CN114122128A - 高电子迁移率晶体管 - Google Patents
高电子迁移率晶体管 Download PDFInfo
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- CN114122128A CN114122128A CN202111392945.9A CN202111392945A CN114122128A CN 114122128 A CN114122128 A CN 114122128A CN 202111392945 A CN202111392945 A CN 202111392945A CN 114122128 A CN114122128 A CN 114122128A
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Abstract
提供拥有漏极场板(140)的高电子迁移率晶体管。漏极场板(140)形成在高电子迁移率晶体管的栅极(118)与漏极(104)之间的区域内。漏极场板(140)包含具有投影区域大于漏极垫(104)的金属垫。漏极场板(140)与设置在漏极场板之下的半导体层(102)形成金属‑半导体(M‑S)肖特基结构。M‑S肖特基结构的电容在半导体区域(102)产生电容,提高高电子迁移率晶体管的晶体管构件的击穿电压。可移除在有源区(203)下的衬底(100)部分,从而提高高电子迁移率晶体管的晶体管构件的热传导性及降低结温度。
Description
本申请是申请号为201780042843.X,申请日为2017年05月08日,发明名称为“高电子迁移率晶体管”的专利申请的分案申请。
技术领域
本发明是有关于半导体装置,特别是有关于高电子迁移率晶体管。
背景技术
高电子迁移率晶体管(High Electron Mobility Transistor,HEMT),也被称为异质结构FET(HFET)或调制掺杂FET(MODFET),是一种在其中形成信道层与电子亲和力小于信道层的阻挡层之间的异质结的场效应晶体管(FET)。HEMT能够在比常规晶体管高的频率,上至毫米波频率操作,且通常使用在高频及高功率产品,例如移动电话站的功率放大器及军用相控阵激光器。
通常,在射频(RF)范围操作的HEMT需要高于常规晶体管的击穿电压,所述击穿电压是晶体管的栅极可处理的最大电压。现有的HEMT中,已使用连接源极的栅极场板提高击穿电压。然而,随着现代移动通信科技的出现,对具有较高击穿电压的HEMT的需求持续增加。而且,为了得到好的线性度,栅极-漏极电容(Cgd)值需要在动态驱动范围内保持平坦。
此外,设计在高功率范围操作的HEMT可能会产生高热能。因此,它们需要被设计用于低输出电阻,以便其可传递大电流至其负载,及良好的结绝缘以抵撑高电压。因为大部分的热能在异质结产生,结的面积可做得尽可能的大,以便热能可被非常快的耗散从而防止过热。然而,在许多高功率应用中,HEMT的尺寸外型可能会加诸限制在装置面积的尺寸上,造成HEMT可处理的最大功率的限制。
因此,存在对于具有高击穿电压、在动态驱动范围内平坦的Cgd值、及加强的热耗散机制的HEMT的需求,从而提高在各种应用,尤其在射频范围的最大电压、线性度、及额定功率。
发明内容
在实施例中,漏极场板形成在HEMT的漏极上。漏极场板包含具有投影面积比漏极垫大的金属垫。漏极场板降低栅极侧的漏极垫产生的电场强度,使HEMT的击穿电压的增加。
在实施例中,漏极场板通过沉积SiN钝化层、图形化SiN钝化层、及沉积金属层在图形化SiN钝化层上而形成。漏极场板及下方的半导体层形成在半导体内产生耗尽层的金属-半导体(M-S)肖特基结,耗尽层提高HEMT的击穿电压。而且,通过改变漏极场板的形状,可控制栅极-漏极电容(Cgd)及漏极-源极电容(Cds),增强HEMT的RF特性。
