CN110504168A - A method for manufacturing a multi-slot gate lateral high-voltage power device - Google Patents
A method for manufacturing a multi-slot gate lateral high-voltage power device Download PDFInfo
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- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D12/00—Bipolar devices controlled by the field effect, e.g. insulated-gate bipolar transistors [IGBT]
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- H10D12/421—Insulated-gate bipolar transistors [IGBT] on insulating layers or insulating substrates, e.g. thin-film IGBTs
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- H10D12/01—Manufacture or treatment
- H10D12/031—Manufacture or treatment of IGBTs
- H10D12/032—Manufacture or treatment of IGBTs of vertical IGBTs
- H10D12/038—Manufacture or treatment of IGBTs of vertical IGBTs having a recessed gate, e.g. trench-gate IGBTs
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- H10D12/00—Bipolar devices controlled by the field effect, e.g. insulated-gate bipolar transistors [IGBT]
- H10D12/411—Insulated-gate bipolar transistors [IGBT]
- H10D12/441—Vertical IGBTs
- H10D12/461—Vertical IGBTs having non-planar surfaces, e.g. having trenches, recesses or pillars in the surfaces of the emitter, base or collector regions
- H10D12/481—Vertical IGBTs having non-planar surfaces, e.g. having trenches, recesses or pillars in the surfaces of the emitter, base or collector regions having gate structures on slanted surfaces, on vertical surfaces, or in grooves, e.g. trench gate IGBTs
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Abstract
本发明属于功率半导体技术领域,具体涉及一种多槽栅横向高压功率器件制造方法。本发明相对与传统结构,新结构在发射极端的N型存储层与集电极端的N型缓冲层、发射极端与集电极端的P型阱区可分别同步推结完成以降低器件热预算成本;发射极端与集电极端的多槽栅结构也可同步制作完成,在器件两端形成多沟道槽栅结构,以此改善器件导通压降与关断损耗。本发明的有益效果为简化器件工艺步骤与成本,实现易集成、低功耗的SOI LIGBT。The invention belongs to the technical field of power semiconductors, and in particular relates to a method for manufacturing a multi-slot gate lateral high-voltage power device. Compared with the traditional structure, the present invention has the N-type storage layer at the emitter end, the N-type buffer layer at the collector end, and the P-type well region at the emitter end and the collector end of the new structure, which can be pushed and completed synchronously to reduce the thermal budget cost of the device. ; The multi-slot gate structure of the emitter terminal and the collector terminal can also be manufactured simultaneously, and a multi-channel trench gate structure is formed at both ends of the device, so as to improve the turn-on voltage drop and turn-off loss of the device. The invention has the beneficial effects of simplifying device process steps and cost, and realizing easy integration and low power consumption SOI LIGBT.
Description
技术领域technical field
本发明属于功率半导体技术领域,涉及一种多槽栅SOI LIGBT(LateralInsulated Gate Bipolar Transistor,横向绝缘栅双极型晶体管)的制造方法。The invention belongs to the technical field of power semiconductors, and relates to a method for manufacturing a multi-slot gate SOI LIGBT (Lateral Insulated Gate Bipolar Transistor, lateral insulated gate bipolar transistor).
背景技术Background technique
绝缘栅双极型晶体管(IGBT)结合了MOS栅控器件的高输入阻抗和双极型器件的低导通压降的优势,实现了高击穿电压和大的导通电流,成为电力电子系统领域的代表器件,广泛应用于智能电网、高铁驱动、航空航天及家用电器等领域。由于SOI技术的发展,SOILIGBT器件有更小的泄漏电流和更小的寄生效应,因而成为单片功率集成芯片的核心元器件。Insulated-gate bipolar transistor (IGBT) combines the advantages of high input impedance of MOS gate-controlled devices and low conduction voltage drop of bipolar devices to achieve high breakdown voltage and large conduction current, and has become a power electronic system Representative devices in the field, widely used in smart grid, high-speed rail drive, aerospace and household appliances and other fields. Due to the development of SOI technology, SOIL IGBT devices have smaller leakage currents and smaller parasitic effects, thus becoming the core components of monolithic power integrated chips.
