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CN107170816B - A kind of landscape insulation bar double-pole-type transistor - Google Patents

A kind of landscape insulation bar double-pole-type transistor Download PDF

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CN107170816B
CN107170816B CN201710328737.XA CN201710328737A CN107170816B CN 107170816 B CN107170816 B CN 107170816B CN 201710328737 A CN201710328737 A CN 201710328737A CN 107170816 B CN107170816 B CN 107170816B
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polysilicon
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dielectric layer
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CN107170816A (en
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张金平
陈钱
刘竞秀
李泽宏
任敏
张波
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University of Electronic Science and Technology of China
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D12/00Bipolar devices controlled by the field effect, e.g. insulated-gate bipolar transistors [IGBT]
    • H10D12/411Insulated-gate bipolar transistors [IGBT]
    • H10D12/421Insulated-gate bipolar transistors [IGBT] on insulating layers or insulating substrates, e.g. thin-film IGBTs
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D84/00Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
    • H10D84/80Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers characterised by the integration of at least one component covered by groups H10D12/00 or H10D30/00, e.g. integration of IGFETs
    • H10D84/811Combinations of field-effect devices and one or more diodes, capacitors or resistors

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Abstract

The invention belongs to semiconductor power device technology fields, particularly relate to a kind of landscape insulation bar double-pole-type transistor.The present invention is by forming three-dimensional structure along orientation etching groove in device surface, forming the landscape insulation bar double-pole-type transistor with three-dimensional structure on the basis of traditional landscape insulation bar double-pole-type transistor;Polycrystalline diode is formed on device three-dimensional drift region surface simultaneously and three-dimensional PMOS and Zener diode are integrated near collector.Structure of the invention has forward conduction voltage drop more lower than traditional LIGBT and negative resistance phenomenon is not present in turn on process, while having higher device electric breakdown strength, faster turn-off speed and lower turn-off power loss.

Description

一种横向绝缘栅双极型晶体管A Lateral Insulated Gate Bipolar Transistor

技术领域technical field

本发明属于半导体功率器件技术领域,具体的说是涉及一种横向绝缘栅双极型晶体管。The invention belongs to the technical field of semiconductor power devices, and in particular relates to a lateral insulated gate bipolar transistor.

背景技术Background technique

绝缘栅双极型晶体管(IGBT)是一种MOS场效应和双极型晶体管复合的新型电力电子器件,它既有MOSFET易于驱动,控制简单的优点,又有功率晶体管导通压降低,通态电流大,损耗小的优点,已成为中高功率电力电子领域的主流功率开关器件,广泛应用在诸如通信、能源、交通、工业、医学、家用电器及航空航天等国民经济的各个领域。国际知名半导体公司,如ABB,Infineon(IR),ST,Renesas,Mitsubishi,FuJi等相继投入到IGBT的研发和制造中。近年来,作为功率电子学的热点领域,IGBT更是获得了美国、日本和欧洲等发达国家和地区的高度重视。Insulated gate bipolar transistor (IGBT) is a new type of power electronic device combined with MOS field effect and bipolar transistor. The advantages of large current and low loss have become the mainstream power switching devices in the field of medium and high power power electronics, and are widely used in various fields of the national economy such as communications, energy, transportation, industry, medicine, household appliances, and aerospace. Internationally well-known semiconductor companies, such as ABB, Infineon (IR), ST, Renesas, Mitsubishi, FuJi, etc. have successively invested in the R&D and manufacturing of IGBTs. In recent years, as a hot field of power electronics, IGBT has received great attention from developed countries and regions such as the United States, Japan and Europe.

IGBT在导通过程中,电子经过MOS沟道进入N型漂移区中,从而引起P型集电区向漂移区注入大量的空穴。因此,处于开态的IGBT漂移区中存储有大量的过剩电子-空穴对,这些电子-空穴对形成电导调制效应,极大地降低了漂移区电阻,从而降低正向导通压降VCE。实际应用中,为减小开态损耗,总是希望VCE越低越好。但VCE越低意味着电导调制效应越强烈,漂移区中过剩的电子-空穴对越多,这些大量的电子-空穴对在IGBT关断过程中需要被全部抽取和复合,从而导致关断损耗EOFF增加。VCE与EOFF是IGBT的一组重要的折中关系,它直接关系到开态损耗与关断损耗的大小。IGBT每一代产品的更迭,其中都包含对该折中关系的优化。During the conduction process of the IGBT, electrons enter the N-type drift region through the MOS channel, which causes the P-type collector region to inject a large number of holes into the drift region. Therefore, a large number of excess electron-hole pairs are stored in the drift region of the IGBT in the on state, and these electron-hole pairs form a conductance modulation effect, which greatly reduces the resistance of the drift region, thereby reducing the forward voltage drop VCE. In practical applications, in order to reduce the on-state loss, it is always hoped that the lower the VCE, the better. However, the lower the VCE, the stronger the conductance modulation effect, and the more excess electron-hole pairs in the drift region. These large numbers of electron-hole pairs need to be fully extracted and recombined during the turn-off process of the IGBT, resulting in turn-off The loss EOFF increases. VCE and EOFF are a set of important compromise relations of IGBT, which are directly related to the size of on-state loss and turn-off loss. The change of each generation of IGBT products includes the optimization of this compromise relationship.

目前,横向功率器件广泛采用绝缘层上硅(SOI)技术,以减小寄生电容、抑制衬底电流、消除衬底引起的闩锁效应等。其典型的制备工艺包括注氧隔离SIMOX技术、键合技术以及Smart-Cut技术等。横向IGBT(LIGBT)由于栅驱动功率小、电流处理能力强、易于集成的优点,广泛应用于功率集成IC(PICs)以及智能功率IC中,其基本结构如图1所示。由于关断过程需要抽取漂移区中的过剩载流子,导致其关断时间较长,关断损耗较大,限制了LIGBT在高频领域的应用。为改善LIGBT的VCE-EOFF折中关系,最有效的方法是在关断过程中增加电子抽取通路,以减小电流的下降时间,典型结构为阳极短路(SA-LIGBT)结构,如图2所示。然而,该结构在正向导通时,电子通过N+发射区5、P型体区4的表面沟道、低掺杂N型漂移区3、集电极N+区8到达集电极,形成寄生MOS结构,产生电子电流通路,会导致导通曲线呈现负阻现象,并减弱漂移区的电导调制效应,增大正向导通压降,不利于器件的实际应用。At present, silicon-on-insulator (SOI) technology is widely used in lateral power devices to reduce parasitic capacitance, suppress substrate current, and eliminate latch-up effects caused by the substrate. Its typical preparation process includes oxygen injection isolation SIMOX technology, bonding technology and Smart-Cut technology, etc. Lateral IGBT (LIGBT) is widely used in power integrated ICs (PICs) and smart power ICs due to its advantages of low gate drive power, strong current handling capability, and easy integration. Its basic structure is shown in Figure 1. Due to the need to extract excess carriers in the drift region during the turn-off process, the turn-off time is longer and the turn-off loss is larger, which limits the application of LIGBT in the high-frequency field. In order to improve the VCE-EOFF trade-off relationship of LIGBT, the most effective method is to increase the electron extraction path during the turn-off process to reduce the falling time of the current. The typical structure is the anode short circuit (SA-LIGBT) structure, as shown in Figure 2 Show. However, when the structure is in forward conduction, electrons reach the collector through the N+ emitter region 5, the surface channel of the P-type body region 4, the low-doped N-type drift region 3, and the collector N+ region 8, forming a parasitic MOS structure. The generation of an electronic current path will cause the conduction curve to show a negative resistance phenomenon, weaken the conductance modulation effect in the drift region, and increase the forward conduction voltage drop, which is not conducive to the practical application of the device.

