{"title":"NAND 闪存中保持瞬态建模的综合表征方法","authors":"Wen-Chien Liu;Yung-Yueh Chiu;Toshiaki Takeshita;Riichiro Shirota","doi":"10.1109/TED.2024.3442984","DOIUrl":null,"url":null,"abstract":"A comprehensive characterization method and a physically based model for profiling the evolution of the trapped oxide charge (\n<inline-formula> <tex-math>${Q}_{T}\\text {)}$ </tex-math></inline-formula>\n during data retention (high-temperature baking after program/erase (P/E) cycling) was developed. This method involves monitoring the transients of threshold-voltage (\n<inline-formula> <tex-math>${V}_{\\text {th}}\\text {)}$ </tex-math></inline-formula>\n shift and transconductance (\n<inline-formula> <tex-math>${G}_{m}\\text {)}$ </tex-math></inline-formula>\n recovery simultaneously. It is observed that the scatter relation between \n<inline-formula> <tex-math>${G}_{m}$ </tex-math></inline-formula>\n recovery and the corresponding \n<inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula>\n reduction for different baking temperatures can be effectively merged over a universal curve. This curve consists of two stages. In the first stage of retention, \n<inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula>\n decreases but \n<inline-formula> <tex-math>${G}_{m}$ </tex-math></inline-formula>\n remains almost constant. In the subsequent stage, \n<inline-formula> <tex-math>${G}_{m}$ </tex-math></inline-formula>\n increases in proportion to the decrease in \n<inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula>\n. To describe this characteristic, two different \n<inline-formula> <tex-math>${Q}_{T}$ </tex-math></inline-formula>\n distribution regions were indispensably introduced; one is a near-interfacial (NI) region close to the Si surface and the other is a bulk oxide (BO) region. During retention, \n<inline-formula> <tex-math>${Q}_{T}$ </tex-math></inline-formula>\n in the NI region tunnels out, and simultaneously \n<inline-formula> <tex-math>${Q}_{T}$ </tex-math></inline-formula>\n in the BO region supplements it via transport mechanisms. The transition point between the first and second stages occurs when all the \n<inline-formula> <tex-math>${Q}_{T}$ </tex-math></inline-formula>\n in the BO region dissipated. Results show good agreement between measured and simulated retention transients.","PeriodicalId":13092,"journal":{"name":"IEEE Transactions on Electron Devices","volume":null,"pages":null},"PeriodicalIF":2.9000,"publicationDate":"2024-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Comprehensive Characterization Method for Modeling Retention Transients in NAND Flash Memory\",\"authors\":\"Wen-Chien Liu;Yung-Yueh Chiu;Toshiaki Takeshita;Riichiro Shirota\",\"doi\":\"10.1109/TED.2024.3442984\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A comprehensive characterization method and a physically based model for profiling the evolution of the trapped oxide charge (\\n<inline-formula> <tex-math>${Q}_{T}\\\\text {)}$ </tex-math></inline-formula>\\n during data retention (high-temperature baking after program/erase (P/E) cycling) was developed. This method involves monitoring the transients of threshold-voltage (\\n<inline-formula> <tex-math>${V}_{\\\\text {th}}\\\\text {)}$ </tex-math></inline-formula>\\n shift and transconductance (\\n<inline-formula> <tex-math>${G}_{m}\\\\text {)}$ </tex-math></inline-formula>\\n recovery simultaneously. It is observed that the scatter relation between \\n<inline-formula> <tex-math>${G}_{m}$ </tex-math></inline-formula>\\n recovery and the corresponding \\n<inline-formula> <tex-math>${V}_{\\\\text {th}}$ </tex-math></inline-formula>\\n reduction for different baking temperatures can be effectively merged over a universal curve. This curve consists of two stages. In the first stage of retention, \\n<inline-formula> <tex-math>${V}_{\\\\text {th}}$ </tex-math></inline-formula>\\n decreases but \\n<inline-formula> <tex-math>${G}_{m}$ </tex-math></inline-formula>\\n remains almost constant. In the subsequent stage, \\n<inline-formula> <tex-math>${G}_{m}$ </tex-math></inline-formula>\\n increases in proportion to the decrease in \\n<inline-formula> <tex-math>${V}_{\\\\text {th}}$ </tex-math></inline-formula>\\n. To describe this characteristic, two different \\n<inline-formula> <tex-math>${Q}_{T}$ </tex-math></inline-formula>\\n distribution regions were indispensably introduced; one is a near-interfacial (NI) region close to the Si surface and the other is a bulk oxide (BO) region. During retention, \\n<inline-formula> <tex-math>${Q}_{T}$ </tex-math></inline-formula>\\n in the NI region tunnels out, and simultaneously \\n<inline-formula> <tex-math>${Q}_{T}$ </tex-math></inline-formula>\\n in the BO region supplements it via transport mechanisms. The transition point between the first and second stages occurs when all the \\n<inline-formula> <tex-math>${Q}_{T}$ </tex-math></inline-formula>\\n in the BO region dissipated. Results show good agreement between measured and simulated retention transients.\",\"PeriodicalId\":13092,\"journal\":{\"name\":\"IEEE Transactions on Electron Devices\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":2.9000,\"publicationDate\":\"2024-08-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE Transactions on Electron Devices\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://ieeexplore.ieee.org/document/10643495/\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Transactions on Electron Devices","FirstCategoryId":"5","ListUrlMain":"https://ieeexplore.ieee.org/document/10643495/","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
Comprehensive Characterization Method for Modeling Retention Transients in NAND Flash Memory
A comprehensive characterization method and a physically based model for profiling the evolution of the trapped oxide charge (
${Q}_{T}\text {)}$
during data retention (high-temperature baking after program/erase (P/E) cycling) was developed. This method involves monitoring the transients of threshold-voltage (
${V}_{\text {th}}\text {)}$
shift and transconductance (
${G}_{m}\text {)}$
recovery simultaneously. It is observed that the scatter relation between
${G}_{m}$
recovery and the corresponding
${V}_{\text {th}}$
reduction for different baking temperatures can be effectively merged over a universal curve. This curve consists of two stages. In the first stage of retention,
${V}_{\text {th}}$
decreases but
${G}_{m}$
remains almost constant. In the subsequent stage,
${G}_{m}$
increases in proportion to the decrease in
${V}_{\text {th}}$
. To describe this characteristic, two different
${Q}_{T}$
distribution regions were indispensably introduced; one is a near-interfacial (NI) region close to the Si surface and the other is a bulk oxide (BO) region. During retention,
${Q}_{T}$
in the NI region tunnels out, and simultaneously
${Q}_{T}$
in the BO region supplements it via transport mechanisms. The transition point between the first and second stages occurs when all the
${Q}_{T}$
in the BO region dissipated. Results show good agreement between measured and simulated retention transients.
期刊介绍:
IEEE Transactions on Electron Devices publishes original and significant contributions relating to the theory, modeling, design, performance and reliability of electron and ion integrated circuit devices and interconnects, involving insulators, metals, organic materials, micro-plasmas, semiconductors, quantum-effect structures, vacuum devices, and emerging materials with applications in bioelectronics, biomedical electronics, computation, communications, displays, microelectromechanics, imaging, micro-actuators, nanoelectronics, optoelectronics, photovoltaics, power ICs and micro-sensors. Tutorial and review papers on these subjects are also published and occasional special issues appear to present a collection of papers which treat particular areas in more depth and breadth.