LIGBT器件作为双极型器件,在导通时会发生电导调制效应在漂移区内储存大量载流子,在降低正向导通压降的同时,也带来了器件关断速度变慢和关断损耗变大的问题。另外,体内寄生晶闸管的存在可能使器件发生闩锁效应,从而安全工作区受到限制。因此,改善IGBT的安全工作区、正向导通压降以及关断损耗三者之间的矛盾关系,成为研究的一大热点。As a bipolar device, the LIGBT device will have a conductance modulation effect when it is turned on, and a large number of carriers will be stored in the drift region. The problem of increased loss. In addition, the presence of parasitic thyristors in the body may cause latch-up of the device, thereby limiting the safe operating area. Therefore, improving the contradictory relationship between the IGBT's safe operating area, forward voltage drop, and turn-off loss has become a hot research topic.
发明内容Contents of the invention
本发明的目的,就是针对上述问题,提出一种多槽栅SOI LIGBT的制造方法。本发明的技术方案是:一种多槽栅SOI LIGBT的制造方法,其特征在于,包括以下步骤:The object of the present invention is to provide a method for manufacturing a multi-groove gate SOI LIGBT to solve the above problems. The technical solution of the present invention is: a method for manufacturing a multi-slot gate SOI LIGBT, which is characterized in that it comprises the following steps:
第一步:准备SOI材料,所述SOI材料包括自下而上的衬底层1、绝缘介质层2和N型漂移区3;The first step: preparing SOI material, said SOI material includes bottom-up substrate layer 1, insulating dielectric layer 2 and N-type drift region 3;
第二步:通过离子注入技术,在所述N型漂移区3表面的一端注入N型杂质,其杂质注入窗口是分段图形分布;Step 2: Implanting N-type impurities into one end of the surface of the N-type drift region 3 through ion implantation technology, and the impurity implantation windows are distributed in segmented patterns;
第三步:通过离子注入技术,在所述N型漂移区3表面的另一端注入N型杂质;Step 3: Implanting N-type impurities into the other end of the surface of the N-type drift region 3 by ion implantation technology;
第四步:将第二步与第三步中离子注入的N型杂质同时进行高温推结,对应形成发射极端的N型存储层41和集电极端的N型缓冲层42;The fourth step: push the junction at high temperature simultaneously with the N-type impurity implanted in the second step and the third step, corresponding to form the N-type storage layer 41 at the emitter end and the N-type buffer layer 42 at the collector end;
第五步:通过离子注入技术,在所述N型漂移区3具有所述N型存储层41的一端注入P型杂质;Step 5: Implanting P-type impurities into the end of the N-type drift region 3 having the N-type storage layer 41 by ion implantation technology;
第六步:通过离子注入技术,在所述N型缓冲层42上方注入P型杂质;Step 6: Implanting P-type impurities above the N-type buffer layer 42 by ion implantation technology;
第七步:将第五步和第六步中子注入的P型杂质同时进行高温推结,对应形成发射极端的P阱51和集电极端的P阱52;Step 7: Simultaneously push the P-type impurity implanted with neutrons in Step 5 and Step 6 into a high-temperature push-in junction, correspondingly forming the P-well 51 at the emitter end and the P-well 52 at the collector end;
第八步:采用刻蚀工艺在所述N型漂移区3两端同时刻蚀多个深度超过所述P阱51和P阱52的深槽;然后采用氧化工艺在槽侧壁形成栅介质层,接着深槽中填充多晶硅材料、平坦化后反刻图形化,最后形成由槽栅介质层81和槽栅多晶硅82组成的间断或互连的发射极控制槽栅,由槽栅介质层83和槽栅多晶硅84组成的发射极阻挡槽栅,由槽栅介质层91和槽栅多晶硅92组成的集电极阻挡槽栅,由槽栅介质层93和槽栅多晶硅94组成的间断或互连的集电极槽栅;其中所述发射极控制槽栅的刻蚀窗口位于所述N型存储层41的注入窗口之间;Step 8: using an etching process to simultaneously etch multiple deep grooves at both ends of the N-type drift region 3 that are deeper than the P well 51 and the P well 52; and then using an oxidation process to form a gate dielectric layer on the side walls of the groove , followed by filling the deep groove with polysilicon material, planarization, and reverse patterning, and finally forming an interrupted