Influence of ultra-thin TiN thickness(1.4 nm and 2.4 nm) on positive bias temperature instability(PBTI)of high-k/metal gate nMOSFETs with gate-last process
The positive bias temperature instability(PBTI) degradations of high-k/metal gate(HK/MG) n MOSFETs with thin TiN capping layers(1.4 nm and 2.4 nm) are systemically investigated. In this paper, the trap energy distribution in gate stack during PBTI stress is extracted by using ramped recovery stress,...
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creator | 祁路伟 杨红 任尚清 徐烨峰 罗维春 徐昊 王艳蓉 唐波 王文武 闫江 朱慧珑 赵超 陈大鹏 叶甜春 |
description | The positive bias temperature instability(PBTI) degradations of high-k/metal gate(HK/MG) n MOSFETs with thin TiN capping layers(1.4 nm and 2.4 nm) are systemically investigated. In this paper, the trap energy distribution in gate stack during PBTI stress is extracted by using ramped recovery stress, and the temperature dependences of PBTI(90℃,125℃, 160℃) are studied and activation energy(Ea) values(0.13 eV and 0.15 eV) are extracted. Although the equivalent oxide thickness(EOT) values of two TiN thickness values are almost similar(0.85 nm and 0.87 nm), the 2.4-nm TiN one(thicker Ti N capping layer) shows better PBTI reliability(13.41% at 0.9 V, 90℃, 1000 s). This is due to the better interfacial layer/high-k(IL/HK) interface, and HK bulk states exhibited through extracting activation energy and trap energy distribution in the high-k layer. |
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In this paper, the trap energy distribution in gate stack during PBTI stress is extracted by using ramped recovery stress, and the temperature dependences of PBTI(90℃,125℃, 160℃) are studied and activation energy(Ea) values(0.13 eV and 0.15 eV) are extracted. Although the equivalent oxide thickness(EOT) values of two TiN thickness values are almost similar(0.85 nm and 0.87 nm), the 2.4-nm TiN one(thicker Ti N capping layer) shows better PBTI reliability(13.41% at 0.9 V, 90℃, 1000 s). This is due to the better interfacial layer/high-k(IL/HK) interface, and HK bulk states exhibited through extracting activation energy and trap energy distribution in the high-k layer.</description><identifier>ISSN: 1674-1056</identifier><identifier>EISSN: 2058-3834</identifier><language>eng</language><subject>不稳定性 ; 偏压 ; 工艺 ; 栅极 ; 温度 ; 等效氧化层厚度 ; 超薄 ; 锡层厚度</subject><ispartof>中国物理B:英文版, 2015 (12), p.499-502</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://image.cqvip.com/vip1000/qk/85823A/85823A.jpg</thumbnail><link.rule.ids>314,776,780,4010</link.rule.ids></links><search><creatorcontrib>祁路伟 杨红 任尚清 徐烨峰 罗维春 徐昊 王艳蓉 唐波 王文武 闫江 朱慧珑 赵超 陈大鹏 叶甜春</creatorcontrib><title>Influence of ultra-thin TiN thickness(1.4 nm and 2.4 nm) on positive bias temperature instability(PBTI)of high-k/metal gate nMOSFETs with gate-last process</title><title>中国物理B:英文版</title><addtitle>Chinese Physics</addtitle><description>The positive bias temperature instability(PBTI) degradations of high-k/metal gate(HK/MG) n MOSFETs with thin TiN capping layers(1.4 nm and 2.4 nm) are systemically investigated. In this paper, the trap energy distribution in gate stack during PBTI stress is extracted by using ramped recovery stress, and the temperature dependences of PBTI(90℃,125℃, 160℃) are studied and activation energy(Ea) values(0.13 eV and 0.15 eV) are extracted. Although the equivalent oxide thickness(EOT) values of two TiN thickness values are almost similar(0.85 nm and 0.87 nm), the 2.4-nm TiN one(thicker Ti N capping layer) shows better PBTI reliability(13.41% at 0.9 V, 90℃, 1000 s). This is due to the better interfacial layer/high-k(IL/HK) interface, and HK bulk states exhibited through extracting activation energy and trap energy distribution in the high-k layer.