发明内容SUMMARY OF THE INVENTION

本发明的目的在于提供一种高速低损耗的横向绝缘栅双极型晶体管。本发明结构通过在传统横向绝缘栅双极型晶体管的基础上,在器件表面沿沟道长度方向刻蚀沟槽形成三维结构,形成具有三维结构的横向绝缘栅双极型晶体管;在器件三维漂移区表面形成多晶二极管并在集电极附近集成三维PMOS和齐纳二极管。在阻断状态下,通过器件表面三维多晶二极管反偏状态下漂移区耗尽提供的电荷和三维场板作用,在提高LIGBT器件漂移区掺杂浓度的同时可获得比传统LIGBT结构更高的耐压;在器件关断过程中,随着集电极电压的增加,利用集电极电压的变化以及表面多晶二极管和齐纳二极管形成的自偏置效应使集电极附近的PMOS自动开启并导通,在集电极端形成电子电流通路,加快LIGBT内部的载流子抽取,同时三维多晶二极管漂移区耗尽提供的电荷和三维场板作用加快器件漂移区耗尽层在垂直于沟道长度方向的扩展,进一步加快LIGBT器件内部的载流子抽取,从而提高器件的关断速度,进一步降低器件的关断损耗;在导通状态下,集电极电压较低,表面多晶二极管和齐纳二极管(或二极管串)形成的自偏置效应使集电极附近的PMOS处于关断状态,电子电流通路被截断,附加结构的存在不会影响器件的正向导通特性,在导通过程中不存在负阻现象,同时三维三栅结构增加了栅结构的等效宽度,进一步减小了器件的正向导通压降。因此,本发明结构具有比传统LIGBT更低的正向导通压降并在导通过程中不存在负阻现象,同时具有更高的器件击穿电压,更快的关断速度和更低的关断损耗。本发明结构不仅适用于N型LIGBT器件,也适用于P型LIGBT器件,仅需将结构中材料的掺杂类型进行N和P的互换。为了描述方便以下仅以N型LIGBT器件为例来说明。The purpose of the present invention is to provide a high-speed and low-loss lateral insulated gate bipolar transistor. The structure of the present invention forms a three-dimensional structure by etching grooves on the surface of the device along the channel length direction on the basis of the traditional lateral insulated gate bipolar transistor, and forms a lateral insulated gate bipolar transistor with a three-dimensional structure; A polycrystalline diode is formed on the surface of the region and a three-dimensional PMOS and Zener diode are integrated near the collector. In the blocking state, the charge and the three-dimensional field plate provided by the depletion of the drift region in the reverse-biased state of the three-dimensional polycrystalline diode on the surface of the device can increase the doping concentration of the drift region of the LIGBT device and obtain a higher density than the traditional LIGBT structure. Withstand voltage; in the process of turning off the device, as the collector voltage increases, the PMOS near the collector is automatically turned on and turned on by using the change of the collector voltage and the self-bias effect formed by the surface polycrystalline diode and the Zener diode , forming an electron current path at the collector terminal, speeding up the carrier extraction inside the LIGBT, and at the same time, the charge provided by the depletion of the drift region of the three-dimensional polycrystalline diode and the effect of the three-dimensional field plate accelerate the depletion layer in the drift region of the device in the direction perpendicular to the channel length The expansion of LIGBT further accelerates the carrier extraction inside the LIGBT device, thereby increasing the turn-off speed of the device and further reducing the turn-off loss of the device; in the on-state, the collector voltage is low, and the surface polycrystalline diode and Zener diode The self-bias effect formed by the collector (or diode string) makes the PMOS near the collector in the off state, and the electronic current path is cut off. The existence of the additional structure will not affect the forward conduction characteristics of the device, and there is no negative conduction during the conduction process. At the same time, the three-dimensional tri-gate structure increases the equivalent width of the gate structure, further reducing the forward conduction voltage drop of the device. Therefore, the structure of the present invention has lower forward conduction voltage drop than traditional LIGBT and does not have negative resistance phenomenon in the conduction process, and has higher device breakdown voltage, faster turn-off speed and lower turn-off break loss. The structure of the present invention is applicable not only to N-type LIGBT devices, but also to P-type LIGBT devices, and it is only necessary to exchange the doping types of materials in the structure between N and P. For the convenience of description, only an N-type LIGBT device is used as an example for illustration below.

本发明的技术方案是:如图3所示,一种横向绝缘栅双极型晶体管,其半元胞结构包括从下至上依次层叠设置的衬底1、绝缘层2和第一N型低掺杂区3;其特征在于,沿器件纵向方向,所述第一N型低掺杂区3为二级阶梯状,定义第二级阶梯的垂直高度大于第一级阶梯,所述第一N型低掺杂区3上层两侧分别具有P型体区4和N型缓冲区7,沿器件纵向方向,所述P型体区4和N型缓冲区7均为二级阶梯状;在第一N型低掺杂区3第二级阶梯和P型体区4及N型缓冲区7第二级阶梯之间具有第二N型低掺杂区150;所述P型体区4上层具有相互并列设置的P+接触区6和N+发射区5,其中N+发射区5位于靠近N型缓冲区7的一侧,所述P+接触区6和N+发射区5均为二级阶梯状;所述P+接触区6和部分N+发射区5上表面具有发射极金属电极130,所述发射极金属电极130为二级阶梯状;所述P型体区4上表面具有第一栅极结构,所述第一栅极结构由第一栅介质层110和位于第一栅介质层110上表面的第一多晶硅栅电极120构成,沿器件纵向方向,所述第一栅介质层110的下表面依次与第一N型低掺杂区3第一阶梯的上表面和第二N型低掺杂区150的上表面和侧面接触,第一栅介质层110的下表面还与部分N+发射区5的上表面接触,第一多晶硅栅电极120的上表面是水平面或二级阶梯状;所述N型缓冲区7中具有P型集电区8、高掺杂N+区9和高掺杂P+区10,高掺杂N+区9和高掺杂P+区10相互接触且高掺杂N+区9位于靠近P型体区4的一侧;所述P型集电区8、高掺杂N+区9和高掺杂P+区10均为二级阶梯状;所述P型集电区8上表面远离P型体区4一侧具有集电极金属电极131,所述集电极金属电极131为二级阶梯状;所述高掺杂N+区9和高掺杂P+区10的上表面具有金属电极132,所述金属电极132为二级阶梯状;所述N型缓冲区7的上表面具有第二栅极结构,所述第二栅极结构由第二栅介质层111和位于第二栅介质层111上表面的第二多晶硅电极124构成,沿器件纵向方向,所述第二栅介质层111的下表面依次与第一N型低掺杂区3第一阶梯的上表面和第二N型低掺杂区150的上表面和侧面接触,第二栅介质层111的下表面还与部分P型集电区8和高掺杂P+区10的上表面接触,第二多晶硅电极124的上表面是水平面或二级阶梯状;在所述P型体区4和N型缓冲区7之间的器件上表面具有介质层112,沿器件纵向方向,所述介质层112的下表面依次与第一N型低掺杂区3第一阶梯的上表面和第二N型低掺杂区150的上表面接触,所述介质层112的下表面还与部分N型缓冲区7的上表面接触;所述介质层112上表面具有多晶硅P+区121、P型区122和N+区123,其中P型区122位于多晶硅P+区121和N+区123之间并相互连接形成多晶硅二极管,P+区121位于靠近P型体区4的一侧,N+区123位于靠近N型缓冲区7一侧,沿器件纵向方向,多晶硅P+区121、P型区122和N+区123的上表面是水平面或二级阶梯状;所述发射极金属电极130与多晶硅P+区121之间电气连接,所述多晶硅N+区123与第二多晶硅电极124之间电气连接并且所述多晶硅N+区123与第二多晶硅电极124通过齐纳二极管140与集电极金属131之间电气连接,其中齐纳二极管140的阴极接集电极金属131,齐纳二极管140的阳极接多晶硅N+区123与第二多晶硅电极124。The technical solution of the present invention is: as shown in FIG. 3 , a lateral insulated gate bipolar transistor, its half-cell structure includes a substrate 1, an insulating layer 2 and a first N-type low-doped transistor stacked sequentially from bottom to top. The impurity region 3; it is characterized in that, along the longitudinal direction of the device, the first N-type low-doped region 3 is in the shape of two steps, and the vertical height of the second step is defined to be greater than that of the first step, and the first N-type There are P-type body regions 4 and N-type buffer regions 7 on both sides of the upper layer of the low-doped region 3, and along the longitudinal direction of the device, the P-type body regions 4 and N-type buffer regions 7 are in the shape of two steps; There is a second N-type low-doped region 150 between the second step of the N-type low-doped region 3 and the second step of the P-type body region 4 and the N-type buffer zone 7; the upper layer of the P-type body region 4 has mutual The P+ contact area 6 and the N+ emission area 5 arranged side by side, wherein the N+ emission area 5 is located on the side close to the N-type buffer zone 7, and the P+ contact area 6 and the N+ emission area 5 are both in the shape of two steps; the P+ The upper surface of the contact region 6 and part of the N+ emitter region 5 has an emitter metal electrode 130, and the emitter metal electrode 130 is in the shape of two steps; the upper surface of the P-type body region 4 has a first gate structure, and the first A gate structure is composed of a first gate dielectric layer 110 and a first polysilicon gate electrode 120 located on the upper surface of the first gate dielectric layer 110. Along the longitudinal direction of the device, the lower surface of the first gate dielectric layer 110 is sequentially connected to the The upper surface of the first step of the first N-type low-doped region 3 is in contact with the upper surface and side surfaces of the second N-type low-doped region 150, and the lower surface of the first gate dielectric layer 110 is also in contact with the upper surface of part of the N+ emitter region 5. Surface contact, the upper surface of the first polysilicon gate electrode 120 is a horizontal plane or two-level ladder shape; the N-type buffer zone 7 has a P-type collector region 8, a highly doped N+ region 9 and a highly doped P+ region 10. The highly doped N+ region 9 and the highly doped P+ region 10 are in contact with each other, and the highly doped N+ region 9 is located on the side close to the P-type body region 4; the P-type collector region 8, the highly doped N+ region 9 and the highly doped P+ region 10 are both in the shape of two steps; the upper surface of the P-type collector region 8 has a collector metal electrode 131 on the side away from the P-type body region 4, and the collector metal electrode 131 is a two-step step shape; the upper surface of the highly doped N+ region 9 and the highly doped P+ region 10 has a metal electrode 132, and the metal electrode 132 is in a two-level ladder shape; the upper surface of the N-type buffer zone 7 has a second gate Pole structure, the second gate structure is composed of a second gate dielectric layer 111 and a second polysilicon electrode 124 located on the upper surface of the second gate dielectric layer 111, along the longitudinal direction of the device, the second gate dielectric layer 111 The lower surface of the second gate dielectric layer 111 is in contact with the upper surface of the first step of the first N-type low-doped region 3 and the upper surface and side surfaces of the second N-type low-doped region 150 in turn, and the lower surface of the second gate dielectric layer 111 is also in contact with the portion P type collector region 8 is in contact with the upper surface of the highly doped P+ region 10, and the upper surface of the second polysilicon electrode 124 is a horizontal plane or a two-level ladder shape; between the P type body region 4 and the N type buffer region 7 The upper surface of the device between has a dielectric layer 112, along the longitudinal direction of the device, the dielectric layer 1 The lower surface of 12 is sequentially in contact with the upper surface of the first step of the first N-type low-doped region 3 and the upper surface of the second N-type low-doped region 150, and the lower surface of the dielectric layer 112 is also in contact with part of the N-type buffer The upper surface of the region 7 is in contact; the upper surface of the dielectric layer 112 has a polysilicon P+ region 121, a P-type region 122 and an N+ region 123, wherein the P-type region 122 is located between the polysilicon P+ region 121 and the N+ region 123 and is connected to each other to form a polysilicon In the diode, the P+ region 121 is located on the side close to the P-type body region 4, and the N+ region 123 is located on the side close to the N-type buffer zone 7. Along the longitudinal direction of the device, the upper surfaces of the polysilicon P+ region 121, the P-type region 122 and the N+ region 123 It is a horizontal plane or a two-level ladder shape; the emitter metal electrode 130 is electrically connected to the polysilicon P+ region 121, the polysilicon N+ region 123 is electrically connected to the second polysilicon electrode 124, and the polysilicon N+ region 123 It is electrically connected with the second polysilicon electrode 124 through the Zener diode 140 and the collector metal 131, wherein the cathode of the Zener diode 140 is connected to the collector metal 131, and the anode of the Zener diode 140 is connected to the polysilicon N+ region 123 and the second polysilicon electrode 124 .

