CN203456468U - Insulated gate bipolar transistor - Google Patents
Insulated gate bipolar transistor Download PDFInfo
- Publication number
- CN203456468U CN203456468U CN201320220862.6U CN201320220862U CN203456468U CN 203456468 U CN203456468 U CN 203456468U CN 201320220862 U CN201320220862 U CN 201320220862U CN 203456468 U CN203456468 U CN 203456468U
- Authority
- CN
- China
- Prior art keywords
- region
- insulated gate
- gate bipolar
- source region
- bipolar transistor
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 239000004065 semiconductor Substances 0.000 claims abstract description 22
- BUGBHKTXTAQXES-UHFFFAOYSA-N Selenium Chemical compound [Se] BUGBHKTXTAQXES-UHFFFAOYSA-N 0.000 claims description 4
- 230000004888 barrier function Effects 0.000 claims description 4
- 229910052711 selenium Inorganic materials 0.000 claims description 4
- 239000011669 selenium Substances 0.000 claims description 4
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 claims description 3
- 238000009413 insulation Methods 0.000 claims 3
- NINIDFKCEFEMDL-UHFFFAOYSA-N Sulfur Chemical group [S] NINIDFKCEFEMDL-UHFFFAOYSA-N 0.000 claims 1
- 230000000694 effects Effects 0.000 abstract description 4
- 239000010410 layer Substances 0.000 description 21
- 239000000463 material Substances 0.000 description 4
- 125000003748 selenium group Chemical group *[Se]* 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 230000003071 parasitic effect Effects 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- 238000000137 annealing Methods 0.000 description 2
- 230000000903 blocking effect Effects 0.000 description 2
- 230000005669 field effect Effects 0.000 description 2
- 238000002513 implantation Methods 0.000 description 2
- 238000005468 ion implantation Methods 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 125000004434 sulfur atom Chemical group 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 210000000746 body region Anatomy 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 238000006731 degradation reaction Methods 0.000 description 1
- 239000007943 implant Substances 0.000 description 1
- 239000011229 interlayer Substances 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 238000013021 overheating Methods 0.000 description 1
- 230000003647 oxidation Effects 0.000 description 1
- 238000007254 oxidation reaction Methods 0.000 description 1
- 230000002035 prolonged effect Effects 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 229910052717 sulfur Inorganic materials 0.000 description 1
- 239000011593 sulfur Substances 0.000 description 1
- -1 sulfur ions Chemical class 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Images
Landscapes
- Electrodes Of Semiconductors (AREA)
Abstract
Description
技术领域technical field
本实用新型涉及一种半导体器件,更具体地,涉及一种绝缘栅双极型晶体管。The utility model relates to a semiconductor device, in particular to an insulated gate bipolar transistor.
背景技术Background technique
绝缘栅双极型晶体管(IGBT:Insulated Gate Bipolar Transistor)是由金属氧化物半导体场效应晶体管(MOSFET:Metal-Oxide-SemiconductorField-Effect Transistor)和双极型晶体管(BJT:Bipolar Junction Transistor)复合而成的半导体器件,其兼具这两种器件的优点,既具有MOSFET的驱动功率小和开关速度快的优点,又具有BJT的饱和压降低且电流承载容量大的优点。因此,近年来IGBT已经广泛应用于诸如交流电机、变频器、开关电源、照明电路、牵引传动等需要进行电力转换的领域。Insulated Gate Bipolar Transistor (IGBT: Insulated Gate Bipolar Transistor) is a combination of Metal-Oxide-Semiconductor Field-Effect Transistor (MOSFET: Metal-Oxide-Semiconductor Field-Effect Transistor) and Bipolar Transistor (BJT: Bipolar Junction Transistor) The semiconductor device has the advantages of these two devices. It not only has the advantages of small driving power and fast switching speed of MOSFET, but also has the advantages of low saturation voltage drop and large current carrying capacity of BJT. Therefore, in recent years, IGBTs have been widely used in fields requiring power conversion such as AC motors, frequency converters, switching power supplies, lighting circuits, and traction drives.
图1示出了现有的IGBT的一个实例。如图1所示,IGBT100被示出为具有沟槽栅场终止型结构,其包括顺次层叠的p型集电区11、n型场终止区12、n-型漂移区13、p型基区14以及n+型源区15,以及形成在n-型漂移区13、p型基区14以及n+型源区15中的栅极16和栅氧化层17。FIG. 1 shows an example of a conventional IGBT. As shown in FIG. 1 , the IGBT100 is shown to have a trench gate field stop structure, which includes a p-
进一步地,在图1所示的IGBT100中,栅极16包括具有均匀截面宽度的上部栅极161以及截面宽度大于上部栅极161的截面宽度的下部栅极162。这种结构可被称为局部窄台(PNM:Partially Narrow Mesa)结构。在Masakiyo Sumitomo等人发表于2012年第24届国际功率半导体器件与功率集成电路会议(ISPSD:International Symposium on PowerSemiconductor Devices and IC)的论文“Low Loss IGBT with PartiallyNarrow Mesa Structure(PNM-IGBT)”以及美国专利第US7800187B2号中记载了具有类似结构的IGBT。通过形成如图1中虚线框所示的局部窄台结构(两个相邻沟槽栅之间的基区被窄化),能够在确保不减小金属-半导体接触面积的情况下减小台面宽度(两个相邻沟槽栅之间的基区的宽度),从而IGBT100的饱和电压显著降低,并且通态电压和关断损耗之间也能获得良好权衡。Further, in the IGBT 100 shown in FIG. 1 , the
然而,在图1所示的IGBT100中,台面区域变窄使得该区域中的电流密度增加。在IGBT100关断过渡期间,该区域中的大部分或者几乎所有的电流由空穴运载,高空穴电流密度要流向下一个P接触区,导致电流在流过p型基区14的位于n+型源区15之下的部分时产生横向电压降(lateral voltage drop)。该电压降使得IGBT100的寄生晶闸管(具有由p型集电区11、n型场终止区12/n-型漂移区13、p型基区14以及n+型源区15构成的PNPN结构)中的NPN管被导通,这特别是在过电流截止(over-current-turn-off)时更容易发生。结果,IGBT100发生闩锁(Latchup)效应,其中的等效MOSFET的控制能力降低甚至无效,IGBT100最终将因过热而损坏。However, in the IGBT 100 shown in FIG. 1 , the narrowing of the mesa region increases the current density in this region. During the turn-off transition of the IGBT100, most or almost all of the current in this region is carried by holes, and the high hole current density will flow to the next P contact region, causing the current to flow through the p-
对于局部窄台结构的IGBT可能出现如上所述的闩锁现象,不仅如此,对于通常的IGBT也可能出现闩锁现象。The above-mentioned latch-up phenomenon may occur for an IGBT with a local narrow mesa structure, not only that, but also for a normal IGBT.
