CN111211167B - 一种消除负阻效应的rc-igbt器件结构 - Google Patents

一种消除负阻效应的rc-igbt器件结构 Download PDF

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CN111211167B
CN111211167B CN202010023986.XA CN202010023986A CN111211167B CN 111211167 B CN111211167 B CN 111211167B CN 202010023986 A CN202010023986 A CN 202010023986A CN 111211167 B CN111211167 B CN 111211167B
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igbt device
collector region
negative resistance
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CN111211167A (zh
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王颖
张孝冬
于成浩
曹菲
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Hangzhou Dianzi University
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
    • H01L29/70Bipolar devices
    • H01L29/72Transistor-type devices, i.e. able to continuously respond to applied control signals
    • H01L29/739Transistor-type devices, i.e. able to continuously respond to applied control signals controlled by field-effect, e.g. bipolar static induction transistors [BSIT]
    • H01L29/7393Insulated gate bipolar mode transistors, i.e. IGBT; IGT; COMFET
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/06Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
    • H01L29/0603Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/06Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
    • H01L29/0684Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by the shape, relative sizes or dispositions of the semiconductor regions or junctions between the regions
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/66007Multistep manufacturing processes
    • H01L29/66075Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials
    • H01L29/66227Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials the devices being controllable only by the electric current supplied or the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched, e.g. three-terminal devices
    • H01L29/66234Bipolar junction transistors [BJT]
    • H01L29/66325Bipolar junction transistors [BJT] controlled by field-effect, e.g. insulated gate bipolar transistors [IGBT]

Abstract

本发明提供了一种消除负阻效应的RC‑IGBT器件。该RC‑IGBT器件与传统器件相比,在N型集电区和P型集电区上方有混合交替排列的N型和P+型缓冲层,且最靠近N型集电区的P+柱边缘超过N型缓冲层。由于上述混合交替排列N型和P型的缓冲层对场截止区的多区段的隔离作用,电子或空穴需要爬过多个P型区域,增长了载流子运动路径,从而增大了RC‑IGBT器件在导通初期N型集电区上方电势差,使得该PN结更容易开启,器件更容易从单极导通转换为双极导通,进而抑制了RC‑IGBT器件在导通初期所产生的Snapback效应。

