-ground-state hyperfine frequencies of 85Rb and 87Rb. The results show that the CPT resonances at both 85Rb and 87Rb can be observed separately. The frequency stabilities of the output signals for each CPT resonance were <10x10-12/day for 85Rb and <6x10-12/day for 87Rb. In addition, the RF modulation signal power for 85Rb was 1.1 dB less than that of 87Rb, which was 3.4 GHz.