B. Hinds, A. Dutta, F. Yun, T. Yamanaka, S. Hatanani, S. Oda
{"title":"Single electron memory utilizing nano-crystalline Si over short-channel silicon-on-insulator transistors","authors":"B. Hinds, A. Dutta, F. Yun, T. Yamanaka, S. Hatanani, S. Oda","doi":"10.1109/DRC.2000.877127","DOIUrl":null,"url":null,"abstract":"A promising approach for high density/low power consumption memory devices is to store a single charge in a nano-scale memory node, which affects electron transport in a nearby channel. Advantages of this design are room temperature operation and self limiting charge storage by Coulomb repulsion. Two notable approaches to this concept are nanocrystalline-Si (nc-Si) acting as a floating gate in a large area MOSFET (Tiwari et al., 1996) and a single polysilicon dot defined by e-beam lithography over a narrow SOI channel (Guo et al., 1997). A device which is sensitive to a single charge while using a method of nc-Si dot fabrication that is scalable to VLSI is required. Single electron memory devices based on two approaches of forming nc-Si with large area deposition processes are reported here. To make the active region of the device sensitive to a single charged dot, narrow channels (40 nm length by 30 nm width) are defined by e-beam lithography of thin (20 nm) SOI. The first approach for nc-Si synthesis is gas phase nucleation and growth by pulsed-source remote PECVD, which form 8/spl plusmn/1 nm diameter nc-Si dots (Ifuku et al., 1997). The second approach for scalable nc-Si formation is to deposit a thin film of SiO/sub x/ (x<2). Annealing of this film results in high density 3-8 nm nc-Si dots isolated from each other by a SiO/sub 2/ tunnel barrier (Hamasaki et al., 1978).","PeriodicalId":126654,"journal":{"name":"58th DRC. Device Research Conference. Conference Digest (Cat. No.00TH8526)","volume":"9 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2000-06-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"58th DRC. Device Research Conference. Conference Digest (Cat. No.00TH8526)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DRC.2000.877127","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
A promising approach for high density/low power consumption memory devices is to store a single charge in a nano-scale memory node, which affects electron transport in a nearby channel. Advantages of this design are room temperature operation and self limiting charge storage by Coulomb repulsion. Two notable approaches to this concept are nanocrystalline-Si (nc-Si) acting as a floating gate in a large area MOSFET (Tiwari et al., 1996) and a single polysilicon dot defined by e-beam lithography over a narrow SOI channel (Guo et al., 1997). A device which is sensitive to a single charge while using a method of nc-Si dot fabrication that is scalable to VLSI is required. Single electron memory devices based on two approaches of forming nc-Si with large area deposition processes are reported here. To make the active region of the device sensitive to a single charged dot, narrow channels (40 nm length by 30 nm width) are defined by e-beam lithography of thin (20 nm) SOI. The first approach for nc-Si synthesis is gas phase nucleation and growth by pulsed-source remote PECVD, which form 8/spl plusmn/1 nm diameter nc-Si dots (Ifuku et al., 1997). The second approach for scalable nc-Si formation is to deposit a thin film of SiO/sub x/ (x<2). Annealing of this film results in high density 3-8 nm nc-Si dots isolated from each other by a SiO/sub 2/ tunnel barrier (Hamasaki et al., 1978).