R. Kishikawa, M. Horibe, A. Miyachi, M. Matsunoshita, S. Kawasaki
{"title":"Uncertainty estimation for gallium nitride diode model based on VNA measurement at 5.8 GHz","authors":"R. Kishikawa, M. Horibe, A. Miyachi, M. Matsunoshita, S. Kawasaki","doi":"10.1109/CPEM.2016.7540753","DOIUrl":null,"url":null,"abstract":"This paper summarizes the uncertainty estimation for gallium nitride shottky diode based on vector network analyzer measurements at 5.8 GHz. The results were traceable to the metrology standard of S-parameter at NMIJ. Considering the uncertainty of the measurements, bias voltage must be applied over 2 V in measuring bias voltage dependence of reflection coefficient. The measurement uncertainty was propagated from reflection coefficient to impedance. As a result, the expanded uncertainty of real and imaginary part of impedance were 0.56 Ω and 0.57 Ω at 5.8 GHz, respectively.","PeriodicalId":415488,"journal":{"name":"2016 Conference on Precision Electromagnetic Measurements (CPEM 2016)","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2016-07-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2016 Conference on Precision Electromagnetic Measurements (CPEM 2016)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CPEM.2016.7540753","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
This paper summarizes the uncertainty estimation for gallium nitride shottky diode based on vector network analyzer measurements at 5.8 GHz. The results were traceable to the metrology standard of S-parameter at NMIJ. Considering the uncertainty of the measurements, bias voltage must be applied over 2 V in measuring bias voltage dependence of reflection coefficient. The measurement uncertainty was propagated from reflection coefficient to impedance. As a result, the expanded uncertainty of real and imaginary part of impedance were 0.56 Ω and 0.57 Ω at 5.8 GHz, respectively.