Theoretical Analysis of Planar Flat Floating Gate NAND Flash Device and Experimental Study of Floating-Gate (FG) / Charge-Trapping (CT) Fusion Device for Comprehensive Understanding of Charge Storage and Operation Principle

H. Lue, P. Du, R. Lo, Chih-Yuan Lu
{"title":"Theoretical Analysis of Planar Flat Floating Gate NAND Flash Device and Experimental Study of Floating-Gate (FG) / Charge-Trapping (CT) Fusion Device for Comprehensive Understanding of Charge Storage and Operation Principle","authors":"H. Lue, P. Du, R. Lo, Chih-Yuan Lu","doi":"10.1109/IMW.2016.7495292","DOIUrl":null,"url":null,"abstract":"The planar flat FG device is theoretically studied extensively. There is a puzzle whether the charge is stored in the inter gate dielectric (IGD). A planar cell has no geometrical coupling ratio help thus IGD bears very high E-field. A high work function FG together with a robust interfacial layer between FG and high-K material that has both large barrier height and large dielectric constant are needed to reduce the out tunneling current. Thus our detailed tunneling simulation indicates that to obtain an “ideal planar FG” device with a large memory window but without charge-trapping in IGD is quite challenging. On the other hand, a very interesting finding from our simulation is that the opposite scenario assuming charge trapping in IGD can also provide identical ISPP/ISPE characteristic as the ideal FG device. This leads to a paradox (Rashomon) for a correct theoretical model for the device. In order to solve this paradox, we propose to apply a gate-sensing and channel-sensing (GSCS) technique to detect the charge location and dig out the real answer of operation principle. GSCS study of FG SONOS “Fusion” device shows that in a device that has both FG and trapping IGD the FG holds only limited amount of electrons and most electrons are stored in the IGD. Finally, the FG/CT fusion devices of the planar FG SONOS and FG BE-SONOS (without high-K and metal gate) are experimentally studied. They show very large memory window (>16V) with nearly ideal ISPP/ISPE slope ~1.","PeriodicalId":365759,"journal":{"name":"2016 IEEE 8th International Memory Workshop (IMW)","volume":"20 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2016-05-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2016 IEEE 8th International Memory Workshop (IMW)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IMW.2016.7495292","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

The planar flat FG device is theoretically studied extensively. There is a puzzle whether the charge is stored in the inter gate dielectric (IGD). A planar cell has no geometrical coupling ratio help thus IGD bears very high E-field. A high work function FG together with a robust interfacial layer between FG and high-K material that has both large barrier height and large dielectric constant are needed to reduce the out tunneling current. Thus our detailed tunneling simulation indicates that to obtain an “ideal planar FG” device with a large memory window but without charge-trapping in IGD is quite challenging. On the other hand, a very interesting finding from our simulation is that the opposite scenario assuming charge trapping in IGD can also provide identical ISPP/ISPE characteristic as the ideal FG device. This leads to a paradox (Rashomon) for a correct theoretical model for the device. In order to solve this paradox, we propose to apply a gate-sensing and channel-sensing (GSCS) technique to detect the charge location and dig out the real answer of operation principle. GSCS study of FG SONOS “Fusion” device shows that in a device that has both FG and trapping IGD the FG holds only limited amount of electrons and most electrons are stored in the IGD. Finally, the FG/CT fusion devices of the planar FG SONOS and FG BE-SONOS (without high-K and metal gate) are experimentally studied. They show very large memory window (>16V) with nearly ideal ISPP/ISPE slope ~1.
平面扁平浮栅NAND闪存器件的理论分析和浮栅/电荷俘获融合器件的实验研究,全面理解电荷存储和工作原理
对平面平面FG器件进行了广泛的理论研究。电荷是否存储在栅间电介质(IGD)中是一个难题。平面细胞没有几何耦合比的帮助,因此IGD承受很高的电场。为了减小输出隧穿电流,需要高功函数FG和具有大势垒高度和大介电常数的高k材料之间坚固的界面层。因此,我们详细的隧道模拟表明,在IGD中获得具有大存储窗口但没有电荷捕获的“理想平面FG”器件是相当具有挑战性的。另一方面,我们的模拟中一个非常有趣的发现是,假设IGD中的电荷捕获的相反情况也可以提供与理想FG器件相同的ISPP/ISPE特性。这导致了一个悖论(罗生门),一个正确的理论模型的设备。为了解决这一矛盾,我们提出采用栅极感应和通道感应(GSCS)技术来检测电荷位置,并找出其工作原理的真实答案。对FG - SONOS“Fusion”装置的GSCS研究表明,在同时具有FG和捕获IGD的装置中,FG仅保留有限数量的电子,大部分电子存储在IGD中。最后,对平面FG -SONOS和FG - BE-SONOS(无高k栅极和金属栅极)的FG/CT融合装置进行了实验研究。它们具有非常大的存储器窗口(>16V), ISPP/ISPE斜率接近理想值~1。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信