上述方案为本发明总的技术方案,上述方案中所述的器件纵向方向对应如图中所示三维直角坐标系中的Y轴方向,器件横向方向对应X轴方向,在器件俯视图中,X轴和Y轴在同一水平面且相互垂直,器件垂直方向对应Z轴方向。The above scheme is the general technical scheme of the present invention. The longitudinal direction of the device described in the above scheme corresponds to the Y-axis direction in the three-dimensional rectangular coordinate system shown in the figure, and the transverse direction of the device corresponds to the X-axis direction. In the top view of the device, the X-axis It is on the same horizontal plane as the Y axis and perpendicular to each other, and the vertical direction of the device corresponds to the direction of the Z axis.

进一步的,所述第二N型低掺杂区150的掺杂浓度等于或大于第一N型低掺杂区3的掺杂浓度。Further, the doping concentration of the second N-type low-doped region 150 is equal to or greater than the doping concentration of the first N-type low-doped region 3 .

进一步的,所述齐纳二极管集成在介质层112上方靠近集电极金属电极131一侧,相应的集电极金属电极131延伸至与介质层112侧面接触并覆盖部分齐纳二极管上表面。Further, the Zener diode is integrated on the side of the dielectric layer 112 close to the collector metal electrode 131 , and the corresponding collector metal electrode 131 extends to contact with the side of the dielectric layer 112 and cover part of the upper surface of the Zener diode.

进一步的,所述齐纳二极管由多个串联的二极管所取代,二极管串的阳极接集电极金属131,阴极接多晶硅高掺杂N+区123与多晶硅电极124,并且二极管串的开启电压值大于PMOS的阈值电压绝对值。Further, the Zener diode is replaced by a plurality of diodes connected in series, the anode of the diode string is connected to the collector metal 131, the cathode is connected to the polysilicon highly doped N+ region 123 and the polysilicon electrode 124, and the turn-on voltage value of the diode string is greater than that of the PMOS The absolute value of the threshold voltage.

进一步的,上述方案中,如图11所示,所述多晶硅P+区121和多晶硅N+区123之间还具有电容151。所述电容可以通过表面布线时由多晶硅电极124和发射极金属电极130之间形成的寄生电容形成,也可通过在N型低掺杂漂移区3中或表面布线的多晶硅层和或金属层中通过集成电容形成。Further, in the above solution, as shown in FIG. 11 , there is a capacitor 151 between the polysilicon P+ region 121 and the polysilicon N+ region 123 . The capacitance can be formed by the parasitic capacitance formed between the polysilicon electrode 124 and the emitter metal electrode 130 during surface wiring, or can be formed in the N-type low-doped drift region 3 or in the polysilicon layer and or metal layer of the surface wiring. Formed by integrating capacitors.

在本发明的方案中,多晶硅P型区122还可以采用N型材料;栅介质层110,介质层111和介质层112的厚度和材料可以相同也可以不同,所用的材料可以是二氧化硅(SiO2),也可以是三氧化二铝(Al2O3),二氧化铪(HfO2)或者氮化硅(Si3N4)等高K材料;器件所用半导体材料可采用硅(Si)、碳化硅(SiC)、砷化镓(GaAs)或者氮化镓(GaN)等予以实现。In the solution of the present invention, polysilicon P-type region 122 can also adopt N-type material; Gate dielectric layer 110, the thickness and material of dielectric layer 111 and dielectric layer 112 can be identical or can be different, and used material can be silicon dioxide ( SiO 2 ), can also be high-K materials such as aluminum oxide (Al 2 O 3 ), hafnium dioxide ( Hf O 2 ) or silicon nitride (Si 3 N 4 ); the semiconductor material used in the device can be silicon ( Si), silicon carbide (SiC), gallium arsenide (GaAs) or gallium nitride (GaN).

本发明的有益效果是:在导通状态下,本发明结构具有比传统LIGBT更低的导通压降并且在导通过程中不存在负阻现象;在阻断状态下,具有更高的击穿电压;同时在关断过程中,具有更快的关断速度和更低的关断损耗。The beneficial effects of the present invention are: in the conduction state, the structure of the present invention has a lower turn-on voltage drop than the traditional LIGBT and there is no negative resistance phenomenon in the conduction process; in the block state, it has higher breakdown voltage; at the same time, in the turn-off process, it has faster turn-off speed and lower turn-off loss.

