R. Ichihara, Kunifumi Suzuki, H. Kusai, K. Ariyoshi, Keisuke Akari, Keisuke Takano, K. Matsuo, Y. Kamiya, Kota Takahashi, Hidenori Miyazawa, Y. Kamimuta, K. Sakuma, M. Saitoh
{"title":"基于记忆过程中自发极化和陷阱电荷直接提取的HfO2 ffet的Vth窗口和可靠性再检验","authors":"R. Ichihara, Kunifumi Suzuki, H. Kusai, K. Ariyoshi, Keisuke Akari, Keisuke Takano, K. Matsuo, Y. Kamiya, Kota Takahashi, Hidenori Miyazawa, Y. Kamimuta, K. Sakuma, M. Saitoh","doi":"10.1109/VLSITechnology18217.2020.9265055","DOIUrl":null,"url":null,"abstract":"We re-examine the dominant factors of the memory window (MW) and reliability of HfO<inf>2</inf> FeFET using a new technique to extract both spontaneous polarization <tex>$(\\mathrm{P}_{\\mathrm{s}})$</tex> and interface trap charges <tex>$(\\mathrm{Q}_{\\mathrm{t}})$</tex> by one-time current measurement of an FeFET during the memory operation. FeFET characteristics are strongly affected by unstable <tex>$\\mathrm{Q}_{t}$</tex> (unrelated to ferroelectric) which causes <tex>$\\mathrm{V}_{\\mathrm{th}}$</tex> instability just after programming, and stable <tex>$\\mathrm{Q}_{1}$</tex> which compensates most of electric(E)- field generated by <tex>$\\mathrm{P}_{\\mathrm{s}}$</tex>. Stable <tex>$\\mathrm{Q}_{\\mathrm{t}}$</tex> is coupled to <tex>$\\mathrm{P}_{\\mathrm{s}}$</tex> with constant ratio (~90%), and reduce MW to the value much lower than the coercive voltage <tex>$(\\mathrm{V}_{\\mathrm{c}})$</tex> limitation. Unlike the conventional model, <tex>$\\mathrm{P}_{\\mathrm{s}}$</tex> increase and stabilization are still effective to improve MW and retention, respectively. During cycling, MW is degraded by <tex>$\\Delta \\mathrm{P}_{\\mathrm{s}}$</tex> reduction as well as the increase of the compensation ratio <tex>$(\\Delta \\mathrm{Q}_{\\mathrm{t}}/\\Delta \\mathrm{P}_{\\mathrm{s}})$</tex> which can be mitigated by suppressing charge injection/ejection via interfacial <tex>$\\mathrm{SiO}_{2}$</tex>.","PeriodicalId":6850,"journal":{"name":"2020 IEEE Symposium on VLSI Technology","volume":"36 1","pages":"1-2"},"PeriodicalIF":0.0000,"publicationDate":"2020-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"20","resultStr":"{\"title\":\"Re-examination of Vth Window and Reliability in HfO2 FeFET Based on the Direct Extraction of Spontaneous Polarization and Trap Charge during Memory Operation\",\"authors\":\"R. Ichihara, Kunifumi Suzuki, H. Kusai, K. Ariyoshi, Keisuke Akari, Keisuke Takano, K. Matsuo, Y. Kamiya, Kota Takahashi, Hidenori Miyazawa, Y. Kamimuta, K. Sakuma, M. Saitoh\",\"doi\":\"10.1109/VLSITechnology18217.2020.9265055\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We re-examine the dominant factors of the memory window (MW) and reliability of HfO<inf>2</inf> FeFET using a new technique to extract both spontaneous polarization <tex>$(\\\\mathrm{P}_{\\\\mathrm{s}})$</tex> and interface trap charges <tex>$(\\\\mathrm{Q}_{\\\\mathrm{t}})$</tex> by one-time current measurement of an FeFET during the memory operation. FeFET characteristics are strongly affected by unstable <tex>$\\\\mathrm{Q}_{t}$</tex> (unrelated to ferroelectric) which causes <tex>$\\\\mathrm{V}_{\\\\mathrm{th}}$</tex> instability just after programming, and stable <tex>$\\\\mathrm{Q}_{1}$</tex> which compensates most of electric(E)- field generated by <tex>$\\\\mathrm{P}_{\\\\mathrm{s}}$</tex>. Stable <tex>$\\\\mathrm{Q}_{\\\\mathrm{t}}$</tex> is coupled to <tex>$\\\\mathrm{P}_{\\\\mathrm{s}}$</tex> with constant ratio (~90%), and reduce MW to the value much lower than the coercive voltage <tex>$(\\\\mathrm{V}_{\\\\mathrm{c}})$</tex> limitation. Unlike the conventional model, <tex>$\\\\mathrm{P}_{\\\\mathrm{s}}$</tex> increase and stabilization are still effective to improve MW and retention, respectively. During cycling, MW is degraded by <tex>$\\\\Delta \\\\mathrm{P}_{\\\\mathrm{s}}$</tex> reduction as well as the increase of the compensation ratio <tex>$(\\\\Delta \\\\mathrm{Q}_{\\\\mathrm{t}}/\\\\Delta \\\\mathrm{P}_{\\\\mathrm{s}})$</tex> which can be mitigated by suppressing charge injection/ejection via interfacial <tex>$\\\\mathrm{SiO}_{2}$</tex>.\",\"PeriodicalId\":6850,\"journal\":{\"name\":\"2020 IEEE Symposium on VLSI Technology\",\"volume\":\"36 1\",\"pages\":\"1-2\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2020-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"20\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2020 IEEE Symposium on VLSI Technology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/VLSITechnology18217.2020.9265055\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2020 IEEE Symposium on VLSI Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/VLSITechnology18217.2020.9265055","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Re-examination of Vth Window and Reliability in HfO2 FeFET Based on the Direct Extraction of Spontaneous Polarization and Trap Charge during Memory Operation
We re-examine the dominant factors of the memory window (MW) and reliability of HfO2 FeFET using a new technique to extract both spontaneous polarization $(\mathrm{P}_{\mathrm{s}})$ and interface trap charges $(\mathrm{Q}_{\mathrm{t}})$ by one-time current measurement of an FeFET during the memory operation. FeFET characteristics are strongly affected by unstable $\mathrm{Q}_{t}$ (unrelated to ferroelectric) which causes $\mathrm{V}_{\mathrm{th}}$ instability just after programming, and stable $\mathrm{Q}_{1}$ which compensates most of electric(E)- field generated by $\mathrm{P}_{\mathrm{s}}$. Stable $\mathrm{Q}_{\mathrm{t}}$ is coupled to $\mathrm{P}_{\mathrm{s}}$ with constant ratio (~90%), and reduce MW to the value much lower than the coercive voltage $(\mathrm{V}_{\mathrm{c}})$ limitation. Unlike the conventional model, $\mathrm{P}_{\mathrm{s}}$ increase and stabilization are still effective to improve MW and retention, respectively. During cycling, MW is degraded by $\Delta \mathrm{P}_{\mathrm{s}}$ reduction as well as the increase of the compensation ratio $(\Delta \mathrm{Q}_{\mathrm{t}}/\Delta \mathrm{P}_{\mathrm{s}})$ which can be mitigated by suppressing charge injection/ejection via interfacial $\mathrm{SiO}_{2}$.