CN111834450B - 一种集成齐纳二极管的soi ligbt器件 - Google Patents
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Abstract
本发明属于功率半导体技术领域,具体涉及一种集成齐纳二极管的SOI LIGBT器件。本发明相对于传统的LIGBT,新器件在发射极端的P阱区中引入一个齐纳二极管,其P型区域和器件发射极电气相连,其N型区域与P阱区通过浮空欧姆金属实现电气相连。当集电极电压不断增加,齐纳二极管会发生反向击穿导通,从而使得P阱区的电势被箝位;这不仅有利降低器件栅电容,导通时可以降低饱和电流以提高器件短路能力,关断时过程中可提供空穴抽取通路以降低关断时间和关断损耗。相对于传统LIGBT结构,本发明提供的LIGBT新结构获得更优的导通压降与关断损耗之间的折中关系,并提升器件抗短路能力。
Description
技术领域
本发明属于功率半导体技术领域,具体涉及一种内部集成齐纳二极管的槽栅SOILIGBT。
背景技术
SOI基的横向绝缘栅双极型晶体管(Lateral Insulated Gate BipolarTransistor,LIGBT)是双极型器件的典型代表。由于其高输入阻抗、低导通压降、高耐压特性、介质隔离等特点,广泛应用于各种电力电子系统,成为中高压开关应用领域的关键半导体器件。
LIGBT器件在正向导通时,漂移区内发生电导调制效应而具有较小的导通压降,但同时关断时需要将漂移区中存储的大量载流子抽出,导致器件具有较大关断损耗。而降低器件导通压降的措施常常使器件有大的饱和电流,从而导致较差的短路安全工作区(Shortcircuit safe operating area,SCSOA)。因此,LIGBT的导通压降、关断损耗以及安全工作区之间存在折中关系。另外,发射极端浮空P阱区结构可以增强LIGBT载流子存储效应,但在开启过程中,浮空P区中积累的空穴引起的位移电流对栅电容充电,严重影响器件的开启特性。
发明内容
针对上述问题,本发明提出一种集成齐纳二极管的SOI LIGBT器件,在发射极端浮空P阱中引入齐纳二极管实现箝位作用,从而改善器件的性能。
本发明的技术方案是:一种集成齐纳二极管的SOI LIGBT器件,包括自下而上依次层叠设置的P衬底层1、介质埋层2和N型漂移区3;所述N型漂移区3上层两端分别具有发射极结构和集电极结构;
所述发射极结构包括P型阱区4、P型重掺杂区5及N型重掺杂区6,所述P型重掺杂区5和所述N型重掺杂区6交替排列于所述P型阱区4的上层,且外侧靠近集电极结构的是N型重掺杂区6,P型重掺杂区5的结深大于N型重掺杂区6的结深;所述P型重掺杂区5和N型重掺杂区6上表面的共同引出端为发射极;
所述集电极结构包括N型缓冲区13和P型集电区14;所述P型集电区14位于N型缓冲区13上层中部;所述P型集电区14上表面的引出端为集电极;
其特征在于,在P型阱区4上层,还具有槽栅结构和齐纳二极管;
所述槽栅结构包括控制槽栅结构和阻挡槽栅结构;所述控制槽栅结构由第一槽栅介质层71和位于第一槽栅介质层71中的第一多晶硅72组成,所述控制槽栅结构沿器件垂直方向依次贯穿N型重掺杂区6和P型阱区4后延伸至所述N型漂移区3中;所述阻挡槽栅结构由第二槽栅介质层81和位于第二槽栅介质层81中的第二多晶硅82组成,所述阻挡槽栅结构沿器件垂直方向贯穿所述P型阱区4延伸至所述N型漂移区3中,所述阻挡槽栅结构的一侧与最外侧的N型重掺杂区6接触,且控制槽栅结构和阻挡槽栅结构之间间隔有P型重掺杂区5;所述控制槽栅多晶硅72和所述阻挡槽栅多晶硅82的共同引出端为栅电极;阻挡槽栅结构的另一侧与齐纳二极管接触;
所述齐纳二极管结构包括P型区域9和N型区域10,所述P型区域9位于N型区域10上层一侧,且P型区域9与阻挡槽栅结构接触;所述P型阱区4与所述N型区域10通过导电材料11电气连接,所述P型区域9的引出端与发射极相连;在齐纳二极管与集电极结构之间的N型漂移区3上表面,还具有场氧层12,且场氧层12还沿P型阱区4和N型缓冲区13的上表面向两侧延伸。
进一步的所述的N型漂移区3上层还具有P型埋层15,所述P型埋层15与所述P型阱区4接触。
进一步的,所述器件采用的半导体材料为Si、SiC、SiGe、GaAs或GaN中的一种。