or interconnected emitter control groove gate composed of the groove gate dielectric layer 81 and the groove gate polysilicon 82, consisting of the groove gate dielectric layer 83 and the groove gate dielectric layer 83. The emitter blocking groove gate composed of the groove gate polysilicon 84, the collector blocking groove gate composed of the groove gate dielectric layer 91 and the groove gate polysilicon 92, the discontinuous or interconnected collection composed of the groove gate dielectric layer 93 and the groove gate polysilicon 94 Electrode groove gate; wherein the etching window of the emitter control groove gate is located between the injection windows of the N-type storage layer 41;
第九步:通过离子注入P型杂质在所述N型缓冲层42上部形成P+集电区62,所述槽栅介质91在靠近发射极的一侧与所述P+集电区62接触;Step 9: forming a P+ collector region 62 on the upper part of the N-type buffer layer 42 by ion implanting P-type impurities, and the groove gate dielectric 91 is in contact with the P+ collector region 62 on the side close to the emitter;
第十步:通过离子注入N型杂质以同时图形化形成在所述P阱51上部的N+发射区71和在所述P阱52上部的N+集电区72,其中所述槽栅介质层81与所述N+发射区71接触,所述槽栅介质层93与所述N+集电区72接触,所述槽栅介质层91在远离发射极端与所述N+集电区72接触;Step 10: Implanting N-type impurities by ion implantation to simultaneously pattern the N+ emitter region 71 on the upper part of the P well 51 and the N+ collector region 72 on the upper part of the P well 52, wherein the trench gate dielectric layer 81 In contact with the N+ emitter region 71, the groove gate dielectric layer 93 is in contact with the N+ collector region 72, and the groove gate dielectric layer 91 is in contact with the N+ collector region 72 at the end far away from the emitter;
第十一步:通过离子注入P型杂质以同时图形化形成在所述P阱51上部的体接触P+区61与在所述P阱52上部的体接触P+区63,所述接触P+区61与所述N+发射区71接触,所述体接触P+区63与所述N+集电区72接触,所述槽栅介质层83在远离集电极端与所述接触P+区61接触;The eleventh step: by ion implanting P-type impurities to simultaneously pattern the body contact P+ region 61 formed on the upper part of the P well 51 and the body contact P+ region 63 on the upper part of the P well 52, the contact P+ region 61 In contact with the N+ emitter region 71, the body contact P+ region 63 is in contact with the N+ collector region 72, and the groove gate dielectric layer 83 is in contact with the contact P+ region 61 at the end far away from the collector;
第十二步:在所述体接触P+区61、所述N+发射区71与槽栅多晶硅84的上表面形成发射极金属,在所述P+集电区62、体接触P+区63、N+集电区72、槽栅多晶硅92与槽栅多晶硅94的上表面形成集电极金属,在所述槽栅多晶硅82的上表面形成栅极金属;The twelfth step: form an emitter metal on the upper surface of the body contact P+ region 61, the N+ emitter region 71 and the groove gate polysilicon 84, and form an emitter metal on the P+ collector region 62, body contact P+ region 63, N+ collector The collector metal is formed on the upper surface of the electrical region 72 , the trench gate polysilicon 92 and the trench gate polysilicon 94 , and the gate metal is formed on the upper surface of the trench gate polysilicon 82 ;
进一步的,根据权利要求1所述的一种多槽栅SOI LIGBT的制造方法,其特征在于:第八步中所述的深槽刻蚀步骤后,在所述N型存储层41附近的深槽底部离子注入P型杂质以形成P型埋层53。Further, the manufacturing method of a multi-groove gate SOI LIGBT according to claim 1 is characterized in that: after the deep groove etching step described in the eighth step, the deep groove near the N-type storage layer 41 P-type impurities are implanted into the groove bottom to form a P-type buried layer 53 .