第二个问题是:在PNM-IGBT中,通常实现了沟槽的高密度。因此,PNM-IGBT每个区域都具有大的沟道宽度和高的沟道导电率。这意味着在短路操作时,极高的电流密度流过器件,并伴随有高的集电极-发射极电压。这将导致器件在几个微秒内损坏。The second problem is: In PNM-IGBT, a high density of trenches is usually achieved. Therefore, each region of the PNM-IGBT has a large channel width and high channel conductivity. This means that during short-circuit operation, extremely high current densities flow through the device, accompanied by high collector-emitter voltages. This will cause the device to fail within a few microseconds.
第三个问题是:台面结构的末端将会有拐角(corner)或者沟槽(trench)的以某种方式弄圆的结构。由于几何原因(如果栅极围绕该拐角将会更明显(effective),由于沟道区域不同的掺杂等级(在氧化期间硼分离到栅极氧化物中,或在不同的晶面(crystallographic plane)平面中高温退火是不同的),或者由于栅极氧化物不同的性能,例如厚度或界面电荷(这些也取决于各个晶面),在该区域(台面末端区域),MOS沟道阈值电压将不同于(通常低于)台面的长侧处的电压。这会导致在台面末端更高的电流密度或者甚至长期退化和阈值电压的不稳定。The third problem is that the ends of the mesa structures will have corners or trenches that are rounded in some way. Due to geometrical reasons (it would be more effective if the gate was around the corner), due to different doping levels of the channel region (boron segregates into the gate oxide during oxidation, or on a different crystallographic plane) High temperature annealing is different in the plane), or due to different properties of the gate oxide, such as thickness or interface charge (these also depend on the individual crystal planes), in this region (mesa end region), the MOS channel threshold voltage will be different Higher (usually lower) voltages at the long sides of the mesa. This can lead to higher current densities or even long-term degradation and instability of the threshold voltage at the end of the mesa.
PNM-IGBT在US6521538B2以及US7800187B2中进行了描述。然而,现有技术中还没有提出对于上述技术问题的解决方案。在US7800187B2中所示的结构具有以下缺陷:与n+区的接触以及间隔的P体区占用很大区域,这抵消了PNM-IGBT的基本思想,PNM-IGBT的基本思想是实现非常窄的台面区域,从而在导通状态下在n基体区域中实现高载流子浓度。PNM-IGBTs are described in US6521538B2 and US7800187B2. However, no solution to the above technical problems has been proposed in the prior art. The structure shown in US7800187B2 has the following drawbacks: the contact with the n+ region and the spaced P-body region occupy a large area, which counteracts the basic idea of the PNM-IGBT, which is to achieve a very narrow mesa area , thus achieving a high carrier concentration in the n-base region in the on-state.
实用新型内容Utility model content
鉴于上述问题,期望提供至少能够避免上述一个缺陷的IGBT器件。In view of the above problems, it is desirable to provide an IGBT device capable of avoiding at least one of the above disadvantages.
根据本实用新型的一个方面,提供了一种绝缘栅双极型晶体管,包括:发射极;以及半导体主体,其中所述半导体主体包括:第一基区,具有第一导电类型;源区,具有不同于所述第一导电类型的第二导电类型,并与所述第一基区形成第一pn结;防闩锁区,形成在所述第一基区中,具有至少一个位于所述源区之下并与所述源区接触的第一部分,所述防闩锁区具有所述第一导电类型,并且掺杂浓度大于所述第一基区的掺杂浓度;以及至少一个沟槽,其中,所述至少一个沟槽被填充有栅电极,其中,所述至少一个沟槽具有:第一沟槽部,具有第一宽度;以及第二沟槽部,具有第二宽度;所述第二宽度不同于所述第一宽度。According to one aspect of the present invention, there is provided an insulated gate bipolar transistor, comprising: an emitter; and a semiconductor body, wherein the semiconductor body includes: a first base region having a first conductivity type; a source region having a second conductivity type different from the first conductivity type, and forming a first pn junction with the first base region; an anti-latch-up region, formed in the first base region, having at least one a first portion below and in contact with the source region, the anti-latch-up region having the first conductivity type and having a doping concentration greater than that of the first base region; and at least one trench, Wherein, the at least one trench is filled with a gate electrode, wherein the at least one trench has: a first trench portion having a first width; and a second trench portion having a second width; the first trench portion having a second width; The second width is different from the first width.
优选地,所述第一基区的一部分横向方向位于所述防闩锁区的第二部分和所述至少一个沟槽之间。Preferably, a portion of the first base region is located laterally between the second portion of the anti-latch-up region and the at least one trench.