本发明的有益效果为,相对于传统LIGBT结构,本发明导通时改善了导通压降与关断损耗间的折中关系。齐纳二极管的引入降低了器件的密勒电容,提高了器件的开关速度。另外,还降低了饱和电流,提高了短路能力,扩大了安全工作区。
附图说明
图1为实施例1的结构示意图;
图2为实施例2的结构示意图;
具体实施方式
下面结合附图和实施例,详细描述本发明的技术方案:
实施例1
如图1所示,本例的具有集成齐纳二极管的槽栅SOI LIGBT与传统器件结构相比,在P阱区4中靠近N型漂移区3一侧集成有齐纳二极管。
本例的工作原理为:
在正向导通时,发射极端阻挡槽栅和控制槽栅起到物理阻挡作用,有利于提高漂移区载流子浓度,同时控制槽栅两侧及阻挡槽栅靠近发射极一侧均有沟道存在,可增大器件沟道密度以降低沟道区电阻,综合作用下器件Von可显著降低。随着阳极电压上升,齐纳二极管发生击穿,使得P阱区4处的电势被箝位,从而降低了密勒电容;同时齐纳二极管的击穿电流迅速增大,提供了空穴通路,使器件的饱和电流降低,从而提高器件的安全工作区。
器件关断过程中,随着阳极电压上升,齐纳二极管反向击穿导通,可以帮助抽取空穴以加快器件关断,从而降低关断损耗。
正向阻断状态下,齐纳二极管发生击穿使P阱区4的电势被箝位,可以保护槽栅电场,避免拐角处提前击穿,提高器件耐压。
实施例2
如图2所示,本例与实施例1中图1的区别在于,本例中N型漂移区3上表面引入一个P型埋层15,与P型阱区4侧面接触。本实施例中器件工作机理和实施例1区别在于:引入的P型埋层15与N型漂移区3之间相互耗尽,形成类似超结(Super junction,SJ)结构。在正向阻断状态时,本例中引入的P型埋层15可与耗尽N型漂移区3相互耗尽,从而优化器件的耐压。同时,器件关断时,P型埋层15和N型漂移区3相互抽取空穴和电子,可加速器件的耗尽,从而进一步降低关断时间,减小关断损耗。
Claims (2)
1.一种集成齐纳二极管的SOI LIGBT器件,包括自下而上依次层叠设置的P衬底层(1)、介质埋层(2)和N型漂移区(3);所述N型漂移区(3)上层两端分别具有发射极结构和集电极结构;
所述发射极结构包括P型阱区(4)、P型重掺杂区(5)及N型重掺杂区(6),所述P型重掺杂区(5)和所述N型重掺杂区(6)交替排列于所述P型阱区(4)的上层,且P型阱区(4)最外侧靠近集电极结构的是N型重掺杂区(6),P型重掺杂区(5)的结深大于N型重掺杂区(6)的结深;所述P型重掺杂区(5)和N型重掺杂区(6)上表面的共同引出端为发射极;
所述集电极结构包括N型缓冲区(13)和P型集电区(14);所述P型集电区(14)位于N型缓冲区(13)上层中部;所述P型集电区(14)上表面的引出端为集电极;
其特征在于,在P型阱区(4)上层,还具有槽栅结构和齐纳二极管;
所述槽栅结构包括控制槽栅结构和阻挡槽栅结构;所述控制槽栅结构由第一槽栅介质层(71)和位于第一槽栅介质层(71)中的第一多晶硅(72)组成,所述控制槽栅结构沿器件垂直方向依次贯穿N型重掺杂区(6)和P型阱区(4)后延伸至所述N型漂移区(3)中;所述阻挡槽栅结构由第二槽栅介质层(81)和位于第二槽栅介质层(81)中的第二多晶硅(82)组成,所述阻挡槽栅结构沿器件垂直方向贯穿所述P型阱区(4)延伸至所述N型漂移区(3)中,所述阻挡槽栅结构的一侧与最外侧的N型重掺杂区(6)接触,且控制槽栅结构和阻挡槽栅结构之间间隔有P型重掺杂区(5);所述控制槽栅多晶硅(72)和所述阻挡槽栅多晶硅(82)的共同引出端为栅电极;阻挡槽栅结构的另一侧与齐纳二极管接触;
所述齐纳二极管包括P型区域(9)和N型区域(10),所述P型区域(9)位于N型区域(10)上层一侧,且P型区域(9)与阻挡槽栅结构接触;所述P型阱区(4)与所述N型区域(10)通过导电材料(11)电气连接,所述P型区域(9)的引出端与发射极相连;在齐纳二极管与集电极结构之间的N型漂移区(3)上表面,还具有场氧层(12),且场氧层(12)还沿P型阱区(4)和N型缓冲区(13)的上表面向两侧延伸。
2.根据权利要求1所述的一种集成齐纳二极管的SOI LIGBT器件,其特征在于,所述的N型漂移区(3)上层还具有P型埋层(15),所述P型埋层(15)与所述P型阱区(4)接触。
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