附图说明Description of drawings

图1是传统的横向绝缘栅双极型晶体管示意图;FIG. 1 is a schematic diagram of a traditional lateral insulated gate bipolar transistor;

图2是传统的阳极短路横向绝缘栅双极型晶体管示意图;FIG. 2 is a schematic diagram of a conventional anode short-circuited lateral insulated gate bipolar transistor;

图3是实施例1的晶体管半元胞三维结构示意图;3 is a schematic diagram of the three-dimensional structure of the transistor half-cell of Embodiment 1;

图4是图3结构沿AA’线的剖面示意图;Fig. 4 is the schematic sectional view of Fig. 3 structure along AA ' line;

图5是图3结构沿BB’线的剖面示意图;Fig. 5 is the schematic sectional view of Fig. 3 structure along BB ' line;

图6是图3结构沿CC’线的剖面示意图;Fig. 6 is the schematic sectional view of Fig. 3 structure along CC ' line;

图7是图3结构沿DD’线的剖面示意;。Fig. 7 is a schematic cross-sectional view of the structure of Fig. 3 along the DD' line;

图8是图3结构沿EE’线的剖面示意图;Fig. 8 is the schematic sectional view of Fig. 3 structure along EE ' line;

图9是实施例2晶体管半元胞三维结构示意图;9 is a schematic diagram of a three-dimensional structure of a transistor half-cell in Embodiment 2;

图10是实施例3晶体管半元胞三维结构示意图;FIG. 10 is a schematic diagram of a three-dimensional structure of a transistor half cell in Embodiment 3;

图11是实施例4晶体管半元胞三维结构示意图;Fig. 11 is a schematic diagram of a three-dimensional structure of a transistor half cell in embodiment 4;

图12是实施例5晶体管制作方法基本工艺流程图;Fig. 12 is a basic process flow chart of the transistor manufacturing method in Embodiment 5;

图13是本发明提供的一种横向绝缘栅双极型晶体管制作方法外延生长形成N型低掺杂区150层后的结构示意图;Fig. 13 is a schematic diagram of the structure of a lateral insulated gate bipolar transistor manufacturing method provided by the present invention after epitaxial growth and formation of 150 layers of N-type low-doped regions;

图14是本发明提供的一种横向绝缘栅双极型晶体管制作方法通过刻蚀工艺在器件表面形成沿X方向的沟槽后的结构示意图;Fig. 14 is a structural schematic diagram of a lateral IGBT manufacturing method provided by the present invention after forming a trench along the X direction on the surface of the device through an etching process;

图15是本发明提供的一种横向绝缘栅双极型晶体管制作方法形成具有折叠结构的N型缓冲层7后的结构示意图;FIG. 15 is a structural schematic diagram after forming an N-type buffer layer 7 with a folded structure in a method for fabricating a lateral insulated gate bipolar transistor provided by the present invention;

图16是本发明提供的一种横向绝缘栅双极型晶体管制作方法形成介质层和多晶硅层后的结构示意图;Fig. 16 is a schematic diagram of the structure of a lateral insulated gate bipolar transistor manufacturing method provided by the present invention after forming a dielectric layer and a polysilicon layer;

图17是本发明提供的一种横向绝缘栅双极型晶体管制作方法完成各区离子注入和退火后的结构示意图;Fig. 17 is a structural schematic diagram after ion implantation and annealing in each region of a lateral insulated gate bipolar transistor manufacturing method provided by the present invention;

图18是本发明提供的一种横向绝缘栅双极型晶体管制作方法完成金属互联后的结构示意图;Fig. 18 is a structural schematic diagram of a method for manufacturing a lateral insulated gate bipolar transistor provided by the present invention after metal interconnection is completed;

图1-图17中:1为P型衬底、2为埋氧化层、3为低掺杂N型区、4为P型体区、5为N+发射区、6为高掺杂P+区、7为N型缓冲层、8为P型集电区、9为高掺杂N+区、10为P型区、110为栅介质层、111为第一介质层、112为第二介质层、120为栅电极、121为多晶硅P+区、122为多晶硅P型区、123为多晶硅N+区、124为多晶硅电极、125多晶硅P+区、126为多晶硅N+区、130为发射极金属电极、131为集电极金属电极、132为第一金属电极,140为齐纳二极管,150为低掺杂N型区,151为电容。In Figure 1-Figure 17: 1 is the P-type substrate, 2 is the buried oxide layer, 3 is the low-doped N-type region, 4 is the P-type body region, 5 is the N+ emitter region, 6 is the highly doped P+ region, 7 is an N-type buffer layer, 8 is a P-type collector region, 9 is a highly doped N+ region, 10 is a P-type region, 110 is a gate dielectric layer, 111 is a first dielectric layer, 112 is a second dielectric layer, 120 121 is the polysilicon P+ area, 122 is the polysilicon P-type area, 123 is the polysilicon N+ area, 124 is the polysilicon electrode, 125 is the polysilicon P+ area, 126 is the polysilicon N+ area, 130 is the emitter metal electrode, 131 is the collector A metal electrode, 132 is a first metal electrode, 140 is a Zener diode, 150 is a low-doped N-type region, and 151 is a capacitor.

具体实施方式Detailed ways

下面结合附图和实施例对本发明进行详细的描述。The present invention will be described in detail below in conjunction with the accompanying drawings and embodiments.