在实施例中,设计HEMT以减少体漏电流及结温度(Tj)。在前侧的加工完成后,(即在衬底的前侧形成晶体管构件),可加工衬底的背侧以加强热耗散。在实施例中,背侧加工包含数个步骤。首先,移除(蚀刻)有源区下的衬底的部分。之后,可将SiN层沉积在整个背侧表面上,其中SiN层的厚度较佳为接近35nm。下一步,形成穿过源极下AlGaN/GaN外延层的贯通孔。由Ti/Au制成的第一金属层可通过像是溅镀的适合的工序沉积在背侧表面上,且具有像是Cu/Au、Cu/Au/Cu/Au、或Cu/Ag/Au复合结构的第二金属层可形成在第一金属层之上,使得衬底的背侧及在前侧上的源极通过贯通孔电连接。
在实施例中,背侧加工可在金属层沉积在有源区下之前移除有源区下的衬底。由于典型的衬底材料,像是Si或蓝宝石,具有比金属层低的热传导率,背侧加工可提高HEMT的热传导率,降低晶体管构件的Tj。在实施例中,背侧加工可在沉积SiN层之前移除有源区下的衬底。由于典型的衬底材料具有比SiN低的电绝缘性,背侧加工可提高电绝缘性,降低晶体管构件的体漏电流。
在实施例中,每个HEMT可从晶圆切块(即执行切割工序)及附接于封装,而无常规的共晶附接的预成形,其减少至少一个制造步骤并因此降低制造成本。在实施例中,表面安装装置(SMD)回流法可用于将裸晶附接至封装。
通常,常规的裸晶黏合工序会遭遇空气空隙问题,空气空隙降低热传导率且负面地影响晶体管的可靠度。在实施例中,焊膏沉积在背侧以填充贯通孔及衬底的凹部区域,避免在裸晶黏合工序期间形成空气空隙。
附图说明
将参考本发明实施例,它们的示例可在附图中示出。这些附图旨在说明而非限制。尽管本发明主要在这些实施例的背景中描述,但应理解,并不意图将本发明的范围限制于这些具体实施例。
图1至图5显示根据本发明实施例在衬底的前侧上形成半导体构件的例示性工序。
图6显示根据本发明实施例沉积钝化层的例示性工序。
图7显示根据本发明实施例形成接触开口的例示性工序。
图8显示根据本发明实施例形成栅极场板及漏极场板的例示性工序。
图9显示根据本发明实施例的漏极场板的俯视图。
图10显示根据本发明实施例的漏极场板的俯视图。
图11显示根据本发明实施例镀覆金属层在晶体管构件上的例示性工序。
图12及图13显示根据本发明实施例沉积电绝缘层及蚀刻电绝缘层的部分的例示性工序。
图14显示根据本发明实施例的晶圆薄化的例示性工序。
图15显示根据本发明实施例的衬底蚀刻的例示性工序。
图16显示根据本发明实施例沉积SiN层的例示性工序。
图17显示根据本发明实施例产生贯通孔的例示性工序。
图18显示根据本发明实施例沉积金属层在晶圆的背侧表面上的例示性工序。
图19显示根据本发明实施例沉积金属层在晶圆的背侧表面上的例示性工序。
图20显示根据本发明实施例施予焊膏至晶圆的背侧表面的例示性工序。
图21显示根据本发明实施例加工HEMT晶圆的背侧的例示性工序。
图22显示根据本发明实施例沉积金属层在晶圆的背侧表面上的例示性工序。
图23显示根据本发明实施例沉积金属层在晶圆的背侧表面上的例示性工序。
图24显示根据本发明实施例施予焊膏至晶圆的背侧表面的例示性工序。
具体实施方式
在以下描述中,出于解释的目的,阐述了具体细节以便提供对本公开的理解。然而,对于本领域技术人员显而易见的是,本公开可在没有这些细节的情况下实践。此外,本领域技术人员将意识到,以下描述本公开的实施例可以各种方式,诸如有形计算器可读取媒介上的工序、设备、系统、装置或方法实现。
本领域技术人员将意识到:(1)某些步骤可选择性地执行,(2)步骤可不限于本文所载的具体顺序,以及(3)某些步骤可以不同的顺序进行,包括同时进行。
图中所示的组件/构件是本公开的示例性实施例的说明,并且旨在避免模糊本公开。本说明书中提及的“一个实施例”、“较佳的实施例”、“一实施例”或“实施例”意味着结合实施例描述的具体特征、结构、特性或功能包括在本公开的至少一个实施例中,且可包含在多于一个实施例中。在本说明书中各处出现的短语“在一个实施例中”,“在一实施例中”或“在实施例中”不一定都指代相同的一或多个实施例。用语“包括”、“包括”、“包含”和“包含”应被理解为开放用语,且该些用语后的任何列表是示例,并不意味着限于所列项目。本文使用的任何标题仅用于组织目的,且不应用于限制说明书或权利要求书的范围。此外,在本说明书中的各个地方使用某些用语仅用于说明而不应被解释为限制。
