{"title":"由激光偏振的快速变化引起的瞬态CPT信号","authors":"J. Camparo, M. Huang, J. Coffer","doi":"10.1109/FREQ.2008.4623082","DOIUrl":null,"url":null,"abstract":"In chip-scale atomic clocks based on coherent-population-trapping (CPT), the laser of choice is a VCSEL due to its low threshold current, very high quantum efficiency, and large dynamic bandwidth. A problem with these lasers, however, is that they suffer from polarization fluctuations, which could degrade CPT signal-to-noise ratios. In previous work we found that a rapid change in laser polarization led to a multi-exponential variation of the light intensity transmitted through a resonant Rb vapor. Here, we show that this is not a systematic effect, but is a result of atomic dynamics. Specifically, we show that the change in transmitted light intensity arises from both a change in the system's trapping state and a re-establishment of the atomic coherence that is at the heart of the CPT signal.","PeriodicalId":220442,"journal":{"name":"2008 IEEE International Frequency Control Symposium","volume":"321 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2008-05-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Transient CPT signals arising from rapid changes in laser polarization\",\"authors\":\"J. Camparo, M. Huang, J. Coffer\",\"doi\":\"10.1109/FREQ.2008.4623082\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In chip-scale atomic clocks based on coherent-population-trapping (CPT), the laser of choice is a VCSEL due to its low threshold current, very high quantum efficiency, and large dynamic bandwidth. A problem with these lasers, however, is that they suffer from polarization fluctuations, which could degrade CPT signal-to-noise ratios. In previous work we found that a rapid change in laser polarization led to a multi-exponential variation of the light intensity transmitted through a resonant Rb vapor. Here, we show that this is not a systematic effect, but is a result of atomic dynamics. Specifically, we show that the change in transmitted light intensity arises from both a change in the system's trapping state and a re-establishment of the atomic coherence that is at the heart of the CPT signal.\",\"PeriodicalId\":220442,\"journal\":{\"name\":\"2008 IEEE International Frequency Control Symposium\",\"volume\":\"321 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2008-05-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2008 IEEE International Frequency Control Symposium\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/FREQ.2008.4623082\",\"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.2008.4623082","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Transient CPT signals arising from rapid changes in laser polarization
In chip-scale atomic clocks based on coherent-population-trapping (CPT), the laser of choice is a VCSEL due to its low threshold current, very high quantum efficiency, and large dynamic bandwidth. A problem with these lasers, however, is that they suffer from polarization fluctuations, which could degrade CPT signal-to-noise ratios. In previous work we found that a rapid change in laser polarization led to a multi-exponential variation of the light intensity transmitted through a resonant Rb vapor. Here, we show that this is not a systematic effect, but is a result of atomic dynamics. Specifically, we show that the change in transmitted light intensity arises from both a change in the system's trapping state and a re-establishment of the atomic coherence that is at the heart of the CPT signal.