实施例1Example 1

如图3所示,为本例的结构示意图,其半元胞结构包括从下至上依次层叠设置的衬底1、绝缘层2和第一N型低掺杂区3;其特征在于,沿器件纵向方向,所述第一N型低掺杂区3为二级阶梯状,定义第二级阶梯的垂直高度大于第一级阶梯,所述第一N型低掺杂区3上层两侧分别具有P型体区4和N型缓冲区7,沿器件纵向方向,所述P型体区4和N型缓冲区7均为二级阶梯状;在第一N型低掺杂区3第二级阶梯和P型体区4及N型缓冲区7第二级阶梯之间具有第二N型低掺杂区150;所述P型体区4上层具有相互并列设置的P+接触区6和N+发射区5,其中N+发射区5位于靠近N型缓冲区7的一侧,所述P+接触区6和N+发射区5均为二级阶梯状;所述P+接触区6和部分N+发射区5上表面具有发射极金属电极130,所述发射极金属电极130为二级阶梯状;所述P型体区4上表面具有第一栅极结构,所述第一栅极结构由第一栅介质层110和位于第一栅介质层110上表面的第一多晶硅栅电极120构成,沿器件纵向方向,所述第一栅介质层110的下表面依次与第一N型低掺杂区3第一阶梯的上表面和第二N型低掺杂区150的上表面接触,第一栅介质层110的下表面还与部分N+发射区5的上表面接触,第一多晶硅栅电极120的上表面是水平面;所述N型缓冲区7中具有P型集电区8、高掺杂N+区9和高掺杂P+区10,高掺杂N+区9和高掺杂P+区10相互接触且高掺杂N+区9位于靠近P型体区4的一侧;所述P型集电区8、高掺杂N+区9和高掺杂P+区10均为二级阶梯状;所述P型集电区8上表面远离P型体区4一侧具有集电极金属电极131,所述集电极金属电极131为二级阶梯状;所述高掺杂N+区9和高掺杂P+区10的上表面具有金属电极132,所述金属电极132为二级阶梯状;所述N型缓冲区7的上表面具有第二栅极结构,所述第二栅极结构由第二栅介质层111和位于第二栅介质层111上表面的第二多晶硅电极124构成,沿器件纵向方向,所述第二栅介质层111的下表面依次与第一N型低掺杂区3第一阶梯的上表面和第二N型低掺杂区150的上表面接触,第二栅介质层111的下表面还与部分P型集电区8和高掺杂P+区10的上表面接触,第二多晶硅电极124的上表面是水平面;在所述P型体区4和N型缓冲区7之间的器件上表面具有介质层112,沿器件纵向方向,所述介质层112的下表面依次与第一N型低掺杂区3第一阶梯的上表面和第二N型低掺杂区150的上表面接触,所述介质层112的下表面还与部分N型缓冲区7的上表面接触;所述介质层112上表面具有多晶硅P+区121、P型区122和N+区123,其中P型区122位于多晶硅P+区121和N+区123之间并相互连接形成多晶硅二极管,P+区121位于靠近P型体区4的一侧,N+区123位于靠近N型缓冲区7一侧,沿器件纵向方向,多晶硅P+区121、P型区122和N+区123的上表面是水平面;所述发射极金属电极130与多晶硅P+区121之间电气连接,所述多晶硅N+区123与第二多晶硅电极124之间电气连接并且所述多晶硅N+区123与第二多晶硅电极124通过齐纳二极管140与集电极金属131之间电气连接,其中齐纳二极管140的阴极接集电极金属131,齐纳二极管140的阳极接多晶硅N+区123与第二多晶硅电极124。As shown in Figure 3, it is a schematic structural diagram of this example, and its semi-cellular structure includes a substrate 1, an insulating layer 2, and a first N-type low-doped region 3 that are stacked in sequence from bottom to top; it is characterized in that, along the device In the longitudinal direction, the first N-type low-doped region 3 is in the shape of a second step, defining the vertical height of the second step to be greater than the first step, and the two sides of the upper layer of the first N-type low-doped region 3 respectively have P-type body region 4 and N-type buffer region 7, along the longitudinal direction of the device, the P-type body region 4 and N-type buffer region 7 are two-level ladder; in the second level of the first N-type low-doped region 3 There is a second N-type low-doped region 150 between the ladder and the P-type body region 4 and the second-level step of the N-type buffer region 7; the upper layer of the P-type body region 4 has a P+ contact region 6 and an N+ emitter arranged side by side. region 5, wherein the N+ emitter region 5 is located on the side close to the N-type buffer zone 7, and the P+ contact region 6 and the N+ emitter region 5 are both in the shape of two steps; the P+ contact region 6 and part of the N+ emitter region 5 are There is an emitter metal electrode 130 on the surface, and the emitter metal electrode 130 is in the shape of two steps; the upper surface of the P-type body region 4 has a first gate structure, and the first gate structure is composed of a first gate dielectric layer 110 and the first polysilicon gate electrode 120 located on the upper surface of the first gate dielectric layer 110, along the longitudinal direction of the device, the lower surface of the first gate dielectric layer 110 is sequentially connected with the first N-type low-doped region 3 The upper surface of a step is in contact with the upper surface of the second N-type low-doped region 150, the lower surface of the first gate dielectric layer 110 is also in contact with the upper surface of part of the N+ emitter region 5, and the first polysilicon gate electrode 120 The upper surface is a horizontal plane; the N-type buffer zone 7 has a P-type collector region 8, a highly doped N+ region 9 and a highly doped P+ region 10, and the highly doped N+ region 9 and the highly doped P+ region 10 are in contact with each other And the highly doped N+ region 9 is located on the side close to the P-type body region 4; the P-type collector region 8, the highly doped N+ region 9 and the highly doped P+ region 10 are all in the shape of a two-level ladder; the P There is a collector metal electrode 131 on the upper surface of the P-type collector region 8 away from the P-type body region 4, and the collector metal electrode 131 is in the shape of a two-level ladder; the highly doped N+ region 9 and the highly doped P+ region 10 The upper surface of the N-type buffer zone 7 has a metal electrode 132, and the metal electrode 132 is in the shape of a second step; the upper surface of the N-type buffer zone 7 has a second gate structure, and the second gate structure is composed of a second gate dielectric layer 111 and the second polysilicon electrode 124 located on the upper surface of the second gate dielectric layer 111, along the longitudinal direction of the device, the lower surface of the second gate dielectric layer 111 is sequentially connected with the first N-type low-doped region 3 first step The upper surface of the second gate dielectric layer 111 is in contact with the upper surface of the second N-type low-doped region 150, and the lower surface of the second gate dielectric layer 111 is also in contact with part of the P-type collector region 8 and the upper surface of the highly doped P+ region 10. The second The upper surface of the polysilicon electrode 124 is a horizontal plane; the upper surface of the device between the P-type body region 4 and the N-type buffer zone 7 has a dielectric layer 112, and along the device longitudinal direction, the lower surface of the dielectric layer 112 is sequentially and the upper surface of the first step of the first N-type low-doped region 3 and the second N-type low The upper surface of the doped region 150 is in contact, and the lower surface of the dielectric layer 112 is also in contact with the upper surface of a part of the N-type buffer zone 7; the upper surface of the dielectric layer 112 has a polysilicon P+ region 121, a P-type region 122 and an N+ region 123, wherein the P-type region 122 is located between the polysilicon P+ region 121 and the N+ region 123 and is connected to each other to form a polysilicon diode, the P+ region 121 is located on the side close to the P-type body region 4, and the N+ region 123 is located near the N-type buffer region 7- Side, along the longitudinal direction of the device, the upper surfaces of the polysilicon P+ region 121, the P-type region 122 and the N+ region 123 are horizontal planes; the emitter metal electrode 130 is electrically connected to the polysilicon P+ region 121, and the polysilicon N+ region 123 is connected to the polysilicon N+ region 123. The second polysilicon electrodes 124 are electrically connected and the polysilicon N+ region 123 and the second polysilicon electrode 124 are electrically connected to the collector metal 131 through the Zener diode 140, wherein the cathode of the Zener diode 140 is connected The electrode metal 131 and the anode of the Zener diode 140 are connected to the polysilicon N+ region 123 and the second polysilicon electrode 124 .

本例中,所述N型低掺杂区150的掺杂浓度等于或大于N型低掺杂区3的掺杂浓度;形成的所述沟槽的深度大于所述沟槽的宽度;形成的所述沟槽的深度大于所述沟槽之间的器件表面宽度;所述N型低掺杂漂移区3/150和多晶硅P型区122在器件击穿之前全耗尽;所述多晶硅栅电极120与多晶硅P+区121的间距小于1微米,所述多晶硅P+区121和N+区123的宽度小于1微米,所述多晶硅N+区123与金属电极132的间距小于1微米;通过调节介质层111的厚度和材料,以及介质层111下N型缓冲层7表面的浓度,使由N+区9、P+区10、介质层111、多晶硅电极124、P型集电区8以及N型缓冲层7形成的PMOS器件的阈值电压为-2V-0V;所述齐纳二极管140与本发明结构的其它部分集成在同一芯片上,通过调节齐纳二极管140的参数使齐纳二极管的稳压值为2V-5V。In this example, the doping concentration of the N-type low-doped region 150 is equal to or greater than the doping concentration of the N-type low-doped region 3; the depth of the formed trench is greater than the width of the trench; the formed The depth of the trenches is greater than the device surface width between the trenches; the N-type low-doped drift region 3/150 and the polysilicon P-type region 122 are fully depleted before device breakdown; the polysilicon gate electrode The distance between 120 and the polysilicon P+ region 121 is less than 1 micron, the width of the polysilicon P+ region 121 and the N+ region 123 is less than 1 micron, and the distance between the polysilicon N+ region 123 and the metal electrode 132 is less than 1 micron; by adjusting the dielectric layer 111 Thickness and material, and the concentration of N-type buffer layer 7 surfaces under dielectric layer 111, make by N+ district 9, P+ district 10, dielectric layer 111, polysilicon electrode 124, P-type collector region 8 and N-type buffer layer 7 form The threshold voltage of the PMOS device is -2V-0V; the Zener diode 140 is integrated with other parts of the structure of the present invention on the same chip, and the Zener diode 140 is adjusted to have a voltage stabilizing value of 2V-5V .