本公开的实施例包含漏极场板以提高HEMT的击穿电压。而且,漏极场板可用来提高或降低HEMT的Cgd及/或Cds、维持平坦的Cgd值、增强HEMT的RF特性。
本公开的实施例包含移除有源区下的衬底的部分的工序,从而提高HEMT构件的热传导率及降低结温度。
本公开的实施例包含移除有源区下的衬底的部分及沉积SiN层的工序。由于SiN层具有比衬底材料更佳的电绝缘特性,此工序可降低HEMT构件的体漏电流。
本公开的实施例包含移除有源区下的衬底的部分及沉积金属层的工序。由于金属层具有比衬底材料更佳的热传导率,此工序可提高HEMT构件的热传导率及降低结温度。
本公开的实施例包含移除有源区下的衬底的部分及形成贯通孔,其中金属层沉积在所述贯通孔中的工序。此工序可降低HEMT的源电感。
本公开的实施例包含移除有源区下的衬底的部分、沉积金属层、及施予焊膏至晶圆的背表面的工序,避免空气空隙的形成,从而增强HEMT构件的热传导特性及降低HEMT构件的结温度。
本公开的实施例包含移除有源区下的衬底的部分、沉积金属层、及施予焊膏至晶圆的背表面的工序。此工序可省去附接HEMT裸晶至封装的常规预成形工序(像是共晶附接工序),其可降低制造成本。
本公开的实施例包含移除有源区下的衬底的部分、沉积金属层、及施予焊膏至晶圆的背表面的工序。因此,可使用共晶附接工序或SMD回流工序来将HEMT裸晶附接至封装。
图1至图5显示根据本发明实施例形成HEMT构件在衬底的前(或上)侧的例示性工序。如图1描述,外延层102形成在衬底100的前(上)侧。衬底100可较佳地由硅或蓝宝石形成,尽管如此,衬底可用其他适合的材料。外延层102可由GaN形成,使得AlGaN/GaN异质结层形成在衬底上。应注意外延层102可由其他适合类型的材料形成。下文中,使用GaN HEMT作为例示性HEMT,尽管如此,其可通过本文件描述的工序制造他类型的HEMT。
漏极(或者,等效地,漏极垫或漏极电极或漏极的奥姆金属化)104及108与源极(或者,等效地,源极垫或源极电极或用于源极的奥姆金属化)106可形成在外延层102之上,其中漏极及源极可由适合的金属形成。在实施例中,漏极及源极可各具有包含Ti/Al/Ni/Au的复合金属层结构。漏极及源极的奥姆接触可通过合金化漏极及源极产生,从而降低在漏极/源极及外延层102之间接口的电阻。
如图2所示,电绝缘层110可形成在衬底100的前表面之上。在实施例中,绝缘层110可由SiN,或可用于电绝缘的任何其他适合的材料制成。绝缘层110可覆盖外延层102、漏极104及108及源极106的这些器件的制造期间形成在外延层102、漏极104及108及源极106的上表面上的损伤。如之后描述,SiN层可被图形化以形成栅极。
图3显示离子布植工序以产生离子布植部分(或者,简短地,布植部分)112,布植部分112可隔绝漏极104及108及源极106作为HEMT的独立工作单元。在实施例中,图形化光致抗蚀剂层(未显示在图3中)可通过适合的光刻工序涂布在HEMT的上表面之上,并用作为光致抗蚀剂(PR)掩模层以选择性地允许离子,像是氮离子或氧离子,在布植工序期间通过绝缘层110且被布植在外延层102之内。接着,随后移除光致抗蚀剂层。
如图4描述,绝缘层110的一或多个部分通过适合的蚀刻工序蚀刻。在实施例中,图形化掩模层(未显示在图4内)可通过光刻工序形成在绝缘层110之上,并用以移除绝缘层的部分,从而形成凹陷116且曝露外延层的上表面。
图5显示形成在凹陷116内,且具有延伸至绝缘层110上的翼的T形栅极118。在实施例中,可执行T形栅极光刻工序(未描述在图5内)且随后使用像是Ni/Au或Ni/Pt/Au的适合的金属执行栅极金属化。