优选地,所述第一基区的一部分横向方向位于所述防闩锁区的第一部分和所述至少一个沟槽之间。Preferably, a portion of the first base region is located laterally between the first portion of the anti-latch-up region and the at least one trench.
优选地,所述防闩锁区与所述沟槽之间的距离为100nm-800nm。Preferably, the distance between the anti-latch-up region and the trench is 100nm-800nm.
优选地,所述防闩锁区的至少一部分与所述至少一个第一沟槽的绝缘部接触,所述绝缘部将所述栅电极至少与所述源区和所述第一基区绝缘。Preferably, at least a part of the anti-latch-up region is in contact with an insulating portion of the at least one first trench, the insulating portion insulating the gate electrode from at least the source region and the first base region.
优选地,所述源区包括第一源区和第二源区,其中,所述防闩锁区的第二部分和所述第一基区的在所述发射极侧的表面的一部分位于所述发射极侧的所述第一源区的表面和所述第二源区的表面之间。Preferably, the source region includes a first source region and a second source region, wherein the second portion of the anti-latch-up region and a portion of the surface of the first base region on the side of the emitter are located at the Between the surface of the first source region on the side of the emitter and the surface of the second source region.
优选地,所述源区沿着所述第一方向的宽度为0.5μm-3μm。Preferably, the width of the source region along the first direction is 0.5 μm-3 μm.
优选地,所述防闩锁区形成有凹槽,其中,所述凹槽被填充有所述发射极的一部分,使得所述发射极与所述源区和所述防闩锁区接触。Preferably, the anti-latch-up region is formed with a groove, wherein the groove is filled with a portion of the emitter such that the emitter contacts the source region and the anti-latch-up region.
优选地,所述凹槽的深度至少等于所述防闩锁区的第一部分和所述源区之间的pn结的深度。Preferably, the depth of the groove is at least equal to the depth of a pn junction between the first portion of the anti-latch-up region and the source region.
优选地,所述凹槽在与所述至少一个沟槽的延伸方向相同的方向延伸。Preferably, said groove extends in the same direction as said at least one groove extends.
优选地,介电层位于所述发射极和所述半导体主体之间;Preferably, a dielectric layer is located between said emitter and said semiconductor body;
所述发射极包括:第一发射极部分,位于所述介电层之上;以及第二发射极部分,穿过所述介电层,从所述第一发射极部分延伸至所述凹槽中。The emitter includes: a first emitter portion overlying the dielectric layer; and a second emitter portion extending through the dielectric layer from the first emitter portion to the recess middle.
优选地,所述源区包括第一源区和第二源区,分别位于所述第二发射极部分的两侧。Preferably, the source region includes a first source region and a second source region respectively located on two sides of the second emitter portion.
优选地,所述第二沟槽部沿所述绝缘栅双极型晶体管的垂直方向设置在所述第一沟槽部之下,其中,在所述绝缘栅双极型晶体管的横向方向,所述第二宽度大于所述第一宽度。Preferably, the second trench portion is disposed below the first trench portion along a vertical direction of the IGBT, wherein, in a lateral direction of the IGBT, the The second width is greater than the first width.
优选地,所述第一沟槽部的第一宽度是沿所述第一沟槽部的均匀宽度。Preferably, the first width of the first groove portion is a uniform width along the first groove portion.
优选地,所述至少一个沟槽包括绝缘部,将所述栅电极至少与所述源区和所述第一基区绝缘。Preferably, the at least one trench includes an insulating portion insulating the gate electrode from at least the source region and the first base region.
优选地,一对所述栅极沟槽和所述源区限定出一个台面结构,所述台面结构的末端的某些位置具有拐角结构、倒角结构或圆弧结构。Preferably, a pair of the gate trench and the source region define a mesa structure, and certain positions at the ends of the mesa structure have corner structures, chamfer structures or arc structures.
优选地,所述防闩锁区的多个部位以预定间隔延伸至所述栅极沟槽结构的预定位置。Preferably, the multiple positions of the anti-latch-up region extend to predetermined positions of the gate trench structure at predetermined intervals.
优选地,所述栅极还包括:栅极沟槽连接部,垂直于所述至少一个栅极沟槽的延伸方向,并连接两个所述栅极沟槽。Preferably, the gate further includes: a gate trench connecting portion, which is perpendicular to the extending direction of the at least one gate trench and connects the two gate trenches.
优选地,所述防闩锁区的预定部位延伸至所述栅极沟槽连接部;或所述防闩锁区的预定部位延伸至所述至少一个沟槽与所述栅极沟槽连接部所形成的拐角处。Preferably, a predetermined portion of the anti-latch-up region extends to the connecting portion of the gate trench; or a predetermined portion of the anti-latch-up region extends to the connecting portion between the at least one trench and the gate trench formed corners.
优选地,所述绝缘栅双极型晶体管是沟槽栅场终止型绝缘栅双极型晶体管。Preferably, the insulated gate bipolar transistor is a trench gate field stop type insulated gate bipolar transistor.
优选地,所述的绝缘栅双极型晶体管还包括:漂移区,具有不同于所述第一导电类型的第二导电类型,并位于所述第一基区的与发射极侧相反的一侧,并与所述第一基区形成第二pn结;集电区,具有所述第一导电类型,并位于所述第二基区的与所述第一基区侧相反的一侧;以及集电极,与所述集电区接触。Preferably, the insulated gate bipolar transistor further includes: a drift region having a second conductivity type different from the first conductivity type and located on the side opposite to the emitter side of the first base region , and form a second pn junction with the first base region; a collector region having the first conductivity type and located on a side of the second base region opposite to the side of the first base region; and a collector electrode in contact with the collector region.
优选地,所述至少一个沟槽在所述漂移区中延伸。Preferably, said at least one trench extends in said drift region.