本例的工作原理为:This example works as follows:

在阻断状态下,本例中发射极金属电极130和栅电极120接地,集电极金属电极131接高电压Vc。此时,在器件三维折叠表面通过齐纳二极管140和由P+区121、P型区122和N+区123组成的多晶二极管形成的集电极到发射极支路上,齐纳二极管击穿处于稳压状态,齐纳二极管阳极侧电压保持Vc-Vz不变(Vz是齐纳二极管稳压值)。由于齐纳二极管的稳压值Vz较低,因此集电极电压主要由多晶二极管承担,多晶二极管的低掺杂P区122耗尽后为负电荷;同时,在具有折叠结构的多晶二极管下N型低掺杂区3/150中,由于低掺杂N区3/150和P型体区4形成的PN结反偏,并且由于P型体区4和N型缓冲层7浓度远高于低掺杂N区3/150,因此耐压主要由低掺杂N区3/150承担,低掺杂N区3/150耗尽后为正电荷;此时,低掺杂P区122耗尽后的负电荷对低掺杂N区3/150耗尽后的正电荷形成电荷补偿,因此具有折叠结构的低掺杂P区122为低掺杂N区3/150提供附加电荷、三维多重场板和降低表面电场的作用。通过使多晶硅P型区122、低掺杂N区3和低掺杂N区150在器件击穿之前全耗尽,可大幅提高本发明LIGBT的击穿电压并提高低掺杂N区3和低掺杂N区150的掺杂浓度。此外,由于多晶硅电极124与齐纳二极管140相连,由N+区9、P型区10、介质层111、多晶硅电极124、P型集电区8以及N型缓冲层7形成的PMOS的栅源电压保持Vz值,通过调节PMOS的阈值电压使齐纳二极管的稳压值大于PMOS的阈值电压绝对值,此时PMOS开启,重掺杂N+区9通过金属电极132和PMOS与P型集电区8相连,通过金属电极132在N+区9和P型区10之间电子电流和空穴电流的转换,形成阳极短路结构,降低了P型集电区8/低掺杂N型漂移区3和150/P型体区4形成的三极管的增益,从而进一步提高了器件的击穿电压;In the blocking state, in this example, the emitter metal electrode 130 and the gate electrode 120 are grounded, and the collector metal electrode 131 is connected to the high voltage Vc. At this time, on the three-dimensional folded surface of the device, the Zener diode 140 and the polycrystalline diode formed by the P+ region 121, the P-type region 122 and the N+ region 123 form the collector to the emitter branch, and the breakdown of the Zener diode is at a stable voltage. state, the voltage on the anode side of the Zener diode remains unchanged at Vc-Vz (Vz is the voltage regulation value of the Zener diode). Because the regulated voltage value Vz of the zener diode is low, the collector voltage is mainly borne by the polycrystalline diode, and the low-doped P region 122 of the polycrystalline diode is negatively charged after depletion; meanwhile, in the polycrystalline diode with folded structure In the lower N-type low-doped region 3/150, due to the reverse bias of the PN junction formed by the low-doped N region 3/150 and the P-type body region 4, and because the concentration of the P-type body region 4 and the N-type buffer layer 7 is much higher In the low-doped N region 3/150, the withstand voltage is mainly borne by the low-doped N region 3/150, and after the low-doped N region 3/150 is depleted, it becomes a positive charge; at this time, the low-doped P region 122 consumes The depleted negative charges form charge compensation for the depleted positive charges of the low-doped N region 3/150, so the low-doped P region 122 with a folded structure provides additional charges for the low-doped N region 3/150, three-dimensional multiple field plate and reduce the surface electric field. By making the polysilicon P-type region 122, the low-doped N region 3 and the low-doped N region 150 fully depleted before the device breaks down, the breakdown voltage of the LIGBT of the present invention can be greatly improved and the low-doped N region 3 and the low-doped N region 3 and low The doping concentration of the doped N region 150 . In addition, since the polysilicon electrode 124 is connected to the Zener diode 140, the gate-source voltage of the PMOS formed by the N+ region 9, the P-type region 10, the dielectric layer 111, the polysilicon electrode 124, the P-type collector region 8, and the N-type buffer layer 7 Keep the Vz value, and adjust the threshold voltage of the PMOS to make the Zener diode’s stable voltage value greater than the absolute value of the threshold voltage of the PMOS. At this time, the PMOS is turned on, and the heavily doped N+ region 9 passes through the metal electrode 132 and the PMOS and the P-type collector region 8 Connected, through the conversion of electron current and hole current between the N+ region 9 and the P-type region 10 through the metal electrode 132, an anode short-circuit structure is formed, which reduces the P-type collector region 8/lowly doped N-type drift region 3 and 150 The gain of the triode formed by the /P-type body region 4, thereby further improving the breakdown voltage of the device;

在导通状态下,本例中发射极金属电极130接地,栅电极120和集电极金属电极131接高电平,此时P型体区4表面反型MOS沟道开启,N+发射区5向低掺杂漂移区3中注入电子,同时P型集电区8向低掺杂漂移区3中注入空穴,绝缘栅双极型晶体管导通。此时,在器件表面通过齐纳二极管140和多晶二极管形成的集电极到发射极支路上,多晶二极管和齐纳二极管均形成反偏,同时由于集电极电压较低,齐纳二极管140不能击穿,多晶硅电极124和集电极金属电极131之间形成的PMOS栅源电压低于PMOS阈值电压,PMOS处于关断状态,N+区9和P型集电区8处于断开状态,附加结构的存在不会影响器件的正向导通特性,即与传统横向绝缘栅双极型晶体管一样不存在负阻现象。同时三维三栅结构的引入增加了栅结构的等效宽度,进一步减小了器件的正向导通压降。因此,本发明结构具有比传统LIGBT更低的正向导通压降并在导通过程中不存在负阻现象。In the conduction state, in this example, the emitter metal electrode 130 is grounded, and the gate electrode 120 and the collector metal electrode 131 are connected to a high level. At this time, the inversion MOS channel on the surface of the P-type body region 4 is turned on, and the N+ emitter region 5 Electrons are injected into the low-doped drift region 3 , and holes are injected into the low-doped drift region 3 by the P-type collector region 8 at the same time, and the IGBT is turned on. At this time, on the collector-to-emitter branch formed by the Zener diode 140 and the polycrystalline diode on the surface of the device, both the polycrystalline diode and the Zener diode form a reverse bias, and because the collector voltage is low, the Zener diode 140 cannot Breakdown, the PMOS gate-source voltage formed between the polysilicon electrode 124 and the collector metal electrode 131 is lower than the PMOS threshold voltage, the PMOS is in the off state, the N+ region 9 and the P-type collector region 8 are in the disconnected state, and the additional structure It does not affect the forward conduction characteristics of the device, that is, there is no negative resistance phenomenon like the traditional lateral insulated gate bipolar transistor. At the same time, the introduction of the three-dimensional tri-gate structure increases the equivalent width of the gate structure and further reduces the forward conduction voltage drop of the device. Therefore, the structure of the present invention has lower forward conduction voltage drop than traditional LIGBT and there is no negative resistance phenomenon in the conduction process.

在关断过程中,本例中发射极金属电极130接地,栅电极120电压由高电平逐渐降低,P型体区4表面MOS沟道截止,集电极金属电极131电压逐渐增加。随着集电极金属电极131电压的增加,当集电极电压低于齐纳二极管击穿电压Vz时,在器件表面通过齐纳二极管140和多晶二极管形成的集电极到发射极支路上,齐纳二极管未击穿,此时,PMOS栅源电压低于其阈值电压,PMOS处于关断状态。当集电极电压高于齐纳二极管击穿电压Vz后,齐纳二极管击穿,多晶二极管开始承担电压,此时PMOS栅源电压即稳定为Vz不变,通过调节PMOS的阈值电压使齐纳二极管的稳压值大于PMOS的阈值电压绝对值,此时PMOS开启并导通,重掺杂N+区9通过金属电极132和PMOS与P型集电区8相连,通过金属电极132在N+区9和P型区10之间电子电流和空穴电流的转换,形成阳极短路结构,此时,漂移区中的电子由高掺杂N+区9抽取并经过金属电极132转换为空穴电流经PMOS漏极P型区10、栅介质层111下方的反型层、PMOS源极P+区8,最后到达集电极金属131。该过程完成了低掺杂N型漂移区3/150中电子的抽取,从而大大提高了LIGBT的关断速度,降低了关断损耗。同时,在关断过程中,当集电极电压高于齐纳二极管击穿电压Vz后,齐纳二极管击穿,多晶二极管开始承担电压,多晶二极管漂移区122开始耗尽,多晶二极管漂移区耗尽提供的电荷和场板作用加快了器件漂移区耗尽层沿X轴在YZ平面的纵向扩展,进一步加快LIGBT器件内部的载流子抽取,从而提高器件的关断速度,进一步降低器件的关断损耗。此外,高的低掺杂漂移区3/150掺杂浓度的采用进一步减小了需抽取的过剩载流子的浓度,进一步提高了器件的关断速度,降低了器件的关断损耗。During the turn-off process, in this example, the emitter metal electrode 130 is grounded, the voltage of the gate electrode 120 gradually decreases from high level, the MOS channel on the surface of the P-type body region 4 is cut off, and the voltage of the collector metal electrode 131 gradually increases. As the voltage of the collector metal electrode 131 increases, when the collector voltage is lower than the Zener diode breakdown voltage Vz, the collector-to-emitter branch formed by the Zener diode 140 and the polycrystalline diode on the device surface, the Zener The diode is not broken down. At this time, the PMOS gate-source voltage is lower than its threshold voltage, and the PMOS is in an off state. When the collector voltage is higher than the Zener diode breakdown voltage Vz, the Zener diode breaks down, and the polycrystalline diode begins to bear the voltage. At this time, the PMOS gate-source voltage is stable at Vz, and the Zener diode is adjusted by adjusting the threshold voltage of the PMOS. The stable voltage value of the diode is greater than the absolute value of the threshold voltage of the PMOS. At this time, the PMOS is turned on and turned on. The heavily doped N+ region 9 is connected to the P-type collector region 8 through the metal electrode 132 and the PMOS, and the N+ region 9 is connected to the metal electrode 132 through the metal electrode 132. The conversion of electron current and hole current between P-type region 10 forms an anode short-circuit structure. At this time, electrons in the drift region are extracted by highly doped N+ region 9 and converted into hole current through metal electrode 132 through PMOS drain. The pole P-type region 10 , the inversion layer under the gate dielectric layer 111 , the PMOS source P+ region 8 , and finally reaches the collector metal 131 . This process completes the extraction of electrons in the low-doped N-type drift region 3/150, thereby greatly improving the turn-off speed of the LIGBT and reducing the turn-off loss. At the same time, during the turn-off process, when the collector voltage is higher than the Zener diode breakdown voltage Vz, the Zener diode breaks down, the polycrystalline diode begins to bear the voltage, the polycrystalline diode drift region 122 begins to be exhausted, and the polycrystalline diode drifts The charge and field plate effect provided by the region depletion accelerates the longitudinal expansion of the device drift region depletion layer along the X axis in the YZ plane, and further accelerates the carrier extraction inside the LIGBT device, thereby increasing the turn-off speed of the device and further reducing the device the turn-off loss. In addition, the use of a high doping concentration of 3/150 in the low-doped drift region further reduces the concentration of excess carriers to be extracted, further improves the turn-off speed of the device, and reduces the turn-off loss of the device.

