{"title":"不同温度下D注入Ti的深度分布","authors":"J. Roth, W. Eckstein, J. Bohdansky","doi":"10.1080/00337578008209259","DOIUrl":null,"url":null,"abstract":"Abstract Depth proliles of 6.6 keV D+ implanted into titanium in the temperature range between 140 K and 500 K have been studied using the D(3He, α) H nuclear reaction. At 140 K the trapped amount is close to 100% at low doses and reaches saturation at about 2 × 1018D/cm2, whereas at room temperature no saturation could be reached up to 2 × 1019 D/cm2. At higher temperatures the amount decreases until no deuterium could be detected in the surface layer above 500 K. The depth profiles are strongly dependent on temperature. At 140 K the deuterium is found in a surface layer of about 2000 A with a maximum ratio of deuterium to metal atoms of 2.5. At room temperature a hydride layer of TiD1.8, forms. The thickness of the hydride layer depends on deuterium dose and extends to 1.5 μm at 2 × 1019 D/cm2. At higher temperatures the atom concentrations are lower and the deuterium seems to diffuse deeply into the bulk. These results are discussed in terms of diffusion of deuterium i n Ti and titanium hydride.","PeriodicalId":251043,"journal":{"name":"Ion Beam Modification of Materials","volume":"44 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"25","resultStr":"{\"title\":\"Depth Profiling of D Implanted into Ti at Different Temperatures\",\"authors\":\"J. Roth, W. Eckstein, J. Bohdansky\",\"doi\":\"10.1080/00337578008209259\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Abstract Depth proliles of 6.6 keV D+ implanted into titanium in the temperature range between 140 K and 500 K have been studied using the D(3He, α) H nuclear reaction. At 140 K the trapped amount is close to 100% at low doses and reaches saturation at about 2 × 1018D/cm2, whereas at room temperature no saturation could be reached up to 2 × 1019 D/cm2. At higher temperatures the amount decreases until no deuterium could be detected in the surface layer above 500 K. The depth profiles are strongly dependent on temperature. At 140 K the deuterium is found in a surface layer of about 2000 A with a maximum ratio of deuterium to metal atoms of 2.5. At room temperature a hydride layer of TiD1.8, forms. The thickness of the hydride layer depends on deuterium dose and extends to 1.5 μm at 2 × 1019 D/cm2. At higher temperatures the atom concentrations are lower and the deuterium seems to diffuse deeply into the bulk. These results are discussed in terms of diffusion of deuterium i n Ti and titanium hydride.\",\"PeriodicalId\":251043,\"journal\":{\"name\":\"Ion Beam Modification of Materials\",\"volume\":\"44 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"25\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Ion Beam Modification of Materials\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1080/00337578008209259\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Ion Beam Modification of Materials","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1080/00337578008209259","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Depth Profiling of D Implanted into Ti at Different Temperatures
Abstract Depth proliles of 6.6 keV D+ implanted into titanium in the temperature range between 140 K and 500 K have been studied using the D(3He, α) H nuclear reaction. At 140 K the trapped amount is close to 100% at low doses and reaches saturation at about 2 × 1018D/cm2, whereas at room temperature no saturation could be reached up to 2 × 1019 D/cm2. At higher temperatures the amount decreases until no deuterium could be detected in the surface layer above 500 K. The depth profiles are strongly dependent on temperature. At 140 K the deuterium is found in a surface layer of about 2000 A with a maximum ratio of deuterium to metal atoms of 2.5. At room temperature a hydride layer of TiD1.8, forms. The thickness of the hydride layer depends on deuterium dose and extends to 1.5 μm at 2 × 1019 D/cm2. At higher temperatures the atom concentrations are lower and the deuterium seems to diffuse deeply into the bulk. These results are discussed in terms of diffusion of deuterium i n Ti and titanium hydride.