优选地,所述的绝缘栅双极型晶体管,还包括:介电层,位于所述发射极和所述第一基区之间;所述发射极包括:第一发射极部分,位于所述介电层之上;以及第二发射极部分,穿过所述介电层,从所述第一发射极部分延伸至所述源区,并与所述源区形成接触区。Preferably, the IGBT further includes: a dielectric layer located between the emitter and the first base region; the emitter includes: a first emitter portion located at the above a dielectric layer; and a second emitter portion extending through the dielectric layer from the first emitter portion to the source region and forming a contact region with the source region.
优选地,在所述发射极和所述源区之间设置有接触区。Preferably, a contact region is provided between the emitter and the source region.
优选地,所述接触区包含硒或硫原子。Preferably, the contact region contains selenium or sulfur atoms.
优选地,所述接触区是阻挡层。Preferably, the contact area is a barrier layer.
优选地,所阻挡层包括Ti、Tiw、TiN、TaN中的至少一个。Preferably, the blocking layer includes at least one of Ti, Tiw, TiN, TaN.
通过本实用新型的技术方案,有效防止了在IGBT发生闩锁(Latchup)效应;而且降低了在短路操作时流过器件的电流密度,延长了器件寿命;减小或消除了MOS沟道阈值电压的不稳定。Through the technical scheme of the utility model, the latch-up (Latchup) effect in the IGBT is effectively prevented; and the current density flowing through the device during short-circuit operation is reduced, and the life of the device is prolonged; the threshold voltage of the MOS channel is reduced or eliminated unstable.
附图说明Description of drawings
在附图中,不同视图中的相似参考符号一般表示相同部分。附图不一定按比例绘制,重点在于对本实用新型的原则进行图解说明。在以下说明中,根据以下附图对本实用新型的各个实施方式进行了说明,在附图中:In the drawings, like reference characters in different views generally identify the same parts. The drawings are not necessarily to scale, emphasis instead being placed upon illustrating the principles of the invention. In the following description, various embodiments of the present utility model are described according to the following drawings, in the drawings:
图1是示出现有的IGBT的一个实例的斜视图;FIG. 1 is a perspective view showing an example of a conventional IGBT;
图2A是示出根据本实用新型的一个实施方式的IGBT的截面图;2A is a cross-sectional view illustrating an IGBT according to an embodiment of the present invention;
图2B是示出根据本实用新型的一个实施方式的IGBT的斜视图。FIG. 2B is a perspective view showing an IGBT according to an embodiment of the present invention.
图3是示出根据本实用新型的一个变形例的IGBT的斜视图;Fig. 3 is a perspective view showing an IGBT according to a modified example of the present invention;
图4是示出根据本实用新型的一个变形例的IGBT的斜视图;Fig. 4 is a perspective view showing an IGBT according to a modified example of the present invention;
图5A、图5B和图5C是示出根据本实用新型的另外的几个变形例的IGBT的截面图;以及5A, 5B and 5C are cross-sectional views illustrating IGBTs according to several other modified examples of the present invention; and
图6是示出根据本实用新型的另一个变形例的IGBT的截面图。FIG. 6 is a cross-sectional view showing an IGBT according to another modified example of the present invention.
具体实施方式Detailed ways
以下详细说明参照附图进行,附图以图解方式示出可实施本实用新型的具体细节和实施方式。The following detailed description refers to the accompanying drawings, which illustrate by way of illustration specific details and embodiments in which the invention may be practiced.
本文可使用关于在侧面或表面“之上”形成材料的词语“之上”,表示该材料可“直接”形成于所述侧面或表面“之上”,例如,与其直接接触;或者,也可表示材料“间接”形成于所述侧面或表面“之上”,所述侧面或表面与该材料之间设有一个或多个附加层。因为实施方式的组件可设置于多种不同的方位,所以方向性术语仅用于示出的目的,而绝不是用于限制。The word "on" may be used herein with reference to forming a material "on" a side or surface to mean that the material may be formed "directly" on said side or surface, e.g., in direct contact with it; Means that the material is formed "indirectly" on the side or surface with one or more additional layers between the side or surface and the material. Because components of an embodiment may be disposed in a variety of different orientations, directional terms are used for purposes of illustration only and are by no means limiting.
本实用新型的核心之一是通过在源区之下使用区域p+(防闩锁区)防止在IGBT中发生闩锁。One of the cores of the invention is to prevent latch-up in the IGBT by using the region p+ (anti-latch-up region) below the source region.
本实用新型的实施方式中,在n+源区之下插入一区域p+,目的是减小源区之下的p区的电阻。因此空穴能够通过该高导电率区域流到发射极接触区(contact),而不会导致压降过大以将源极-体区-pn结正向偏置,从而防止了闩锁。In the embodiment of the present invention, a region p+ is inserted under the n+ source region, in order to reduce the resistance of the p region under the source region. Holes are thus able to flow through this high conductivity region to the emitter contact without causing an excessive voltage drop to forward bias the source-body-pn junction, thereby preventing latch-up.
优选实施例:Preferred embodiment:
1)在一个优选实施例中,区域p+和通过沟槽接触与n+源区同时接触。1) In a preferred embodiment, the region p+ is contacted simultaneously with the n+ source region through a trench contact.
2)在第二优选实施例中,区域P+到达位于台面的末端的某些位置的沟槽。这可以是一个拐角(corner)或者位于台面的最末端。在这些位置,源极之下的p掺杂如此高,以至于在额定范围内的栅极电压下没有MOS沟道能够形成。因此,上述降低的或不稳定的MOS阈值电压的问题得到了解决。2) In the second preferred embodiment, the region P+ reaches the trench at some position at the end of the mesa. This can be a corner or at the very end of the countertop. At these locations, the p-doping under the source is so high that no MOS channel can form at gate voltages within the nominal range. Therefore, the above-mentioned problem of reduced or unstable MOS threshold voltage is solved.