如图6所述,钝化层120可沉积在HEMT的前表面上。在实施例中,钝化层120可由SiN形成,尽管如此,钝化层120可使用其他适合的电绝缘材料。钝化层120可提高T形栅极118及漏极/源极之间的击穿电压层,从而增强HEMT的可靠度。T形栅极118的翼及绝缘层110可产生降低在漏极侧上的栅极边缘区域的电场的电容,从而提高栅极118的击穿电压。
图7显示根据本发明实施例制作接触开口的例示性工序。如所述,移除绝缘层110的部分及钝化层120以形成接触开口(或凹陷)130、132及134,以及SiN接触开口(或凹陷)131及135。如下所述,SiN接触开口131及135可以金属填充以形成漏极场金属(或者,等效的漏极场板)。在实施例中,基于光刻工序的蚀刻工序可用来移除绝缘层110及钝化层120的部分,从而曝露外延层102的上表面的部分。
图8显示根据本发明实施例形成连接源极的栅极场效金属(或者,等效地,连接源极的栅极场板)144及漏极场板140的例示性工序。图9显示根据本发明实施例的漏极场板140的俯视图。连接源极的栅极场板(或者,简短地栅极场板)144,形成在钝化层120上,钝化层在T形栅极118上且向漏极104延伸,与底下的层110及120产生电容,其中此电容降低在漏极侧上的栅极边缘区域的电场,从而提高栅极118及漏极104之间的击穿电压。在实施例中,连接源极的栅极场板144可由适合的金属形成。
在实施例中,漏极场板140可形成在漏极104上并且延伸超过漏极104的边缘。漏极场板140具有与连接源极的栅极场板144相似的效应,其中通过漏极场板140产生的电容可提高击穿电压。更具体的说,漏极场板140;层110、120;及外延层102形成金属-半导体(M-S)结构。M-S肖特基结构产生电容,电容又在外延层102内产生耗尽区域,从而提高击穿电压。
通常,当RF信号被施加至栅极118,即静态电流具有波动的瞬态周期时,栅极118及漏极104之间的边缘电容(Cgd)在漏极-源极静态电流上具有负效应。在实施例中,通过漏极场板140的M-S肖特基结构产生电容可控制边缘电容(Cgd),从而可维持Cgd的平坦性。
如图9所述,在实施例中,漏极场板140指的是覆盖漏极104的投影区域及进一步在X方向延伸至漏极104的投影区域外的金属区域。(下文中,用语投影区域指的是通过将三维物体的形状投影至x-y平面上而获得的二维区域,其中x-y平面平行外延层102的上表面。)漏极场板140也指覆盖SiN接触开口131的投影区域的金属区域及进一步在x及y两方向延伸至SiN接触开口131的投影区域外的金属区域。相反地,在常规的系统中,漏极接触开口130填充金属材料,且漏极接触开口130的投影区域不延伸至漏极104的投影区域外。
在实施例中,为SiN接触开口131的边缘及漏极场板140的边缘之间在y方向的距离的长度D1为约1μm。为漏极场板140的边缘及漏极104的边缘之间在y方向的距离的长度D2为约1μm。为SiN接触开口131在x方向的尺寸的宽度D3为约1μm。为SiN接触开口131的边缘及漏极104的边缘之间在x方向的距离的宽度D4为约1μm。为SiN接触开口131的边缘及漏极场板140的边缘之间在x方向的距离的宽度D5为约1μm。为SiN接触开口131的边缘及漏极场板140的边缘之间在x方向的距离的宽度D6为约3μm。为接触开口区域130的边缘及漏极104的边缘之间在x方向的距离的宽度D7为约5μm。应注意的是长度D1至D7的值为例示性且可以使用其他适合的值。
在实施例中,即使在漏极104的尺寸改变时,仍可维持长度D1至D7之间的比值。例如,在漏极104的尺寸改变时,D6及D7之间的比值可维持为1。
漏极场板140可由多重金属层结构形成,像是Ti/Au或Ti/Au/Ti/Au。在实施例中,连接源极的栅极场板144及漏极场板140可在相同工序期间形成,例如,图形化掩模层(未显示在图8及图9内)可通过适合的光刻工序沉积,使得在沉积连接源极的栅极场板140极漏极场板140的同时,接触开口区域130、132及134也可在相同工序期间以相同金属材料填充。