实施例2Example 2

如图9所示,与实施例1中不同的是,As shown in Figure 9, the difference from Example 1 is that

在介质层112上方的多晶硅层中直接形成齐纳二极管,所述齐纳二极管形成在沟槽之间的器件表面上,P+区125为齐纳二极管的阳极,N+区126为齐纳二极管的阴极。所述齐纳二极管的类型、位置和形状可根据需要进行调整。A zener diode is directly formed in the polysilicon layer above the dielectric layer 112, the zener diode is formed on the device surface between the trenches, the P+ region 125 is the anode of the zener diode, and the N+ region 126 is the cathode of the zener diode . The type, location and shape of the Zener diodes can be adjusted as desired.

实施例3Example 3

如图10所示,与实施例1中不同的是,在介质层111上方的多晶硅层中直接形成齐纳二极管,所述齐纳二极管形成在沟槽之间的器件表面上,P+区125为齐纳二极管的阳极,N+区126为齐纳二极管的阴极。所述齐纳二极管的类型、位置和形状可根据需要进行调整。As shown in FIG. 10, the difference from Embodiment 1 is that a Zener diode is directly formed in the polysilicon layer above the dielectric layer 111, and the Zener diode is formed on the device surface between the trenches, and the P+ region 125 is The anode of the Zener diode, N+ region 126 is the cathode of the Zener diode. The type, location and shape of the Zener diodes can be adjusted as desired.

实施例4Example 4

在上述实施例的基础上,齐纳二极管由多个串联的二极管所取代,二极管串的阳极接集电极金属131,阴极接多晶硅高掺杂N+区123与多晶硅电极124,并且二极管串的开启电压值大于PMOS的阈值电压绝对值。On the basis of the above-mentioned embodiments, the Zener diode is replaced by a plurality of diodes connected in series, the anode of the diode string is connected to the collector metal 131, the cathode is connected to the polysilicon highly doped N+ region 123 and the polysilicon electrode 124, and the turn-on voltage of the diode string The value is greater than the absolute value of the threshold voltage of the PMOS.

实施例5Example 5

如图11所示,与实施例3不同的是,本例中在所述多晶硅P+区121和多晶硅N+区123之间还具有电容151;所述电容151的电容值小于由N+区9、P+区10、介质层111、多晶硅电极124、P型集电区8以及N型缓冲层7形成的PMOS的栅极电容值。所述电容可以通过表面布线时由多晶硅电极124和发射极金属电极130之间形成的寄生电容形成,也可通过在N型低掺杂漂移区3中或表面布线的金属层和或多晶层中通过集成电容形成。与实施例3相比提高了对多晶硅电极124电压的控制,进一步提高了器件的性能。As shown in Figure 11, different from Embodiment 3, in this example, there is also a capacitor 151 between the polysilicon P+ region 121 and the polysilicon N+ region 123; The gate capacitance value of the PMOS formed by the region 10, the dielectric layer 111, the polysilicon electrode 124, the P-type collector region 8 and the N-type buffer layer 7. The capacitance can be formed by the parasitic capacitance formed between the polysilicon electrode 124 and the emitter metal electrode 130 during surface wiring, or can be formed by the metal layer and or polycrystalline layer in the N-type low-doped drift region 3 or surface wiring Formed by integrating capacitors. Compared with Embodiment 3, the control of the voltage of the polysilicon electrode 124 is improved, and the performance of the device is further improved.

本发明还提供的一种横向绝缘栅双极型晶体管制作方法,基本工艺流程如图12所示,以200V N型横向绝缘栅双极型晶体管结构为例,说明其具体工艺步骤。其特征在于,主要包括以下步骤:The present invention also provides a method for manufacturing a lateral insulated gate bipolar transistor. The basic process flow is shown in FIG. 12 , taking the structure of a 200V N-type lateral insulated gate bipolar transistor as an example to illustrate its specific process steps. It is characterized in that it mainly includes the following steps:

第一步:选取合适的SOI材料,材料包括厚度为300~500微米,浓度为10~100Ω·cm的P型半导体材料衬底1,厚度为0.5~1微米的埋氧化层2,厚度为5~10um、电阻率为5~10Ω·cm的N型低掺杂硅层3;Step 1: Select a suitable SOI material, which includes a P-type semiconductor material substrate 1 with a thickness of 300-500 microns and a concentration of 10-100 Ω·cm, a buried oxide layer 2 with a thickness of 0.5-1 microns, and a thickness of 5 An N-type low-doped silicon layer 3 of ~10um and a resistivity of 5-10Ω·cm;

第二步:通过外延生长形成厚度5~10微米、电阻率为3~10Ω·cm的N型低掺杂区150层,如图13所示;Step 2: Form 150 layers of N-type low-doped regions with a thickness of 5-10 microns and a resistivity of 3-10Ω·cm by epitaxial growth, as shown in Figure 13;

第三步:通过刻蚀工艺在器件表面沿X方向形成沟槽,沟槽的深度为5~10微米,宽度为1~2微米,沟槽之间的宽度为1~2微米,沟槽的下表面在XY平面和N型低掺杂区3接触,沟槽的侧面在XZ平面与N型低掺杂漂移区3和N型低掺杂区150接触,如图14所示;Step 3: Form grooves along the X direction on the surface of the device through an etching process. The depth of the grooves is 5-10 microns, the width is 1-2 microns, and the width between the grooves is 1-2 microns. The lower surface is in contact with the N-type low-doped region 3 on the XY plane, and the sides of the trench are in contact with the N-type low-doped drift region 3 and the N-type low-doped region 150 on the XZ plane, as shown in FIG. 14 ;

第四步:通过光刻、离子注入和退火工艺在器件表面一侧形成具有折叠结构的N型缓冲层7,N型缓冲层7的厚度为1~3um,如图15所示;Step 4: Form an N-type buffer layer 7 with a folded structure on one side of the device surface through photolithography, ion implantation and annealing process, the thickness of the N-type buffer layer 7 is 1-3um, as shown in Figure 15;