3)在第三优选实施例中,区域P+到达沟槽的沿着台面的大部分或多或少的规则间隔开的位置。这导致沟道宽度以及短路模式流过的电流的相当大的减少。取决于剩余的有源沟道宽度,可以实现更长的短路持续时间。3) In a third preferred embodiment, the regions P+ reach more or less regularly spaced locations along most of the mesa of the trench. This results in a considerable reduction of the channel width as well as the current flowing in short-circuit mode. Depending on the remaining active channel width, longer short durations can be achieved.
以下参照附图具体描述:Describe in detail below with reference to accompanying drawing:
图2A是示出根据本实用新型的一个实施方式的IGBT的截面图。参照图2A,IGBT200被示出为具有沟槽栅场终止型结构,其包括顺次层叠的集电极C、p型集电区21、n型场终止区22、n-型漂移区23;半导体主体,其中所述半导体主体包括:p型基区24以及n+型源区25,以及形成在n-型漂移区23、p型基区24以及n+型源区25中的栅极26和栅氧化层27,其中,所述n+型源区25与所述第一基区24形成第一pn结。另外,在p型基区24、n+型源区25、栅极26的上表面上形成有介电层(层间电介质)28。其中,n-型漂移区23位于所述第一基区24的与发射极侧相反的一侧,并与所述第一基区24形成第二pn结。FIG. 2A is a cross-sectional view illustrating an IGBT according to an embodiment of the present invention. Referring to FIG. 2A, the IGBT200 is shown as having a trench gate field stop type structure, which includes a sequentially stacked collector electrode C, a p-
IGBT200还包括至少一个沟槽,其中所述至少一个沟槽被填充有栅电极26,其中,所述至少一个沟槽具有:第一沟槽部261(为了便于说明,填充在所述第一沟槽部261中的第一栅极部也由标号261表示),具有第一宽度;以及第二沟槽部262(为了便于说明,填充在所述第二沟槽部262中的第二栅极部也由标号262表示)。所述第二沟槽部262沿所述绝缘栅双极型晶体管200的垂直方向设置在所述第一沟槽部261之下,其中,在所述绝缘栅双极型晶体管200的横向方向,所述第二宽度大于所述第一宽度。所述至少一个沟槽在所述漂移区23中延伸。The IGBT200 also includes at least one trench, wherein the at least one trench is filled with the
所述第一沟槽部261的第一宽度是沿所述第一沟槽部的均匀宽度。The first width of the
所述至少一个沟槽包括绝缘部27,将所述栅电极26至少与所述源区25和所述第一基区24绝缘。The at least one trench includes an insulating
IGBT200还具有发射极29,发射极29包括第一发射极部分291和第二发射极部分292。第一发射极部分291形成在介电层28上,换句话说,介电层28位于所述发射极29和所述半导体主体之间。第二发射极部分292从第一发射极部分291的下表面向下延伸穿过介电层28,与n+型源区25接触。
集电区21具有所述第一导电类型,并位于所述第二基区(漂移区23)的与所述第一基区24侧相反的一侧;集电极C与所述集电区21接触。The
该实施方式中,还设置有接触区P+(防闩锁区),形成在p型基区24中,所述接触区P+的至少一部分位于所述源区25之下并与所述源区25接触,所述接触区P+为P+掺杂,并且掺杂浓度大于所述第一基区24的掺杂浓度。所述防闩锁区P+的至少一部分与所述至少一个第一沟槽的绝缘部27接触。In this embodiment, a contact region P+ (anti-latch-up region) is also provided, formed in the p-
其中,所述防闩锁区P+与所述发射极29接触。所述防闩锁区P+具有与源区25横向相邻的第二部。所述第一基区的一部分横向方向位于所述防闩锁区P+的第二部分和所述至少一个沟槽之间。Wherein, the anti-latch-up region P+ is in contact with the
优选地,所述防闩锁区P+与所述栅极沟槽之间的距离为100nm-800nm。Preferably, the distance between the anti-latch-up region P+ and the gate trench is 100nm-800nm.
所述防闩锁区P+的至少一部分与所述沟槽的绝缘部27接触,所述绝缘部27将所述栅电极26至少与所述源区25和所述第一基区24绝缘。At least a part of the anti-latch-up region P+ is in contact with the insulating
所述源区25包括第一源区和第二源区,其中,所述防闩锁区P+的第二部分和所述第一基区24的在所述发射极侧的表面的一部分位于所述发射极29侧的所述第一源区的表面和所述第二源区的表面之间。The
一对所述栅极沟槽和所述源区25限定出一个台面结构,所述台面结构的末端的某些位置具有拐角结构、倒角结构或圆弧结构。通过设置接触区P+,能够减小源区25之下的p区的电阻。因此空穴能够通过该高导电率区域流到发射极接触区(contact),而不会在该区域产生过大的压降,以将源极-体区-pn结正向偏置,从而防止了闩锁。A pair of the gate trenches and the
图2B是示出根据本实用新型的一个实施方式的IGBT的斜视图。FIG. 2B is a perspective view showing an IGBT according to an embodiment of the present invention.
在图2B中,为便于观察,省略了发射极与半导体上侧表面之间的介电层。In FIG. 2B , for ease of observation, the dielectric layer between the emitter and the upper surface of the semiconductor is omitted.
