CN109891562A - 化合物半导体器件 - Google Patents

化合物半导体器件 Download PDF

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CN109891562A
CN109891562A CN201680090265.2A CN201680090265A CN109891562A CN 109891562 A CN109891562 A CN 109891562A CN 201680090265 A CN201680090265 A CN 201680090265A CN 109891562 A CN109891562 A CN 109891562A
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electrode
semiconductor device
compound semiconductor
strong correlation
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CN109891562B (zh
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佐佐木肇
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Mitsubishi Electric Corp
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a 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
    • H01L29/76Unipolar devices, e.g. field effect transistors
    • H01L29/772Field effect transistors
    • H01L29/778Field effect transistors with two-dimensional charge carrier gas channel, e.g. HEMT ; with two-dimensional charge-carrier layer formed at a heterojunction interface
    • H01L29/7786Field effect transistors with two-dimensional charge carrier gas channel, e.g. HEMT ; with two-dimensional charge-carrier layer formed at a heterojunction interface with direct single heterostructure, i.e. with wide bandgap layer formed on top of active layer, e.g. direct single heterostructure MIS-like HEMT
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N99/00Subject matter not provided for in other groups of this subclass
    • H10N99/03Devices using Mott metal-insulator transition, e.g. field-effect transistor-like devices
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a 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
    • H01L29/12Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/20Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only AIIIBV compounds
    • H01L29/2003Nitride compounds
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    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/402Field plates
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/41Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
    • H01L29/417Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions carrying the current to be rectified, amplified or switched
    • H01L29/41725Source or drain electrodes for field effect devices
    • H01L29/41758Source or drain electrodes for field effect devices for lateral devices with structured layout for source or drain region, i.e. the source or drain region having cellular, interdigitated or ring structure or being curved or angular
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N70/00Solid-state devices having no potential barriers, and specially adapted for rectifying, amplifying, oscillating or switching
    • H10N70/20Multistable switching devices, e.g. memristors
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    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N70/00Solid-state devices having no potential barriers, and specially adapted for rectifying, amplifying, oscillating or switching
    • H10N70/801Constructional details of multistable switching devices
    • H10N70/821Device geometry
    • H10N70/826Device geometry adapted for essentially vertical current flow, e.g. sandwich or pillar type devices
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    • H10N70/00Solid-state devices having no potential barriers, and specially adapted for rectifying, amplifying, oscillating or switching
    • H10N70/801Constructional details of multistable switching devices
    • H10N70/881Switching materials
    • H10N70/883Oxides or nitrides
    • H10N70/8833Binary metal oxides, e.g. TaOx

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  • Engineering & Computer Science (AREA)
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  • Power Engineering (AREA)
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Abstract

在衬底(1)之上形成有半导体层(2、3)。在半导体层(3)之上形成有栅极电极(4)、源极电极(5)以及漏极电极(6)。在栅极电极(4)与源极电极(5)之间连接有强关联电子体系材料(12)。

