东南大学学报(英文版)
東南大學學報(英文版)
동남대학학보(영문판)
JOURNAL OF SOUTHEAST UNIVERSITY
2014年
1期
17-21
,共5页
黄婷婷%刘斯扬%孙伟锋%张春伟
黃婷婷%劉斯颺%孫偉鋒%張春偉
황정정%류사양%손위봉%장춘위
绝缘栅双极型晶体管%绝缘体上硅%热载流子效应%优化
絕緣柵雙極型晶體管%絕緣體上硅%熱載流子效應%優化
절연책쌍겁형정체관%절연체상규%열재류자효응%우화
lateral insulated gate bipolar transistor%LIGBT%silicon-on-insulator%SOI%hot-carrier effect%HCE%optimi-zation
提出了一种新型绝缘体上硅横向绝缘栅双极型晶体管(SOI-LIGBT),该晶体管在沟道下方的 P 型体区旁增加了一个特殊的低掺杂 P 型阱区,在不增加额外工艺的基础上减小了器件线性区电流的退化.分析了低掺杂 P 阱的宽度和深度对 SOI-LIGBT 器件热载流子可靠性的影响.通过增加低掺杂 P 型阱区的宽度,可以减小器件的纵向电场峰值和碰撞电离峰值,从而优化器件的热载流子效应.另外,增加低掺杂 P 型阱区的深度,也会减小器件内部的碰撞电离率,从而减弱器件的热载流子退化.结合低掺杂 P 型阱区的作用和工艺窗口大小的影响,确定低掺杂 P 型阱区的宽度和深度都为2μm.
提齣瞭一種新型絕緣體上硅橫嚮絕緣柵雙極型晶體管(SOI-LIGBT),該晶體管在溝道下方的 P 型體區徬增加瞭一箇特殊的低摻雜 P 型阱區,在不增加額外工藝的基礎上減小瞭器件線性區電流的退化.分析瞭低摻雜 P 阱的寬度和深度對 SOI-LIGBT 器件熱載流子可靠性的影響.通過增加低摻雜 P 型阱區的寬度,可以減小器件的縱嚮電場峰值和踫撞電離峰值,從而優化器件的熱載流子效應.另外,增加低摻雜 P 型阱區的深度,也會減小器件內部的踫撞電離率,從而減弱器件的熱載流子退化.結閤低摻雜 P 型阱區的作用和工藝窗口大小的影響,確定低摻雜 P 型阱區的寬度和深度都為2μm.
제출료일충신형절연체상규횡향절연책쌍겁형정체관(SOI-LIGBT),해정체관재구도하방적 P 형체구방증가료일개특수적저참잡 P 형정구,재불증가액외공예적기출상감소료기건선성구전류적퇴화.분석료저참잡 P 정적관도화심도대 SOI-LIGBT 기건열재류자가고성적영향.통과증가저참잡 P 형정구적관도,가이감소기건적종향전장봉치화팽당전리봉치,종이우화기건적열재류자효응.령외,증가저참잡 P 형정구적심도,야회감소기건내부적팽당전리솔,종이감약기건적열재류자퇴화.결합저참잡 P 형정구적작용화공예창구대소적영향,학정저참잡 P 형정구적관도화심도도위2μm.
A novel lateral insulated gate bipolar transistor on a silicon-on-insulator substrate SOI-LIGBT with a special low-doped P-well structure is proposed.The P-well structure is added to attach the P-body under the channel so as to reduce the linear anode current degradation without additional process.The influence of the length and depth of the P-well on the hot-carrier HC reliability of the SOI-LIGBT is studied.With the increase in the length of the P-well the perpendicular electric field peak and the impact ionization peak diminish resulting in the reduction of the hot-carrier degradation. In addition the impact ionization will be weakened with the increase in the depth of the P-well which also makes the hot-carrier degradation decrease.Considering the effect of the low-doped P-well and the process windows the length and depth of the P-well are both chosen as 2 μm.