Description

一种消除负阻效应的RC-IGBT器件结构
技术领域
本发明涉及半导体技术领域,具体而言,涉及一种消除负阻效应的RC-IGBT器件结构。
背景技术
绝缘栅双极型晶体管(IGBT),是一种集成了MOS(绝缘栅型场效应晶体管)控制和双极导通BJT(双极型晶体管)组成的功率半导体器件,相比传统VDMOS器件,IGBT具有电导调制作用,是一种双极器件。具有MOSFET的输入阻抗高、控制功率小、驱动电路简单、开关速度高、开关损耗小的优点,同时具有双极功率晶体管的电流密度大、饱和压降低、电流处理能力强的优点。
电力电子系统中,IGBT通常需要与反向并联的快恢复二极管(Fast RecoveryDiode,简称为FRD)配合使用。因此将FRD与IGBT单片地集成在一起的逆导型IGBT(ReverseConductive IGBT)近年来得到了国内外的广泛关注。由于单片集成的IGBT和FRD共用同一个结终端,因此RC-IGBT大大提高了硅片的利用率,降低了成本,并且避免了互连引线等的寄生效应,提高了器件的可靠性。相对传统IGBT器件,RC-IGBT在成本和性能上的巨大优势,使得该器件具备了巨大的发展潜力。在关断瞬态期间,RC-IGBT的N型集电区为漂移区残留的载流子提供了一条快速抽走的通道,因此可以大大减少关断时间。然而,传统RC-IGBT在正向导通初期,器件由单极导通向双极导通转换过程中,会存在一个负阻区,称作Snapback现象,严重时导致器件无法开启,对器件可靠性及性能造成危害。
发明内容
本发明的主要目的在于提供一种消除负阻效应的RC-IGBT器件结构,以解决现有技术中的RC-IGBT在正向导通初期产生的snapback现象,从而对器件可靠性及性能造成危害的问题。
本发明一种消除负阻效应的RC-IGBT器件结构,传统的RC-IGBT器件通过离子注入在N型衬底背面形成一定厚度的N-buffer层,N-buffer层的宽度小于N-漂移区的宽度;一定厚度的N-buffer层通过离子注入形成P+柱,进而形成一个N-buffer层内部下沿带有多个P+柱的混合交替排列N型和P型的缓冲层;N型集电区和P型集电区被空隙分隔开,所述的N型集电区上方的P+柱不与P型集电区接触;N-buffer层中最靠近N型集电区一侧的P+柱边缘超出N-buffer层。
作为优选,所述的P+柱数量为三个。
作为优选,所述的离子注入一定厚度的N-buffer层的掺杂浓度为1×1016cm-3,厚度为6μm。
作为优选,所述的离子注入一定厚度的N-buffer层的N型集电区上方的开口宽度为1.2μm。
作为优选,所述的离子注入一定厚度的混合P+/N-buffer层的P+型掺杂浓度为1×1017cm-3,厚度为5μm。
本发明的有益效果在于:由于上述混合交替排列N型和P型的缓冲层对场截止区的多区段的隔离作用,载流子需要爬过多个P型区域,增长了载流子运动路径,从而增大了RC-IGBT器件在导通初期N型集电区上方电势差,使得该PN结更容易开启,器件更容易从单极导通转换为双极导通,进而抑制了RC-IGBT器件在导通初期所产生的Snapback效应。
附图说明
图1示出了传统RC-IGBT结构示意图;
图2示出了基于本发明设计的RC-IGBT半元胞结构示意图;
图3~6示出了图2所示结构中背面结构的制作流程示意图;
图7示出了图1所示结构的IV曲线图;
图8示出了图2所示结构的IV曲线图。
具体实施方式
为使本发明的目的、技术方案和优点更加清楚,以下结合附图对本发明进行具体阐述。
传统RC-IGBT结构如图1所示,本发明提出的RC-IGBT半元胞结构如图2所示,与传统RC-IGBT相比,本发明提出的RC-IGBT不同之处在于在N-型漂移区的内底部引入了混合P+/N-buffer层,如图3~6所示,其背面结构具体制作步骤如下:
1.选用1200V RC-IGBT器件,单个mos元胞宽度为10μm,半集电极宽度为10μm,厚度为130μm;漂移区浓度为5.0×1013cm-3,栅氧化层厚度为0.05μm;
2.通过离子注入在N-漂移区底部形成宽度为8.5μm、厚度为10μm、掺杂浓度为1.0×1016cm-3的N-缓冲层。
3.通过离子注入在N-缓冲层内部底部制作3个P+柱区,纵向注入结深为5μm,横向注入宽度1μm,掺杂浓度为1.0×1017cm-3,其中最接近N-漂移区的P+柱边缘超出N-buffer层。
4.继续分别离子注入形成N+集电区和P+集电区,并刻蚀N+集电区和P+集电区交接处,形成空隙隔离,使N+型集电区上方的P+柱不与P+型集电区接触。
根据图7所示仿真结果可以得出,当mos元胞宽度为10μm、半集电极宽度为320μm时,图1结构的传统RC-IGBT表现出明显的snapback现象。
根据图8所示仿真结果可以得出,当mos元胞宽度为10μm、半集电极宽度为10μm时,图2结构的RC-IGBT没有snapback现象。
显然,本领域的技术人员可以对本发明进行各种改动和变形而不脱离本发明的精神和范围。应注意到的是,以上所述仅为本发明的具体实施例,并不限制本发明,凡在本发明的精神和原则之内,所做的调制和优化,皆应属本发明权利要求的涵盖范围。

Claims (7)

1.一种消除负阻效应的RC-IGBT器件结构,其特征在于,RC-IGBT器件通过离子注入在N型衬底背面形成一定厚度的N-buffer层,N-buffer层的宽度小于N-漂移区的宽度,一定厚度的N-buffer层通过离子注入形成P+柱,进而形成一个N-buffer层内部下沿带有多个P+柱的混合交替排列N型和P型的缓冲层;N型集电区和P型集电区被空隙分隔开,所述的N型集电区上方的P+柱不与P型集电区接触;N-buffer层中最靠近N型集电区一侧的P+柱边缘超出N-buffer层。
2.根据权利要求1所述的一种消除负阻效应的RC-IGBT器件结构,其特征在于:所述的P+柱数量为三个。
3.根据权利要求1所述的一种消除负阻效应的RC-IGBT器件结构,其特征在于:所述的离子注入一定厚度的N-buffer层的掺杂浓度为1×1016cm-3
4.根据权利要求1所述的一种消除负阻效应的RC-IGBT器件结构,其特征在于:N-buffer层中最靠近N型集电区一侧的P+柱边缘与N型集电区外侧边缘的距离为1.2μm。
5.根据权利要求1所述的一种消除负阻效应的RC-IGBT器件结构,其特征在于:所述的离子注入一定厚度的N-buffer层的厚度为6μm。
6.根据权利要求1所述的一种消除负阻效应的RC-IGBT器件结构,其特征在于:所述的离子注入一定厚度的混合P+柱/N-buffer层的P+型掺杂浓度为1×1017cm-3
7.根据权利要求1所述的一种消除负阻效应的RC-IGBT器件结构,其特征在于:所述的离子注入一定厚度的混合P+柱/N-buffer层的P+型厚度为5μm。
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