</description><subject>不稳定性</subject><subject>偏压</subject><subject>工艺</subject><subject>栅极</subject><subject>温度</subject><subject>等效氧化层厚度</subject><subject>超薄</subject><subject>锡层厚度</subject><issn>1674-1056</issn><issn>2058-3834</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqNjUtOwzAURS0EEqFlD0_MDfm6GYNAdMBHIvPKDU7yqPMS7BdQdwDrYBvdU7eAVbEARvfq6h6dIxGlcVHKrMzyYxElapHLJC7UqTjz_i2OVRKnWSR-ltTYyVBtYGhgsuy05A4JKnyEUOoNGe_3u6_kMgfqQdMrpIe6333DQDAOHhk_DKxRe2DTj8ZpnpwBJM96jRZ5G_jn62oZkCDpsO3k5qo3rC20mg3Qw9PL3W3l4RO5O0zSas8wuqEO9rk4abT15vwvZ-IivG_uZd0N1L4jtavRYa_ddqWUWpRFqYrsX6dfYMtg9A</recordid><startdate>2015</startdate><enddate>2015</enddate><creator>祁路伟 杨红 任尚清 徐烨峰 罗维春 徐昊 王艳蓉 唐波 王文武 闫江 朱慧珑 赵超 陈大鹏 叶甜春</creator><scope>2RA</scope><scope>92L</scope><scope>CQIGP</scope><scope>~WA</scope></search><sort><creationdate>2015</creationdate><title>Influence of ultra-thin TiN thickness(1.4 nm and 2.4 nm) on positive bias temperature instability(PBTI)of high-k/metal gate nMOSFETs with gate-last process</title><author>祁路伟 杨红 任尚清 徐烨峰 罗维春 徐昊 王艳蓉 唐波 王文武 闫江 朱慧珑 赵超 陈大鹏 叶甜春</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-chongqing_primary_6667858653</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>不稳定性</topic><topic>偏压</topic><topic>工艺</topic><topic>栅极</topic><topic>温度</topic><topic>等效氧化层厚度</topic><topic>超薄</topic><topic>锡层厚度</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>祁路伟 杨红 任尚清 徐烨峰 罗维春 徐昊 王艳蓉 唐波 王文武 闫江 朱慧珑 赵超 陈大鹏 叶甜春</creatorcontrib><collection>中文科技期刊数据库</collection><collection>中文科技期刊数据库-CALIS站点</collection><collection>中文科技期刊数据库-7.0平台</collection><collection>中文科技期刊数据库- 镜像站点</collection><jtitle>中国物理B:英文版</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>祁路伟 杨红 任尚清 徐烨峰 罗维春 徐昊 王艳蓉 唐波 王文武 闫江 朱慧珑 赵超 陈大鹏 叶甜春</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Influence of ultra-thin TiN thickness(1.4 nm and 2.4 nm) on positive bias temperature instability(PBTI)of high-k/metal gate nMOSFETs with gate-last process</atitle><jtitle>中国物理B:英文版</jtitle><addtitle>Chinese Physics</addtitle><date>2015</date><risdate>2015</risdate><issue>12</issue><spage>499</spage><epage>502</epage><pages>499-502</pages><issn>1674-1056</issn><eissn>2058-3834</eissn><abstract>The positive bias temperature instability(PBTI) degradations of high-k/metal gate(HK/MG) n MOSFETs with thin TiN capping layers(1.4 nm and 2.4 nm) are systemically investigated. In this paper, the trap energy distribution in gate stack during PBTI stress is extracted by using ramped recovery stress, and the temperature dependences of PBTI(90℃,125℃, 160℃) are studied and activation energy(Ea) values(0.13 eV and 0.15 eV) are extracted. Although the equivalent oxide thickness(EOT) values of two TiN thickness values are almost similar(0.85 nm and 0.87 nm), the 2.4-nm TiN one(thicker Ti N capping layer) shows better PBTI reliability(13.41% at 0.9 V, 90℃, 1000 s). This is due to the better interfacial layer/high-k(IL/HK) interface, and HK bulk states exhibited through extracting activation energy and trap energy distribution in the high-k layer.</abstract></addata></record> |
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subjects | 不稳定性 偏压 工艺 栅极 温度 等效氧化层厚度 超薄 锡层厚度 |
title | Influence of ultra-thin TiN thickness(1.4 nm and 2.4 nm) on positive bias temperature instability(PBTI)of high-k/metal gate nMOSFETs with gate-last process |
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