图10显示根据本发明的另一个实施例的漏极场板的俯视图。
如所述,漏极场板150包含三个板401、402、及403,其中板401及403与板402电性分离且板402电连接至漏极104。板402包含填充接触开口区域130的金属层,而板401及403包含分别填充二个SiN接触开口131的金属层。
在实施例中,宽度D10、D11、及D12与图9中的D5、D3、及D4相似,其各皆为约1μm。同样地,分别地与D2及D1相似的长度D13及D14,各约为1μm。
如图10所述,漏极场板401、402及403的侧面可为交指形。例如,与交指部分的突起/凹陷部分相关长度D15至D17及D19至D23,可各为约1μm。为漏极104的边缘及接触孔区域130的边缘之间在x方向的距离的长度D18可为约5μm。
在实施例中,漏极场板140、401、402及403可具有其他适合的形状,使得M-S肖特基结构可具有预期的电容以控制Cgd及/或Cgs(栅极与源极之间的边缘电容)。在实施例中,漏极场板的形状及漏极场板与漏极104的边缘之间的距离可被调整以达到预期的电容。在实施例中,指叉式电容对DC信号是断路,但是对RF信号是电短路,其导致指叉式电容响应于RF信号选择性的操作。应注意的是漏极场板142及SiN接触开口135的俯视图具有与图9及图10相同的配置,即漏极场板142可具有与漏极场板140相同的形状或漏极场板142可具有与金属板401、402、及403相似的三个金属板。
图11显示根据本发明实施例镀覆金属层在晶体管构件上的例示性工序。如所述,金属组件160、162、及164可通过镀覆工序沉积在漏极及源极之上,像是Au镀覆工序,使得构件可通过气桥或接合垫工序电连接。
图12及图13显示根据本发明实施例沉积电绝缘层166及蚀刻绝缘层166的部分的例示性工序。如所述,绝缘层166被部分蚀刻使得金属组件(接合垫)160、162及164分别具有接触开口170、172及174以连接引线至其。例如,在实施例中,引线的一端可被接合(引线接合)至接触孔170,使得电信号经由金属组件(接合垫)160及漏极场板140从引线传输至漏极104或从漏极104传输至引线。
图14至图24说明加工衬底100及外延层102的背侧(底侧)。图14显示根据本发明实施例的晶圆薄化的例示性工序。如所述,衬底100可通过适合的工序薄化,像是研磨及抛光,以便于HEMT的组装至封装及背侧工序,像是贯通孔的产生及切割。
图15显示根据本发明实施例的衬底蚀刻的例示性工序。如所述,有源区203下的衬底100的部分可通过适合的工序移除,像是干式蚀刻或湿式蚀刻。此处,有源区203指的是在工作期间产生热的主动半导体构件,像是漏极、栅极及源极的下方区域。然后,如图16所示,电绝缘层204,像是SiN层,可沉积在衬底的背侧(或底侧)表面上。
图17显示根据本发明实施例产生贯通孔206的例示性工序。如所述,在实施例中,贯通孔206可延伸至源极106的底侧。如所述,绝缘层204及外延层102可通过适合的蚀刻工序蚀刻以形成贯通孔206,其中贯通孔206可为槽孔。
图18显示根据本发明实施例沉积金属层206在衬底的背侧表面上的例示性工序。在实施例中,溅镀工序可用来沉积例如由Ti/Au形成的金属层,于衬底的背侧表面上,尽管如此,可使用其他适合的工序来沉积金属层206。
图19显示根据本发明实施例电镀金属层208在衬底的背侧表面上的例示性工序。在实施例中,金属层206可为金属层208的晶种层。在实施例中,金属层208可通过适合的工序沉积,像是电镀工序,且金属层208可具有复合金属结构,像是Cu/Au/Cu/Au及Cu/Ag/Au。
图20显示根据本发明实施例施予焊膏208至衬底的背侧表面的例示性工序。如所述,焊膏208可填充至贯通孔206中以及在有源区203下的衬底100的凹陷部分。