进一步的,根据权利要求1-2中所述的任意一种多槽栅SOI LIGBT的制造方法,其特征在于:第八步中形成的间断或互连的发射极控制槽栅、间断或互连的集电极槽栅的形状可以是矩形、菱形或六边形;Further, according to any one of the manufacturing methods of multi-groove gate SOI LIGBT described in claims 1-2, it is characterized in that: the discontinuous or interconnected emitter control groove gate, discontinuity or interconnection formed in the eighth step The shape of the collector grid can be rectangular, rhombus or hexagonal;
本发明的有益效果为,相对于传统LIGBT结构,新结构在发射极端与集电极端的工艺步骤兼容性高,导通时不仅有效消除snapback现象,还增强器件发射极端载流子注入效率与抗闩锁能力,并实现更快的关断速度与更低的关断损耗。The beneficial effect of the present invention is that, compared with the traditional LIGBT structure, the new structure has high compatibility between the process steps of the emitter terminal and the collector terminal, and not only effectively eliminates the snapback phenomenon when it is turned on, but also enhances the carrier injection efficiency and the resistance of the emitter terminal of the device. Latch-up capability, and achieve faster turn-off speed and lower turn-off loss.
附图说明Description of drawings
图1为SOI材料准备;Figure 1 is SOI material preparation;
图2为N型杂质注入形成N型缓冲层和N型存储层;FIG. 2 is an N-type impurity implantation to form an N-type buffer layer and an N-type storage layer;
图3为P型杂质注入形成两端的P阱区;Figure 3 shows the P-well regions at both ends formed by P-type impurity implantation;
图4为多槽栅刻蚀、栅氧化层生长、多晶硅淀积;Fig. 4 shows multi-groove gate etching, gate oxide layer growth, and polysilicon deposition;
图5为P型杂质注入形成P+集电区;Figure 5 shows the P+ collector region formed by P-type impurity implantation;
图6为形成N+发射区、N+集电区、体接触P+区;Figure 6 is the formation of N+ emitter region, N+ collector region, body contact P+ region;
图7为电极金属互连;Fig. 7 is the electrode metal interconnection;
图8为发射极端槽栅底部离子注入形成P型埋层;Figure 8 is the ion implantation at the bottom of the emitter trench gate to form a P-type buried layer;
图9、图10为间断分布的发射极控制槽栅与集电极槽栅版图布局为矩形或六边形;Figures 9 and 10 show the layout of the intermittently distributed emitter control slots and collector slots as rectangles or hexagons;
图11为矩形版图布局互连型发射极控制槽栅和集电极槽栅;Fig. 11 is a rectangular layout layout interconnection type emitter control slot gate and collector slot gate;
具体实施方式Detailed ways
下面结合附图和实施例,详细描述本发明的技术方案:Below in conjunction with accompanying drawing and embodiment, describe technical solution of the present invention in detail:
实施例1Example 1
本例中多槽栅SOI LIGBT器件的制造流程如下:The manufacturing process of the multi-groove gate SOI LIGBT device in this example is as follows:
一种多槽栅SOI LIGBT的制造方法,其特征在于,包括以下步骤:A method for manufacturing multi-groove gate SOI LIGBT, characterized in that it comprises the following steps:
第一步:准备SOI材料,所述SOI材料包括自下而上的衬底层1、绝缘介质层2和N型漂移区3,如图1所示;The first step: preparing SOI material, the SOI material includes a bottom-up substrate layer 1, an insulating dielectric layer 2 and an N-type drift region 3, as shown in Figure 1;
第二步:通过离子注入技术,在所述N型漂移区3表面的一端注入N型杂质,其杂质注入窗口是分段图形分布;Step 2: Implanting N-type impurities into one end of the surface of the N-type drift region 3 through ion implantation technology, and the impurity implantation windows are distributed in segmented patterns;
第三步:通过离子注入技术,在所述N型漂移区3表面的另一端注入N型杂质;Step 3: Implanting N-type impurities into the other end of the surface of the N-type drift region 3 by ion implantation technology;
第四步:将第二步与第三步中离子注入的N型杂质同时进行高温推结,对应形成发射极端的N型存储层41和集电极端的N型缓冲层42,如图2所示;Step 4: The N-type impurity ion-implanted in the second step and the third step are simultaneously subjected to high-temperature push junction, correspondingly forming the N-type storage layer 41 at the emitter end and the N-type buffer layer 42 at the collector end, as shown in FIG. 2 Show;
第五步:通过离子注入技术,在所述N型漂移区3具有所述N型存储层41的一端注入P型杂质;Step 5: Implanting P-type impurities into the end of the N-type drift region 3 having the N-type storage layer 41 by ion implantation technology;
