{"title":"at切割石英晶体中辐射诱导的频率偏移和声损失","authors":"J.J. Martin","doi":"10.1109/FREQ.1989.68913","DOIUrl":null,"url":null,"abstract":"The acoustic loss and frequency versus temperature spectra are measured as a function of radiation dose for a number of matching Na-swept crystals and for H-swept AT-cut quartz crystals. As expected, large positive frequency offsets at both the upper and lower turnovers were observed for the Na-swept crystals. However, the magnitude of the offset was consistently much smaller than the change in height of the strong 53 K (5 MHz) Al-Na loss peak. This smaller offset was caused by a change in the 'apparent' angle of the crystal that comes about when the Al-Na center is replaced by the Al-OH or Al-hole center. The offsets of the swept crystals were usually smaller than those of the unswept samples. Only part of the observed fractional frequency offset at the turnovers could be explained by summing the heights of the loss peak changes. An additional radiation-induced offset was observed at temperatures below 15 K where the frequency versus temperature curves flatten out.<<ETX>>","PeriodicalId":294361,"journal":{"name":"Proceedings of the 43rd Annual Symposium on Frequency Control","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1989-05-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Radiation induced frequency offsets and acoustic loss in AT-cut quartz crystals\",\"authors\":\"J.J. Martin\",\"doi\":\"10.1109/FREQ.1989.68913\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The acoustic loss and frequency versus temperature spectra are measured as a function of radiation dose for a number of matching Na-swept crystals and for H-swept AT-cut quartz crystals. As expected, large positive frequency offsets at both the upper and lower turnovers were observed for the Na-swept crystals. However, the magnitude of the offset was consistently much smaller than the change in height of the strong 53 K (5 MHz) Al-Na loss peak. This smaller offset was caused by a change in the 'apparent' angle of the crystal that comes about when the Al-Na center is replaced by the Al-OH or Al-hole center. The offsets of the swept crystals were usually smaller than those of the unswept samples. Only part of the observed fractional frequency offset at the turnovers could be explained by summing the heights of the loss peak changes. An additional radiation-induced offset was observed at temperatures below 15 K where the frequency versus temperature curves flatten out.<<ETX>>\",\"PeriodicalId\":294361,\"journal\":{\"name\":\"Proceedings of the 43rd Annual Symposium on Frequency Control\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1989-05-31\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of the 43rd Annual Symposium on Frequency Control\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/FREQ.1989.68913\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the 43rd Annual Symposium on Frequency Control","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/FREQ.1989.68913","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
摘要
对于一些匹配的na扫描晶体和h扫描at切割石英晶体,测量了声损失和频率随温度谱作为辐射剂量的函数。正如预期的那样,在na扫描晶体的上下翻转处观察到大的正频率偏移。然而,偏移量的大小始终远小于强53 K (5 MHz) Al-Na损耗峰高度的变化。这种较小的偏移是由于当Al-Na中心被Al-OH或Al-hole中心取代时,晶体的“视角”发生了变化。扫描晶体的偏移量通常小于未扫描样品的偏移量。只有部分观察到的分数频率偏移可以用损耗峰变化的总和来解释。在温度低于15 K时,观察到额外的辐射引起的偏移,此时频率与温度曲线趋于平缓。
Radiation induced frequency offsets and acoustic loss in AT-cut quartz crystals
The acoustic loss and frequency versus temperature spectra are measured as a function of radiation dose for a number of matching Na-swept crystals and for H-swept AT-cut quartz crystals. As expected, large positive frequency offsets at both the upper and lower turnovers were observed for the Na-swept crystals. However, the magnitude of the offset was consistently much smaller than the change in height of the strong 53 K (5 MHz) Al-Na loss peak. This smaller offset was caused by a change in the 'apparent' angle of the crystal that comes about when the Al-Na center is replaced by the Al-OH or Al-hole center. The offsets of the swept crystals were usually smaller than those of the unswept samples. Only part of the observed fractional frequency offset at the turnovers could be explained by summing the heights of the loss peak changes. An additional radiation-induced offset was observed at temperatures below 15 K where the frequency versus temperature curves flatten out.<>