如上所述,有源区203下的衬底的部分可在金属层206及208沉积之前移除。由于衬底材料,像是硅或蓝宝石,可具有比金属层206及208低的热传导率,图15至图20中的工序可提高HEMT的热传导率,降低有源区203中晶体管构件的Tj。同样地,由于典型的衬底材料具有比SiN低的电绝缘性,背侧工序提高电绝缘性,降低晶体管构件的体漏电流。
图21显示根据本发明实施例的HEMT晶圆的背侧加工。图21中HEMT与图17中的HEMT相似,差异在于图21中的HEMT为具有彼此可通过气桥(未表示在图21中)连接的多重源极310、314及318。例如,在实施例中,贯通孔302及304可用于电连接源极310及318至HEMT的底侧,其中贯通孔302及304可位于有源区309外。如所述,绝缘层(像是SiN层)301、衬底300、外延层305及离子布植区307可通过适合的工序蚀刻以形成贯通孔302及304。
应注意在图21只显示三个源极。然而,对所属技术领域具有通常知识者来说显而易见的是,其他适合的数量的源极可通过气桥彼此连接。而且,在图21只显示二个标准贯通孔,尽管如此,可形成其他适合数量的贯通孔。
图22显示根据本发明实施例沉积金属层330在衬底的背侧表面上的例示性工序。在实施例中,溅镀工序可用来沉积例如由Ti/Au形成的金属层在衬底的背侧表面上。
图23显示根据本发明实施例沉积金属层332在衬底的背侧表面上的例示性工序。在实施例中,金属层330可为金属层332的晶种层。在实施例中,金属层332可通过适合的工序沉积,像是电镀工序,且金属层332可具有复合金属结构,像是Cu/Au/Cu/Au及Cu/Ag/Au。
图24显示根据本发明实施例用于施予焊膏334至晶圆的背侧表面的例示性工序。如所述,焊膏334可填充在贯通孔302及304中以及有源区309下的衬底300的凹陷部分。
本公开的实施例包含移除(蚀刻)有源区203或309下的衬底100或300的部分及沉积一或多个金属层的工序。由于金属层具有较典型衬底材料更佳的热传导率,这些工序可提高操作期间HEMT构件产生的热耗散。
本公开的实施例包含移除(蚀刻)有源区下的衬底的部分、沉积金属层、及施予焊膏220或334至背侧表面的工序,避免空气空隙的形成,从而增强HEMT构件的热传导特性及降低HEMT构件的结温度。
本公开的实施例包含移除(蚀刻)有源区下的衬底的部分及沉积SiN层204或301的工序。由于SiN层具有较典型衬底材料更佳的电绝缘特性,此工序可降低HEMT构件的体漏电流。
在实施例中,在图20及图24中的每个HEMT可从晶圆切块(切割)及通过加热(即回流)焊膏220或332附接至封装(未显示在图20及图24中)。相反的,在常规方法中,包含共晶金属的焊膏在裸晶被附接之前被施予在陶瓷封装或引线框上。因此,在实施例中,不需要常规共晶金属的预成形,减少至少一个制造工序及制造成本。在实施例中,表面安装装置(SMD)回流法可用于将HEMT附接至封装。
结合图1至图24描述的一或多个工序可通过计算器软件执行。应注意的是,本公开的实施例可进一步涉及其上具有用于执行各种计算器实施操作的计算器编码的非瞬时、有形的计算器可读取媒介的计算器产品。媒介及计算器编码可为那些为了本公开的目的而特别设计及建构的,或可为所属技术领域具有通常知识者习知或可得的种类。有形计算器可读取媒介的例子包含,但不限于:磁媒介,像是硬盘、软盘、及磁带;光学媒介,像是CD-ROM及全息装置;磁光媒介,及特别配置以存储或存储及执行程序编码的硬件装置,像是专用集成电路(ASICs)、可编程逻辑设备(PLDs)、闪存装置、及ROM与RAM装置。计算器编码的例子包含像是通过编译程序产生的机械编码及包含通过使用编译程序的计算器来执行的更高阶编码的文件。本公开的实施例可整个或部分作为可在通过加工装置执行的程序模块中的机械执行指令实施。程序模块的例子包含库、编码指令、程序、对象、构件、及数据结构。在分布式计算环境中,程序模块可物理性地位于本机、远程或者两者的设定中。
所属技术领域具有通常知识者应理解的是,没有计算系统或程序语言为本公开的实践的关键。所属技术领域具有通常知识者也应理解的是,以上描述的组件数量可物理性地及/或功能性地分离成子模块或结合在一起。