该实施方式中,所述源区25可包括n个子源区,以预定间隔沿着第一方向(即图中垂直于纸面的方向)设置于所述第一基区24之上,其中n为大于或等于2的整数。In this embodiment, the
可用不同的方式制造所述接触区P+。如果使用了与半导体表面的平面接触,该接触区P+能够在所述第一方向以与源区25交替的方式制造。在没有源区25的位置处,区域P+域可到达半导体表面。The contact region P+ can be produced in different ways. If a planar contact to the semiconductor surface is used, the contact regions P+ can be produced in the first direction alternating with the
即,除了前面所提到的,所述接触区P+的一部分位于所述源区25之下并与所述源区25接触,所述接触区P+还可包括第二部分,该第二部分与所述n个子源区交替设置。That is, in addition to the aforementioned, a part of the contact region P+ is located under the
第一方向上的子源极区的宽度必须保持足够小(例如,0.5μm–3μm),以尽量减少该子源极区之下可能产生闩锁效应的电流的路径,从而防止发生闩锁。The width of the sub-source region in the first direction must be kept small enough (for example, 0.5 μm-3 μm) to minimize the path of current under the sub-source region that may cause latch-up, thereby preventing latch-up from occurring.
图2B中示出了源区25包括两个子源区,分别设置于半导体表面的前部和后部,接触区P+的第二部分设置于两个子源区之间;所述接触区P+的第二部分的上表面与所述源区25的上表面齐平,当然也可以设置为并非齐平。Figure 2B shows that the
其中,栅极26形成于栅极沟槽中,其包括:第一栅极部分261,具有均匀宽度;以及第二栅极部分262,位于所述第一栅极部分261以下,并且具有大于所述均匀宽度的宽度。Wherein, the
一对所述栅极沟槽与所述源区25限定出一个台面结构,所述台面结构的末端的某些位置具有拐角结构、倒角结构或圆弧结构。A pair of gate trenches and the
图3是示出根据本实用新型的一个变形例的IGBT的斜视图;Fig. 3 is a perspective view showing an IGBT according to a modified example of the present invention;
接触区域P+的另一种可能性是使用凹槽(groove)接触来将接触区连接到发射极金属。Another possibility for the contact region P+ is to use a groove contact to connect the contact region to the emitter metal.
图3中示出了这样的实施方式。该实施方式与图2A、图2B中所示的实施方式相比,主要区别在于,接触区P+的上表面形成有凹槽(groove)G1,其中,所述凹槽G1被填充有所述发射极39的一部分,使得所述发射极与所述源区35和所述防闩锁区P+接触。凹槽G1的延伸方向可与栅极36的沟槽(trench)的延伸方向相同,即图中垂直于纸面的方向。第二发射极部分392的下部穿过n+型源区35并延伸至凹槽G1的底部。由于发射极39与接触区P+形成了凹槽接触,其旁路(bypass)所述基区34和n+源区35之间的pn结,从而部分地短路由p型集电区31、n型场终止区32、n-型漂移区33、p型基区34以及n+型源区35形成的PNPN结构,也就是说,由n-型漂移区33、p型基区34以及n+型源区35形成的寄生npn晶体管在p型基区34和n+型源区35之间起到短路作用。因此在IGBT300过电流截止期间,p型基区34的位于n+型源区35之下的长度被限制到沟槽和凹槽接触之间的距离,从而降低截止期间的欧姆压降。因此,避免了IGBT300在截止期间出现闩锁,保证了IGBT300的正常工作。Such an embodiment is shown in FIG. 3 . Compared with the embodiment shown in FIG. 2A and FIG. 2B , the main difference of this embodiment is that a groove G1 is formed on the upper surface of the contact region P+, wherein the groove G1 is filled with the emitter A portion of the
优选地,凹槽G1的深度至少等于所述接触区P+的第一部分和n+型源区35之间形成的pn结的深度。在这种情况下,可以使用连续的n+源区。如图3中所示,所述源区25包括第一源区和第二源区,分别位于所述第二发射极部分392两侧。其中第一源区和第二源区各自都为连续的,不同于图2A、图2B中所示的以预定间隔设置。Preferably, the depth of the groove G1 is at least equal to the depth of the pn junction formed between the first part of the contact region P+ and the n+
所述凹槽G1在与至少一个沟槽的延伸方向相同的方向延伸。其中,凹槽G1的底部可距由p型基区34和n+型源区35共同形成的半导体上侧表面0.2至1.5μm。The groove G1 extends in the same direction as that of the at least one groove. Wherein, the bottom of the groove G1 may be 0.2 to 1.5 μm away from the upper surface of the semiconductor formed by the p-
由此,可以确保IGBT300中的寄生npn晶体管的基区和发射极被有效地短路。Thereby, it can be ensured that the base region and the emitter of the parasitic npn transistor in
图4是示出根据本实用新型的一个变形例的IGBT的截面图;以及4 is a cross-sectional view illustrating an IGBT according to a modified example of the present invention; and
图4中所示的实施方式中,IGBT400是从源区45的上表面剖开的。与之前的实施方式不同之处在于,所述IGBT400的栅极26还包括:第三栅极部分44,具有均匀宽度,垂直于所述第一栅极部分461,第二栅极部462,并连接彼此相对的两个第一栅极部分461和462。In the embodiment shown in FIG. 4 ,
第三栅极部463,也称作沟槽连接部,垂直于所述至少一个栅极沟槽的延伸方向,并连接两个所述栅极沟槽。The
所述防闩锁区P+的预定部位延伸至所述栅极沟槽连接部463;或所述防闩锁区P+的预定部位延伸至所述至少一个沟槽与所述栅极沟槽连接部463所形成的拐角处。A predetermined portion of the anti-latch-up region P+ extends to the gate
图5A、图5B和图5C是示出根据本实用新型的另外的几个变形例的IGBT的截面图;5A, 5B and 5C are cross-sectional views illustrating IGBTs according to several other modified examples of the present invention;
图5A、图5B和图5C示出了区域P+接触沟槽的实施例。所示的三个实施例是沿着n+源极区之下(以及接触凹槽之下)的深度水平剖开的。5A, 5B and 5C illustrate embodiments of region P+ contact trenches. The three embodiments shown are sectioned horizontally along the depth below the n+ source region (and below the contact groove).
