{"title":"蒸汽电池时钟频率和环境压力:共振电池体积变化","authors":"M. Huang, C. Klimcak, J. Camparo","doi":"10.1109/FREQ.2010.5556344","DOIUrl":null,"url":null,"abstract":"For space-qualified vapor-cell atomic clocks, the pressure-shift coefficient describes the frequency change as the device transitions from atmospheric pressure to vacuum. Two processes are known to affect this frequency change: a thermal pathways mechanism and a resonance-cell volume mechanism (i.e., the so-called barometric frequency shift). Here, we focus on the barometric frequency shift, and employ finite element methods to examine how the barometric shift depends on resonance-cell size and wall thickness.","PeriodicalId":344989,"journal":{"name":"2010 IEEE International Frequency Control Symposium","volume":"420 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2010-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":"{\"title\":\"Vapor-cell clock frequency and environmental pressure: Resonance-cell volume changes\",\"authors\":\"M. Huang, C. Klimcak, J. Camparo\",\"doi\":\"10.1109/FREQ.2010.5556344\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"For space-qualified vapor-cell atomic clocks, the pressure-shift coefficient describes the frequency change as the device transitions from atmospheric pressure to vacuum. Two processes are known to affect this frequency change: a thermal pathways mechanism and a resonance-cell volume mechanism (i.e., the so-called barometric frequency shift). Here, we focus on the barometric frequency shift, and employ finite element methods to examine how the barometric shift depends on resonance-cell size and wall thickness.\",\"PeriodicalId\":344989,\"journal\":{\"name\":\"2010 IEEE International Frequency Control Symposium\",\"volume\":\"420 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2010-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"6\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2010 IEEE International Frequency Control Symposium\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/FREQ.2010.5556344\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2010 IEEE International Frequency Control Symposium","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/FREQ.2010.5556344","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Vapor-cell clock frequency and environmental pressure: Resonance-cell volume changes
For space-qualified vapor-cell atomic clocks, the pressure-shift coefficient describes the frequency change as the device transitions from atmospheric pressure to vacuum. Two processes are known to affect this frequency change: a thermal pathways mechanism and a resonance-cell volume mechanism (i.e., the so-called barometric frequency shift). Here, we focus on the barometric frequency shift, and employ finite element methods to examine how the barometric shift depends on resonance-cell size and wall thickness.