所属技术领域具有通常知识者将理解的是,前述例子和实施例是例示性的,并不限制本公开的范围。意图将经由阅读说明书和研究附图而对所属技术领域具有通常知识者是显而易见的对其所有的排列、增强、等效、组合和改进都包括在本公开的真实精神和范围内。
Claims (9)
1.一种半导体晶体管,其特征在于,包含:
外延层;
多个晶体管构件,形成在所述外延层的上表面上;
衬底,形成在所述外延层的底表面上,且设置在所述多个晶体管构件的部分下的区域外的区域上;
绝缘层,由电绝缘材料形成,且设置在所述衬底的底表面上以及在所述外延层的底表面的部分上;
至少一个贯通孔,从所述绝缘层的底表面经过所述外延层延伸至所述多个晶体管构件的至少一个的底表面,以及
至少一个金属层,形成在所述绝缘层的底表面、所述至少一个贯通孔的侧壁、及在所述多个晶体管构件的所述至少一个的所述底表面上;
焊膏,施予在所述至少一个金属层的底表面。
2.根据权利要求1所述的半导体晶体管,其特征在于,所述至少一个金属层包含:
第一金属层,形成在所述衬底的所述底表面、所述至少一个贯通孔的所述侧壁、及所述多个晶体管构件的所述至少一个的所述底表面上;以及
第二金属层,形成在所述第一金属层的底表面上。
3.根据权利要求1所述的半导体晶体管,其特征在于,所述半导体晶体管是高电子迁移率晶体管。
4.根据权利要求1所述的半导体晶体管,其特征在于,所述多个晶体管构件的所述至少一个包含源极。
5.根据权利要求1所述的半导体晶体管,其特征在于,所述多个晶体管构件的所述至少一个包含二个或更多的源极,其中所述至少一个贯通孔包含二个或更多的贯通孔,且所述二个或更多的贯通孔的每一个延伸到所述二个或更多的源极中的对应一个的所述底表面。
6.一种半导体晶体管,其特征在于,包含:
外延层;
多个晶体管构件,形成在所述外延层的上表面上;
衬底,形成在所述外延层的底表面上,且设置在所述多个晶体管构件的部分下的区域外的区域上;
绝缘层,由电绝缘材料形成,且设置在所述衬底的底表面上以及在所述外延层的底表面的部分上;
至少一个贯通孔,从所述绝缘层的底表面经过所述外延层延伸至所述多个晶体管构件的至少一个的底表面,
第一金属层,形成在所述衬底的所述底表面、所述至少一个贯通孔的所述侧壁、及所述多个晶体管构件的所述至少一个的所述底表面上;以及
第二金属层,形成在所述第一金属层的底表面上。
7.根据权利要求6所述的半导体晶体管,其特征在于,所述半导体晶体管是高电子迁移率晶体管。
8.根据权利要求6所述的半导体晶体管,其特征在于,所述多个晶体管构件的所述至少一个包含源极。
9.根据权利要求6所述的半导体晶体管,其特征在于,所述多个晶体管构件的所述至少一个包含二个或更多的源极,其中所述至少一个贯通孔包含二个或更多的贯通孔,且所述二个或更多的贯通孔的每一个延伸到所述二个或更多的源极中的对应一个的所述底表面。
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CN109716530A (zh) | 2019-05-03 |
KR102199173B1 (ko) | 2021-01-07 |
EP3455883A2 (en) | 2019-03-20 |
US10707311B2 (en) | 2020-07-07 |
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JP6718982B2 (ja) | 2020-07-08 |
JP2020150280A (ja) | 2020-09-17 |
KR102136356B1 (ko) | 2020-07-23 |
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US10861947B2 (en) | 2020-12-08 |
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