Yingying Yang, Bin Li, Brian Johnson, Hal Banbrook
{"title":"一种确定放大器晶体管几何形状的新方法","authors":"Yingying Yang, Bin Li, Brian Johnson, Hal Banbrook","doi":"10.1109/BCICTS50416.2021.9682478","DOIUrl":null,"url":null,"abstract":"This method uses a new concept “Gain Number <tex>${\\left( {GN} \\right)}$</tex>” and “Transition Frequency <tex>${\\left( {f_{Tr}} \\right)}$</tex>” (between Maximum Stable Gain <tex>${\\left( {MSG} \\right)}$</tex> and Maximum Available Gain <tex>$\\left. {\\left( {MAG} \\right)} \\right)$</tex> as figures-of-merit to select a most suitable HBT device for a PA design of a certain required frequency <tex>${\\left( {f \\_ dsn} \\right)}$</tex>. The key is to establish relationships between <tex>${GN}$</tex> and <tex>${f_Tr}$</tex>, and the HBT's geometrical parameters and associated mathematical quantities: the ratio of an HBT's base pedestal area <tex>$\\left. {\\left( {A_B} \\right)} \\right)$</tex> to emitter area <tex>$\\left. {\\left( {A_E} \\right)} \\right)$</tex> and the product of base resistance <tex>$\\left. {\\left( {R_B} \\right)} \\right)$</tex> and <tex>${A_E}$</tex>.","PeriodicalId":284660,"journal":{"name":"2021 IEEE BiCMOS and Compound Semiconductor Integrated Circuits and Technology Symposium (BCICTS)","volume":"417 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2021-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A Novel Method to Determine Transistor Geometry for PA Design\",\"authors\":\"Yingying Yang, Bin Li, Brian Johnson, Hal Banbrook\",\"doi\":\"10.1109/BCICTS50416.2021.9682478\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This method uses a new concept “Gain Number <tex>${\\\\left( {GN} \\\\right)}$</tex>” and “Transition Frequency <tex>${\\\\left( {f_{Tr}} \\\\right)}$</tex>” (between Maximum Stable Gain <tex>${\\\\left( {MSG} \\\\right)}$</tex> and Maximum Available Gain <tex>$\\\\left. {\\\\left( {MAG} \\\\right)} \\\\right)$</tex> as figures-of-merit to select a most suitable HBT device for a PA design of a certain required frequency <tex>${\\\\left( {f \\\\_ dsn} \\\\right)}$</tex>. The key is to establish relationships between <tex>${GN}$</tex> and <tex>${f_Tr}$</tex>, and the HBT's geometrical parameters and associated mathematical quantities: the ratio of an HBT's base pedestal area <tex>$\\\\left. {\\\\left( {A_B} \\\\right)} \\\\right)$</tex> to emitter area <tex>$\\\\left. {\\\\left( {A_E} \\\\right)} \\\\right)$</tex> and the product of base resistance <tex>$\\\\left. {\\\\left( {R_B} \\\\right)} \\\\right)$</tex> and <tex>${A_E}$</tex>.\",\"PeriodicalId\":284660,\"journal\":{\"name\":\"2021 IEEE BiCMOS and Compound Semiconductor Integrated Circuits and Technology Symposium (BCICTS)\",\"volume\":\"417 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2021-12-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2021 IEEE BiCMOS and Compound Semiconductor Integrated Circuits and Technology Symposium (BCICTS)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/BCICTS50416.2021.9682478\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2021 IEEE BiCMOS and Compound Semiconductor Integrated Circuits and Technology Symposium (BCICTS)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/BCICTS50416.2021.9682478","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A Novel Method to Determine Transistor Geometry for PA Design
This method uses a new concept “Gain Number ${\left( {GN} \right)}$” and “Transition Frequency ${\left( {f_{Tr}} \right)}$” (between Maximum Stable Gain ${\left( {MSG} \right)}$ and Maximum Available Gain $\left. {\left( {MAG} \right)} \right)$ as figures-of-merit to select a most suitable HBT device for a PA design of a certain required frequency ${\left( {f \_ dsn} \right)}$. The key is to establish relationships between ${GN}$ and ${f_Tr}$, and the HBT's geometrical parameters and associated mathematical quantities: the ratio of an HBT's base pedestal area $\left. {\left( {A_B} \right)} \right)$ to emitter area $\left. {\left( {A_E} \right)} \right)$ and the product of base resistance $\left. {\left( {R_B} \right)} \right)$ and ${A_E}$.