根据本实用新型的一些实施例,所述接触区P+延伸至所述台面结构末端的栅极沟槽的预定位置。其中,所述接触区P+的边缘处与栅极沟槽的距离必须相当小,例如,100nm-800nm。这也指的是不位于台面结构的末端的接触区P+的某些部分。According to some embodiments of the present invention, the contact region P+ extends to a predetermined position of the gate trench at the end of the mesa structure. Wherein, the distance between the edge of the contact region P+ and the gate trench must be relatively small, for example, 100nm-800nm. This also refers to certain parts of the contact region P+ that are not located at the ends of the mesa structures.
防闩锁区P+的多个部位以预定间隔延伸至所述栅极沟槽结构的预定位置。Multiple parts of the anti-latch-up region P+ extend to predetermined positions of the gate trench structure at predetermined intervals.
具体地,如图5A所示,所述接触区P+的预定部位(左上侧角581和右上侧角582延伸至所述第一、第二栅极部分461,462的沟槽与所述第三栅极部分463的沟槽形成的拐角处。该拐角(corner)可以为90度至135°角或其他角度,也可以是弄圆了的角。Specifically, as shown in FIG. 5A, the predetermined parts of the contact region P+ (the upper
如图5B所述,所述接触区P+的预定部位延伸至台面结构的一侧的整个末端583,即,所述第三栅极部分的沟槽处;As shown in FIG. 5B , the predetermined portion of the contact region P+ extends to the
在这些位置,源极之下的p掺杂如此高,以至于在额定范围内的栅极电压下没有MOS沟道能够形成。因此,上述降低的或不稳定的MOS阈值电压的问题得到了解决。At these locations, the p-doping under the source is so high that no MOS channel can form at gate voltages within the nominal range. Therefore, the above-mentioned problem of reduced or unstable MOS threshold voltage is solved.
如图5C所述,区域P+到达沟槽的沿着台面的大部分或多或少的规则间隔开的位置,具体地,所述接触区P+多个部位585、586以预定间隔延伸至靠近所述第一栅极的沟槽处。As shown in FIG. 5C , the region P+ reaches more or less regularly spaced locations along most of the mesa of the trench, in particular, the contact region P+ has a plurality of
图5C所示的技术方案,能够导致沟道宽度降低以及短路模式流过的电流的相当大的降低。取决于剩余的有源沟道宽度,可以实现更长的短路持续时间。The technical solution shown in FIG. 5C can lead to a reduction in the channel width and a considerable reduction in the current flowing in the short-circuit mode. Depending on the remaining active channel width, longer short durations can be achieved.
图6是示出根据本实用新型的另一个变形例的IGBT的截面图。FIG. 6 is a cross-sectional view showing an IGBT according to another modified example of the present invention.
本实用新型进一步的实施例通过不同的方法防止闩锁。此处,通过将掺杂等级降至,例如,1*1019cm-3或者甚至优选降至1*1018cm-3之下,n+源区的发射效率会降低。由于只有当npn晶体管(n源极/p体区/n漂移区)以及pnp晶体管(p发射极/n漂移区/p体区)的增益之和达到1时,闩锁才会出现,降低npn结晶体管的增益能够防止闩锁。由于与唯一适度高掺杂的n源极的接触电阻将会很高,没有进一步措施,该实施例应该与位于接触金属和n源极之间的界面处的额外接触区相结合。该额外的接触区具有低接触电阻,可以是注入有,例如,硒或硫离子的区域。特别地,硒原子的注入导致欧姆接触处于较低掺杂浓度,因为在离子注入范围的末端,硒原子分离并部分形成能量级深深位于带隙间的电无源簇(inactivecluster)。通常的注入剂量在3*1013硒原子每cm3和3*1014硒原子每cm3。离子注入能量应该在20和150KeV之间或者最好在30至70keV之间范围内。A further embodiment of the invention prevents latch-up by a different method. Here, by reducing the doping level to, for example, 1*1019 cm-3 or even preferably below 1*1018 cm-3, the emission efficiency of the n+ source region is reduced. Since the latch-up occurs only when the sum of the gains of the npn transistor (n source/p body/n drift region) and the pnp transistor (p emitter/n drift region/p body region) reaches 1, reduce the npn The gain of the junction transistor prevents latch-up. Since the contact resistance with only a moderately highly doped n-source will be high, without further measures, this embodiment should be combined with an additional contact area at the interface between the contact metal and the n-source. This additional contact region has a low contact resistance and may be a region implanted with, for example, selenium or sulfur ions. In particular, the implantation of selenium atoms results in lower doping concentrations for ohmic contacts, since at the end of the ion-implantation range, the selenium atoms separate and partially form electrically inactive clusters with energy levels deep in the bandgap. The usual implant dose is 3*1013 selenium atoms per cm3 and 3*1014 selenium atoms per cm3. The ion implantation energy should be in the range between 20 and 150 KeV or preferably between 30 and 70 KeV.
可选地,可通过高剂量注入通常非掺杂元素(例如氩或硅)能够实现具有强损坏以及深能级高浓度的欧姆接触区;优选地,后续退火温度应该在950°C之下或者在350°C之下更好,或者在300°C之下更好。Alternatively, high-dose implantation of normally non-doped elements (such as argon or silicon) can achieve ohmic contact regions with strong damage and a high concentration of deep levels; preferably, the subsequent annealing temperature should be below 950°C or Better yet, below 350°C, or better yet, below 300°C.
