{"title":"Ag掺杂对Ge2Sb2Te5薄膜电性能的影响","authors":"N. Kanda, A. Thakur, Abhinav Pratap Singh","doi":"10.1063/1.5113099","DOIUrl":null,"url":null,"abstract":"In this work thin films of the phase change material Ge2Sb2Te5 (GST), pure and Ag-doped, were studied. These films were prepared by thermal evaporation method. Amorphous nature of both pure and Ag-doped GST thin films has been confirmed from X-ray diffraction analysis. Raman spectra confirms the host structure of GST which is confirmed by the two sharp peaks at 126.4 cm−1 and 144.9 cm−1 for GST thin films. The hole concentration was found to increase by three orders of magnitude due to Ag doping, as measured by Hall measurements. I-V measurements of the samples show thermal switching at moderate voltage as large current flows through Ag-doped GST. The increase in conductivity was attributed to the crystallization of the films due to heating caused by the large electric current for I-V measurements.In this work thin films of the phase change material Ge2Sb2Te5 (GST), pure and Ag-doped, were studied. These films were prepared by thermal evaporation method. Amorphous nature of both pure and Ag-doped GST thin films has been confirmed from X-ray diffraction analysis. Raman spectra confirms the host structure of GST which is confirmed by the two sharp peaks at 126.4 cm−1 and 144.9 cm−1 for GST thin films. The hole concentration was found to increase by three orders of magnitude due to Ag doping, as measured by Hall measurements. I-V measurements of the samples show thermal switching at moderate voltage as large current flows through Ag-doped GST. The increase in conductivity was attributed to the crystallization of the films due to heating caused by the large electric current for I-V measurements.","PeriodicalId":10874,"journal":{"name":"DAE SOLID STATE PHYSICS SYMPOSIUM 2018","volume":"285 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2019-07-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Effect of Ag doping on electrical properties Ge2Sb2Te5 thin films\",\"authors\":\"N. Kanda, A. Thakur, Abhinav Pratap Singh\",\"doi\":\"10.1063/1.5113099\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this work thin films of the phase change material Ge2Sb2Te5 (GST), pure and Ag-doped, were studied. These films were prepared by thermal evaporation method. Amorphous nature of both pure and Ag-doped GST thin films has been confirmed from X-ray diffraction analysis. Raman spectra confirms the host structure of GST which is confirmed by the two sharp peaks at 126.4 cm−1 and 144.9 cm−1 for GST thin films. The hole concentration was found to increase by three orders of magnitude due to Ag doping, as measured by Hall measurements. I-V measurements of the samples show thermal switching at moderate voltage as large current flows through Ag-doped GST. The increase in conductivity was attributed to the crystallization of the films due to heating caused by the large electric current for I-V measurements.In this work thin films of the phase change material Ge2Sb2Te5 (GST), pure and Ag-doped, were studied. These films were prepared by thermal evaporation method. Amorphous nature of both pure and Ag-doped GST thin films has been confirmed from X-ray diffraction analysis. Raman spectra confirms the host structure of GST which is confirmed by the two sharp peaks at 126.4 cm−1 and 144.9 cm−1 for GST thin films. The hole concentration was found to increase by three orders of magnitude due to Ag doping, as measured by Hall measurements. I-V measurements of the samples show thermal switching at moderate voltage as large current flows through Ag-doped GST. The increase in conductivity was attributed to the crystallization of the films due to heating caused by the large electric current for I-V measurements.\",\"PeriodicalId\":10874,\"journal\":{\"name\":\"DAE SOLID STATE PHYSICS SYMPOSIUM 2018\",\"volume\":\"285 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-07-12\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"DAE SOLID STATE PHYSICS SYMPOSIUM 2018\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/1.5113099\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"DAE SOLID STATE PHYSICS SYMPOSIUM 2018","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.5113099","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Effect of Ag doping on electrical properties Ge2Sb2Te5 thin films
In this work thin films of the phase change material Ge2Sb2Te5 (GST), pure and Ag-doped, were studied. These films were prepared by thermal evaporation method. Amorphous nature of both pure and Ag-doped GST thin films has been confirmed from X-ray diffraction analysis. Raman spectra confirms the host structure of GST which is confirmed by the two sharp peaks at 126.4 cm−1 and 144.9 cm−1 for GST thin films. The hole concentration was found to increase by three orders of magnitude due to Ag doping, as measured by Hall measurements. I-V measurements of the samples show thermal switching at moderate voltage as large current flows through Ag-doped GST. The increase in conductivity was attributed to the crystallization of the films due to heating caused by the large electric current for I-V measurements.In this work thin films of the phase change material Ge2Sb2Te5 (GST), pure and Ag-doped, were studied. These films were prepared by thermal evaporation method. Amorphous nature of both pure and Ag-doped GST thin films has been confirmed from X-ray diffraction analysis. Raman spectra confirms the host structure of GST which is confirmed by the two sharp peaks at 126.4 cm−1 and 144.9 cm−1 for GST thin films. The hole concentration was found to increase by three orders of magnitude due to Ag doping, as measured by Hall measurements. I-V measurements of the samples show thermal switching at moderate voltage as large current flows through Ag-doped GST. The increase in conductivity was attributed to the crystallization of the films due to heating caused by the large electric current for I-V measurements.