Description

化合物半导体器件
技术领域
本发明涉及即使在暴露于高能粒子的严苛的环境下也难以破坏以及老化的化合物半导体器件。
背景技术
作为MES-FET或者HEMT等场效应晶体管而使用化合物半导体器件(例如,参照专利文献1~3)。有时器件暴露于严苛的环境下,高能粒子射入,穿过钝化膜、源极场板、器件的有源区域而到达衬底。此时,在高能粒子所穿过的轨迹周边产生大量的电子-空穴对,相应于材料的迁移率、复合速度、施加电压而扩散、复合。
专利文献1:日本特开2006-253654号公报
专利文献2:日本特开2010-67693号公报
专利文献3:日本特开2011-243632号公报
发明内容
向源极场板的漏极电极侧的端部与AlGaN沟道层之间施加高电场。因此,如果高能粒子射入而在钝化膜内产生大量的电子-空穴对,则在该部分形成导通路径而导致破坏。或者,存在以下这样的问题,即,在半导体内所产生的电子-空穴对的扩散、复合过程中半导体表面附近的空穴浓度上升,引起电位的上升或者空穴电流的增加,导致破坏,或者易于老化。同样地,向栅极电极的漏极电极侧的端部与AlGaN沟道层之间也施加高电场,存在易于破坏或者老化的问题。
另外,为了使高频特性提高,有时在栅极电极与源极电极之间连接SiN电容器。但是,由于SiN是绝缘体,因此无法将在半导体内产生的电子-空穴对的电荷经由SiN电容器而去除。
本发明就是为了解决上述这样的课题而提出的,其目的在于得到即使在暴露于高能粒子的严苛的环境下也难以破坏以及老化的化合物半导体器件。
本发明涉及的化合物半导体器件的特征在于,具备:衬底;半导体层,其形成于所述衬底之上;栅极电极、源极电极以及漏极电极,它们形成于所述半导体层之上;以及强关联电子体系材料,其连接在所述栅极电极与所述源极电极之间。
发明的效果
在本发明中,在器件内产生了电子-空穴对时,与栅极电极连接的强关联电子体系材料对器件内的电位变动进行感知,以短时间从绝缘体向导电体进行相变。在器件内产生的电子-空穴对穿过变化为导电性的强关联电子体系材料而流向接地,能够降低对器件的损伤。由此,本发明涉及的化合物半导体器件即使在暴露于高能粒子的严苛的环境下也难以破坏以及老化。
附图说明
图1是表示本发明的实施方式1涉及的化合物半导体器件的剖面图。
图2是表示本发明的实施方式1涉及的化合物半导体器件的俯视图。
图3是本发明的实施方式1涉及的化合物半导体器件的电路图。
图4是表示本发明的实施方式1涉及的强关联电子体系材料的剖面图。
图5是本发明的实施方式2涉及的化合物半导体器件的电路图。
具体实施方式
参照附图对本发明的实施方式涉及的化合物半导体器件进行说明。对相同或相应的结构要素标注相同的标号,有时省略重复说明。
实施方式1.
图1是表示本发明的实施方式1涉及的化合物半导体器件的剖面图。在SiC衬底1之上形成有GaN缓冲层2。在GaN缓冲层2之上形成有AlGaN沟道层3。在AlGaN沟道层3之上形成有栅极电极4、源极电极5以及漏极电极6。
第1钝化膜7覆盖栅极电极4以及AlGaN沟道层3。源极场板9形成于第1钝化膜7之上,从源极电极5延伸到栅极电极4与漏极电极6之间。源极场板9缓和栅极电极4与漏极电极6之间的电场,使得高电压动作成为可能,并且,降低寄生电容,由此改善高频特性。为了保护器件整体,第2钝化膜10覆盖第1钝化膜7以及源极场板9。
如果在向源极电极5与漏极电极6之间施加了电压,向栅极电极4施加了期望的偏置电压的状态下向栅极电极4输入高频,则二维电子气11内的电子高速地移动,作为从漏极电极6得到被放大的高频电力的放大器而动作。
图2是表示本发明的实施方式1涉及的化合物半导体器件的俯视图。图3是本发明的实施方式1涉及的化合物半导体器件的电路图。在栅极电极4与源极电极5之间连接有强关联电子体系材料12。源极电极5接地。
强关联电子体系材料12的代表例是VO2、SrTiO3、LaVO3、SrO等,报道了铜氧化物系、Fe系、Mn系、超导系等大量的示出强关联的材料。强关联电子体系材料12是在通常的状态下尽管充满电子,但由于电子彼此的关联过强,因此无法自由地移动,示出绝缘性的MOTT绝缘体。已知如果向强关联电子体系材料12施加电压、温度、光等刺激,则相变为导电性材料。由于强关联电子体系材料12能够通过PLD法等通常半导体工艺中使用的方法而形成、加工,因此易于与现有的半导体制造工艺结合。
高能粒子如果射入器件,则有时穿过第2钝化膜10、源极场板9、第1钝化膜7、AlGaN沟道层3、GaN缓冲层2而到达SiC衬底1。飞来的粒子是重粒子、质子、电子、中子、μ介子等,具有从1keV到100GeV左右的能量。在高能粒子所穿过的轨迹周边产生大量的电子-空穴对。在以往的构造中,在产生的电子-空穴对在器件内扩散、漂移、复合而逐步消灭的过程中给半导体带来大的损伤,发生破坏或者老化。
在本实施方式中,在器件内产生了电子-空穴对时,与栅极电极4连接的强关联电子体系材料12对器件内的电位变动进行感知,以短时间从绝缘体向导电体进行相变。在器件内产生的电子-空穴对穿过变化为导电性的强关联电子体系材料12而流向接地,能够降低对器件的损伤。由此,本实施方式涉及的化合物半导体器件即使在暴露于高能粒子的严苛的环境下也难以破坏以及老化。
图4是表示本发明的实施方式1涉及的强关联电子体系材料的剖面图。在SiC衬底1之上配置有基底电极13。基底电极13与栅极电极4连接。在基底电极13之上形成有强关联电子体系材料12的薄膜。在强关联电子体系材料12之上形成有上层电极14。上层电极14与源极电极5连接。如此,能够通过与电容器同样的简单的构造而将强关联电子体系材料12连接在源极电极5与漏极电极6之间。另外,通过将强关联电子体系材料12配置于SiC衬底1之上,能够实现器件的小型化。此外,也可以是在强关联电子体系材料12的两端分别连接源极电极5和漏极电极6的构造。
实施方式2.
图5是本发明的实施方式2涉及的化合物半导体器件的电路图。在本实施方式中,在实施方式1的结构的基础上,在源极电极5与漏极电极6之间连接有强关联电子体系材料15。由此,电荷逃逸路径增加,因而效果增强。此外,也可以省略源极侧的强关联电子体系材料12而仅设置漏极侧的强关联电子体系材料15,能够得到与实施方式1同样的效果。
标号的说明
1 SiC衬底,2 GaN缓冲层,3 AlGaN沟道层,4栅极电极,5源极电极,6漏极电极,12、15强关联电子体系材料,13基底电极,14上层电极。

Claims (4)

1.一种化合物半导体器件,其特征在于,具备:
衬底;
半导体层,其形成于所述衬底之上;
栅极电极、源极电极以及漏极电极,它们形成于所述半导体层之上;以及
强关联电子体系材料,其连接在所述栅极电极与所述源极电极之间。
2.一种化合物半导体器件,其特征在于,具备:
衬底;
半导体层,其形成于所述衬底之上;
栅极电极、源极电极以及漏极电极,它们形成于所述半导体层之上;以及
强关联电子体系材料,其连接在所述源极电极与所述漏极电极之间。
3.根据权利要求1或2所述的化合物半导体器件,其特征在于,
所述强关联电子体系材料配置于所述衬底之上。
4.根据权利要求1至3中任一项所述的化合物半导体器件,其特征在于,
所述强关联电子体系材料夹在基底电极与上层电极之间。
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