此外,可以提供源极区中的n型掺杂等级的横向变化;例如,该区域中较高的掺杂级别(其中p型浓度高),以及该区域中较低的掺杂级别(其中,p型浓度低)。以此方式,能够实现发射极效率的同质的(homogenous)降低。Furthermore, a lateral variation of the n-type doping level in the source region can be provided; for example, a higher doping level in this region (where p-type concentration is high), and a lower doping level in this region (where, low concentration of p-type). In this way, a homogenous reduction in emitter efficiency can be achieved.
图6所示的IGBT600为采用上述方法形成的,与图2A所示的IGBT200的区别在于发射极69的第二部分692之下形成有额外的接触区61。The
如图6所示,发射极69,位于所述源区65之上;介电层68,位于所述发射极69和所述第一基区64之间;所述发射极69包括:第一发射极部分691,位于所述介电层68之上;以及第二发射极部分692,穿过所述介电层68。与所述源区65的电接触是通过额外的接触区61实现的。该接触区61设置在发射极和源区65之间。As shown in FIG. 6, the
所述接触区61包含硒或硫原子。所述接触区61是阻挡层。所阻挡层包括Ti、TiW、TiN、TaN中的至少一个。The
通过图6所示的技术方案,同样能够有效防止闩锁的形成。Through the technical solution shown in FIG. 6 , the formation of latches can also be effectively prevented.
尽管上文以具有局部窄台结构的IGBT器件为例进行了说明,但本实用新型的技术不限于此,例如也可应用于具有通常的沟槽栅结构的IGBT尽管上文以具有沟槽栅场终止型结构的IGBT器件为例进行了说明,但本实用新型的技术不限于此,例如也可应用于平面栅结构的IGBT器件。在除上文所述的IGBT器件之外的具有其他结构的IGBT器件中,应用本实用新型的技术,同样能够有效地避免闩锁效应的发生。Although the IGBT device with a local narrow mesa structure has been described above as an example, the technology of the present invention is not limited thereto. For example, it can also be applied to an IGBT with a common trench gate structure. An IGBT device with a field stop structure is described as an example, but the technology of the present invention is not limited thereto, for example, it can also be applied to an IGBT device with a planar gate structure. In IGBT devices with other structures than the above-mentioned IGBT devices, the technology of the present invention can also be used to effectively avoid the latch-up effect.
上文根据特定实施方式对本实用新型进行了具体示出和说明,但本领域的技术人员应理解,只要不脱离所附权利要求限定的本实用新型的主旨和范围,可对其形式和细节进行各种改变。因此,本实用新型的范围如所附权利要求所述,因此,只要符合权利要求等同物的意义和范围,可进行各种改变。The utility model has been specifically shown and described according to specific embodiments above, but those skilled in the art should understand that as long as it does not depart from the gist and scope of the utility model defined by the appended claims, its form and details can be modified. Various changes. Therefore, the scope of the present invention is as described in the appended claims, and therefore, various changes may be made as long as they are within the meaning and range of equivalency of the claims.
Claims (29)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201320220862.6U CN203456468U (en) | 2013-04-26 | 2013-04-26 | Insulated gate bipolar transistor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201320220862.6U CN203456468U (en) | 2013-04-26 | 2013-04-26 | Insulated gate bipolar transistor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN203456468U true CN203456468U (en) | 2014-02-26 |
Family
ID=50136325
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201320220862.6U Expired - Lifetime CN203456468U (en) | 2013-04-26 | 2013-04-26 | Insulated gate bipolar transistor |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN203456468U (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111418072A (en) * | 2018-06-22 | 2020-07-14 | 富士电机株式会社 | Method for manufacturing semiconductor device and semiconductor device |
-
2013
- 2013-04-26 CN CN201320220862.6U patent/CN203456468U/en not_active Expired - Lifetime
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111418072A (en) * | 2018-06-22 | 2020-07-14 | 富士电机株式会社 | Method for manufacturing semiconductor device and semiconductor device |
| CN111418072B (en) * | 2018-06-22 | 2023-11-21 | 富士电机株式会社 | Semiconductor device manufacturing method and semiconductor device |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US11735584B2 (en) | Semiconductor device | |
| USRE47198E1 (en) | Power semiconductor device | |
| CN110574146B (en) | Semiconductor device | |
| JP3935042B2 (en) | Insulated gate semiconductor device | |
| US8344480B2 (en) | Insulated gate bipolar transistor | |
| CN104952925B (en) | Trench transistor device | |
| CN102420242B (en) | Semiconductor device | |
| CN108604594A (en) | The manufacturing method of semiconductor device and semiconductor device | |
| JP5781383B2 (en) | Power semiconductor devices | |
| TWI575736B (en) | Double trench gate insulating gate bipolar transistor structure | |
| CN107210299A (en) | Semiconductor device | |
| CN108365007B (en) | Insulated Gate Bipolar Transistor | |
| CN103872097B (en) | Power semiconductor device and its manufacture method | |
| US20150144989A1 (en) | Power semiconductor device and method of manufacturing the same | |
| CN107534053A (en) | Semiconductor device and manufacturing method thereof | |
| US20150171198A1 (en) | Power semiconductor device | |
| CN203288596U (en) | Insulated gate bipolar transistor | |
| CN203456468U (en) | Insulated gate bipolar transistor | |
| JP5292157B2 (en) | Horizontal insulated gate bipolar transistor and method of manufacturing the same | |
| KR101397784B1 (en) | Insulated gate bipolar transistor | |
| JP5309427B2 (en) | Semiconductor device | |
| KR20150031668A (en) | Power semiconductor device | |
| KR102013226B1 (en) | A insulated gate bipolar transistor | |
| JP5309428B2 (en) | Semiconductor device | |
| JP2024071184A (en) | Silicon carbide semiconductor device |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| CX01 | Expiry of patent term |
Granted publication date: 20140226 |
|
| CX01 | Expiry of patent term |