第六步:通过离子注入技术,在所述N型缓冲层42上方注入P型杂质;Step 6: Implanting P-type impurities above the N-type buffer layer 42 by ion implantation technology;
第七步:将第五步和第六步中子注入的P型杂质同时进行高温推结,对应形成发射极端的P阱51和集电极端的P阱52,如图3所示;Step 7: Simultaneously push the P-type impurity implanted with neutrons in the fifth and sixth steps into a junction at high temperature, correspondingly forming a P-well 51 at the emitter end and a P-well 52 at the collector end, as shown in FIG. 3 ;
第八步:采用刻蚀工艺在所述N型漂移区3两端同时刻蚀多个深度超过所述P阱51和P阱52的深槽;然后采用氧化工艺在槽侧壁形成栅介质层,接着深槽中填充多晶硅材料、平坦化后反刻图形化,最后形成由槽栅介质层81和槽栅多晶硅82组成的间断或互连的发射极控制槽栅,由槽栅介质层83和槽栅多晶硅84组成的发射极阻挡槽栅,由槽栅介质层91和槽栅多晶硅92组成的集电极阻挡槽栅,由槽栅介质层93和槽栅多晶硅94组成的间断或互连的集电极槽栅;其中所述发射极控制槽栅的刻蚀窗口位于所述N型存储层41的注入窗口之间,如图4所示;Step 8: using an etching process to simultaneously etch multiple deep grooves at both ends of the N-type drift region 3 that are deeper than the P well 51 and the P well 52; and then using an oxidation process to form a gate dielectric layer on the side walls of the groove , followed by filling the deep groove with polysilicon material, planarization, and reverse patterning, and finally forming an interrupted or interconnected emitter control groove gate composed of the groove gate dielectric layer 81 and the groove gate polysilicon 82, consisting of the groove gate dielectric layer 83 and the groove gate dielectric layer 83. The emitter blocking groove gate composed of the groove gate polysilicon 84, the collector blocking groove gate composed of the groove gate dielectric layer 91 and the groove gate polysilicon 92, the discontinuous or interconnected collection composed of the groove gate dielectric layer 93 and the groove gate polysilicon 94 An electrode groove gate; wherein the etching window of the emitter control groove gate is located between the injection windows of the N-type storage layer 41, as shown in FIG. 4 ;
第九步:通过离子注入P型杂质在所述N型缓冲层42上部形成P+集电区62,所述槽栅介质91在靠近发射极的一侧与所述P+集电区62接触,如图5所示;Step 9: Form a P+ collector region 62 on the upper part of the N-type buffer layer 42 by ion implanting P-type impurities, and the groove gate dielectric 91 is in contact with the P+ collector region 62 on the side close to the emitter, as As shown in Figure 5;
第十步:通过离子注入N型杂质以同时图形化形成在所述P阱51上部的N+发射区71和在所述P阱52上部的N+集电区72,其中所述槽栅介质层81与所述N+发射区71接触,所述槽栅介质层93与所述N+集电区72接触,所述槽栅介质层91在远离发射极端与所述N+集电区72接触;Step 10: Implanting N-type impurities by ion implantation to simultaneously pattern the N+ emitter region 71 on the upper part of the P well 51 and the N+ collector region 72 on the upper part of the P well 52, wherein the trench gate dielectric layer 81 In contact with the N+ emitter region 71, the groove gate dielectric layer 93 is in contact with the N+ collector region 72, and the groove gate dielectric layer 91 is in contact with the N+ collector region 72 at the end far away from the emitter;
第十一步:通过离子注入P型杂质以同时图形化形成在所述P阱51上部的体接触P+区61与在所述P阱52上部的体接触P+区63,所述接触P+区61与所述N+发射区71接触,所述体接触P+区63与所述N+集电区72接触,所述槽栅介质层83在远离集电极端与所述接触P+区61接触,如图6所示;The eleventh step: by ion implanting P-type impurities to simultaneously pattern the body contact P+ region 61 formed on the upper part of the P well 51 and the body contact P+ region 63 on the upper part of the P well 52, the contact P+ region 61 In contact with the N+ emitter region 71, the body contact P+ region 63 is in contact with the N+ collector region 72, and the groove gate dielectric layer 83 is in contact with the contact P+ region 61 at the end far away from the collector, as shown in Figure 6 shown;
第十二步:在所述体接触P+区61、所述N+发射区71与槽栅多晶硅84的上表面形成发射极金属,在所述P+集电区62、体接触P+区63、N+集电区72、槽栅多晶硅92与槽栅多晶硅94的上表面形成集电极金属,在所述槽栅多晶硅82的上表面形成栅极金属,如图7所示;The twelfth step: form an emitter metal on the upper surface of the body contact P+ region 61, the N+ emitter region 71 and the groove gate polysilicon 84, and form an emitter metal on the P+ collector region 62, body contact P+ region 63, N+ collector The collector metal is formed on the upper surface of the electrical region 72, the trench gate polysilicon 92 and the trench gate polysilicon 94, and the gate metal is formed on the upper surface of the trench gate polysilicon 82, as shown in FIG. 7;
本例的工作原理为:This example works as follows:
在工艺制备方面,新器件发射极端与集电极端的槽栅结构同步制作完成,N型存储层41与N型缓冲层42、P阱区51与P阱区52可分别同步推结完成以降低器件热预算成本。新器件正向导通时,N+集电极区72被P阱区52与集电极槽栅结构包围,集电极槽栅中槽栅多晶硅层92与集电极短接,集电极槽栅沟道关断,对应N+集电极区72与N型缓冲层42的通路被阻断,因此新器件正向导通时消除snapback效应。阻挡槽栅和控制槽栅起到物理阻挡作用,而槽栅之间的N型存储层41可作为空穴势垒,均能防止空穴通过发射极端P阱区51被P+体接触区61快速抽走,有利于提高漂移区载流子浓度,同时分段式控制槽栅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。区别于传统平面栅结构LIGBT,新结构发射极端采用槽栅结构,仅有少部分空穴电流流经N+集电极区72下方,因而可大幅提升器件抗闩锁能力。器件关断过程中,随着集电极电压上升,集电极槽栅侧壁沟道会逐步开启,经N型缓冲层42-集电极槽栅侧壁沟道-N+集电极区72的快速抽取电子路径开启,同时阻挡槽栅与P+体接触区61接触而形成有空穴旁路,二者均能加速器件关断而降低Eoff。器件关断状态下,集电极槽栅与集电极短接处于高电位,集电极槽栅侧壁沟道开启,N+集电极区72与N型缓冲层42等效连通而几乎等电位,使得新器件结构具有类MOS单极击穿模式,降低了P+集电极区62对器件耐压的影响。In terms of process preparation, the groove gate structure of the emitter terminal and the collector terminal of the new device is produced synchronously, and the N-type storage layer 41 and N-type buffer layer 42, and the P-well region 51 and P-well region 52 can be respectively pushed and completed synchronously to reduce Device thermal budget cost. When the new device is forward-conducting, the N+ collector region 72 is surrounded by the P well region 52 and the collector groove gate structure, the groove gate polysilicon layer 92 in the collector groove gate is short-circuited with the collector, and the collector groove gate channel is turned off. The path corresponding to the N+ collector region 72 and the N-type buffer layer 42 is blocked, so the snapback effect is eliminated when the new device is conducting forward. The blocking groove gate and the control groove gate play a physical blocking role, and the N-type storage layer 41 between the groove gates can be used as a hole barrier, which can prevent holes from passing through the P well region 51 at the emitter end and being rapidly absorbed by the P+ body contact region 61. Pumping away is beneficial to increase the carrier concentration in the drift region. At the same time, the segmented control of the trench gate can increase the channel density of the device to reduce the resistance of the channel region. Under the combined effect, the V on of the device can be significantly reduced. Different from the traditional planar gate structure LIGBT, the emitter of the new structure adopts a trench gate structure, and only a small part of the hole current flows under the N+ collector region 72, thus greatly improving the anti-latch-up capability of the device. During the shutdown process of the device, as the collector voltage rises, the channel on the sidewall of the collector groove gate will gradually open, and the electrons will be quickly extracted through the N-type buffer layer 42-the sidewall channel of the collector groove gate-N+collector region 72 The path is opened, and at the same time, a hole bypass is formed by blocking the groove gate from contacting the P+ body contact region 61 , both of which can accelerate device turn-off and reduce E off . In the off state of the device, the short-circuit between the collector slot gate and the collector is at a high potential, the channel on the side wall of the collector slot gate is opened, and the N+ collector region 72 is equivalently connected to the N-type buffer layer 42 and is almost equipotential, so that the new The device structure has a MOS-like unipolar breakdown mode, which reduces the influence of the P+ collector region 62 on the withstand voltage of the device.
本发明的有益效果为,相对于传统短路阳极-LIGBT结构,新结构在发射极端与集电极端的工艺步骤兼容性高,导通时不仅有效消除snapback现象,还增强器件发射极端载流子注入效率与抗闩锁能力,并实现更快的关断速度与更低的关断损耗。The beneficial effect of the present invention is that, compared with the traditional short-circuited anode-LIGBT structure, the new structure has high compatibility between the process steps of the emitter terminal and the collector terminal, and not only effectively eliminates the snapback phenomenon when it is turned on, but also enhances carrier injection at the emitter terminal of the device Efficiency and anti-latch-up ability, and achieve faster turn-off speed and lower turn-off loss.
实施例2Example 2
如图8所示,本例与实施例1中图4的区别在于,本例在第八步中发射极端控制槽栅与阻挡槽栅底部离子注入形成P型埋层53。本实施例中器件关断工作机理和实施例1保持一致,区别在于:正向导通时,本例中引入的P型埋层53可辅助耗尽N型存储层41,从而提高N型存储层41优化掺杂浓度并增强载流子存储效果,因此本例中器件漂移区内载流子浓度更高,导通压降可进一步降低;同时,阻断状态下,P型埋层53亦可降低发射极端槽栅结构底部的电场尖峰,提高器件的可靠性。因此,与实施例1相比,本例中新器件能获得更低正向导通压降,并提高发射极端槽栅结构的可靠性。As shown in FIG. 8 , the difference between this example and FIG. 4 in Example 1 is that in this example, in the eighth step, ion implantation at the bottom of the emitter-side control slot gate and the blocking slot gate forms a P-type buried layer 53 . The working mechanism of device shutdown in this embodiment is consistent with that of Embodiment 1, the difference is that: when conducting forward conduction, the P-type buried layer 53 introduced in this example can assist in depleting the N-type storage layer 41, thereby improving the efficiency of the N-type storage layer. 41 Optimize the doping concentration and enhance the carrier storage effect, so in this example, the carrier concentration in the drift region of the device is higher, and the conduction voltage drop can be further reduced; at the same time, in the blocking state, the P-type buried layer 53 can also The electric field peak at the bottom of the emitter groove gate structure is reduced, and the reliability of the device is improved. Therefore, compared with Example 1, the new device in this example can obtain a lower forward conduction voltage drop and improve the reliability of the trench gate structure at the emitter terminal.
实施例3Example 3
如图9与图10所示,本例与实施例1中图7的区别在于,发射极控制槽栅与集电极槽栅的版图布局可为矩形或六边形的间断式分布;图11示意了发射极控制槽栅和集电极槽栅分别以矩形版图分布互连,当然发射极控制槽栅、集电极槽栅也可以六边形版图分布互连。本实施例中器件关断工作机理和实施例1保持一致,区别在于:不同槽栅的形状可以改变器件沟道密度大小,有利设计器件的导通压降与关断损耗。As shown in Figures 9 and 10, the difference between this example and Figure 7 in Embodiment 1 is that the layout of the emitter control slots and the collector slots can be a rectangular or hexagonal discontinuous distribution; Figure 11 shows The emitter control slots and the collector slots are respectively interconnected in a rectangular layout, and of course the emitter control slots and the collector slots may also be interconnected in a hexagonal layout. The device turn-off working mechanism in this embodiment is the same as that in Embodiment 1, the difference is that the shape of the groove gate can change the channel density of the device, which is beneficial to design the turn-on voltage drop and turn-off loss of the device.
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