第五步:生长栅氧化层、进行多晶硅淀积并光刻、刻蚀形成器件的栅氧化层110、栅电极120、介质层111、多晶硅电极124、介质层112以及介质层112上的多晶层,多晶硅淀积过程中采用原位P型掺杂(用于获得多晶硅P型区122的掺杂),氧化层的厚度为50~100纳米,多晶层的厚度为0.5~1um,多晶层为P型掺杂,掺杂浓度为1015~1016cm-3,如图16所示;The fifth step: grow the gate oxide layer, perform polysilicon deposition and photolithography, etch to form the gate oxide layer 110, gate electrode 120, dielectric layer 111, polysilicon electrode 124, dielectric layer 112 and the polycrystalline silicon on the dielectric layer 112 Layer, in-situ P-type doping (for obtaining the doping of the P-type region 122 of polysilicon) is used in the polysilicon deposition process, the thickness of the oxide layer is 50-100 nanometers, the thickness of the polycrystalline layer is 0.5-1um, and the polycrystalline The layer is P-type doped, and the doping concentration is 10 15 ~ 10 16 cm -3 , as shown in Figure 16;

第六步:进行P型体区光刻和P型离子注入、退火,形成P型体区4,P型体区4的厚度为1~3um;Step 6: Perform photolithography of the P-type body region, P-type ion implantation, and annealing to form the P-type body region 4, and the thickness of the P-type body region 4 is 1-3um;

第七步:进行N+光刻和N型离子注入形成N+发射区5、重掺杂N+区9、多晶硅二极管N+区123;Step 7: Perform N+ photolithography and N-type ion implantation to form N+ emitter region 5, heavily doped N+ region 9, and polysilicon diode N+ region 123;

第八步:进行P+光刻和P型离子注入,形成高掺杂P+区6、P型区10、多晶硅二极管P+区121;Step 8: Perform P+ photolithography and P-type ion implantation to form highly doped P+ regions 6, P-type regions 10, and polysilicon diode P+ regions 121;

第九步:进行P型集电区光刻和离子注入,形成P型集电区8,如图17所示;Step 9: Perform photolithography and ion implantation of the P-type collector region to form a P-type collector region 8, as shown in Figure 17;

第十步:进行BPSG淀积,孔光刻,金属淀积并光刻、刻蚀形成金属互联,即制备获得如图18所示的横向绝缘栅双极型晶体管。Step 10: perform BPSG deposition, hole photolithography, metal deposition, photolithography, and etching to form metal interconnections, that is, to prepare a lateral insulated gate bipolar transistor as shown in FIG. 18 .

进一步地,在介质层的制备工艺中可分两步或三步形成不同厚度和材料的栅介质层110、介质层111和介质层112;Further, the gate dielectric layer 110, dielectric layer 111 and dielectric layer 112 of different thicknesses and materials can be formed in two steps or three steps in the preparation process of the dielectric layer;

进一步地,多晶硅二极管P型区122的掺杂可不采用原位掺杂,而是在P型集电区光刻和离子注入步骤中通过调整光刻版图形比例获得。Further, the doping of the P-type region 122 of the polysilicon diode may not be in-situ doping, but obtained by adjusting the pattern ratio of the photolithography plate during the photolithography and ion implantation steps of the P-type collector region.

Claims (5)

1.一种横向绝缘栅双极型晶体管,其半元胞结构包括从下至上依次层叠设置的衬底(1)、绝缘层(2)和第一N型低掺杂区(3);其特征在于,沿器件纵向方向,所述第一N型低掺杂区(3)为二级阶梯状,定义第二级阶梯的垂直高度大于第一级阶梯,所述第一N型低掺杂区(3)上层两侧分别具有P型体区(4)和N型缓冲区(7),沿器件纵向方向,所述P型体区(4)和N型缓冲区(7)均为二级阶梯状;在第一N型低掺杂区(3)第二级阶梯和P型体区(4)及N型缓冲区(7)第二级阶梯之间具有第二N型低掺杂区(150);所述P型体区(4)上层具有相互并列设置的P+接触区(6)和N+发射区(5),其中N+发射区(5)位于靠近N型缓冲区(7)的一侧,所述P+接触区(6)和N+发射区(5)均为二级阶梯状;所述P+接触区(6)和部分N+发射区(5)上表面具有发射极金属电极(130),所述发射极金属电极(130)为二级阶梯状;所述P型体区(4)上表面具有第一栅极结构,所述第一栅极结构由第一栅介质层(110)和位于第一栅介质层(110)上表面的第一多晶硅栅电极(120)构成,沿器件纵向方向,所述第一栅介质层(110)的下表面依次与第一N型低掺杂区(3)第一阶梯的上表面和第二N型低掺杂区(150)的上表面接触,第一栅介质层(110)的下表面还与部分N+发射区(5)的上表面接触,第一多晶硅栅电极(120)的上表面是水平面;所述N型缓冲区(7)中具有P型集电区(8)、高掺杂N+区(9)和高掺杂P+区(10),高掺杂N+区(9)和高掺杂P+区(10)相互接触且高掺杂N+区(9)位于靠近P型体区(4)的一侧;所述P型集电区(8)、高掺杂N+区(9)和高掺杂P+区(10)均为二级阶梯状;所述P型集电区(8)上表面远离P型体区(4)一侧具有集电极金属电极(131),所述集电极金属电极(131)为二级阶梯状;所述高掺杂N+区(9)和高掺杂P+区(10)的上表面具有金属电极(132),所述金属电极(132)为二级阶梯状;所述N型缓冲区(7)的上表面具有第二栅极结构,所述第二栅极结构由第二栅介质层(111)和位于第二栅介质层(111)上表面的第二多晶硅电极(124)构成,沿器件纵向方向,所述第二栅介质层(111)的下表面依次与第一N型低掺杂区(3)第一阶梯的上表面和第二N型低掺杂区(150)的上表面接触,第二栅介质层(111)的下表面还与部分P型集电区(8)和高掺杂P+区(10)的上表面接触,第二多晶硅电极(124)的上表面是水平面;在所述P型体区(4)和N型缓冲区(7)之间的器件上表面具有介质层(112),沿器件纵向方向,所述介质层(112)的下表面依次与第一N型低掺杂区(3)第一阶梯的上表面和第二N型低掺杂区(150)的上表面接触,所述介质层(112)的下表面还与部分N型缓冲区(7)的上表面接触;所述介质层(112)上表面具有多晶硅P+区(121)、P型区(122)和N+区(123),其中P型区(122)位于多晶硅P+区(121)和N+区(123)之间并相互连接形成多晶硅二极管,P+区(121)位于靠近P型体区(4)的一侧,N+区(123)位于靠近N型缓冲区(7)一侧,沿器件纵向方向,多晶硅P+区(121)、P型区(122)和N+区(123)的上表面是水平面;所述发射极金属电极(130)与多晶硅P+区(121)之间电气连接,所述N+区(123)与第二多晶硅电极(124)之间电气连接并且所述N+区(123)与第二多晶硅电极(124)通过齐纳二极管(140)与集电极金属(131)之间电气连接,其中齐纳二极管(140)的阴极接集电极金属(131),齐纳二极管(140)的阳极接N+区(123)与第二多晶硅电极(124)。1. A lateral insulated gate bipolar transistor, whose half-cell structure includes a substrate (1), an insulating layer (2) and a first N-type low-doped region (3) stacked sequentially from bottom to top; It is characterized in that, along the longitudinal direction of the device, the first N-type low-doped region (3) is in the shape of two steps, defining the vertical height of the second step to be greater than that of the first step, and the first N-type low-doped region There are P-type body regions (4) and N-type buffer regions (7) on both sides of the upper layer of the region (3), and along the longitudinal direction of the device, the P-type body regions (4) and N-type buffer regions (7) are two Step-like; there is a second N-type low doping between the second step of the first N-type low-doped region (3) and the second step of the P-type body region (4) and the N-type buffer zone (7). Region (150); the upper layer of the P-type body region (4) has a P+ contact region (6) and an N+ emitter region (5) arranged side by side, wherein the N+ emitter region (5) is located near the N-type buffer zone (7) One side of the P+ contact region (6) and the N+ emitter region (5) are two-level stepped; the upper surface of the P+ contact region (6) and part of the N+ emitter region (5) has an emitter metal electrode ( 130), the emitter metal electrode (130) is in the shape of two steps; the upper surface of the P-type body region (4) has a first gate structure, and the first gate structure is composed of a first gate dielectric layer ( 110) and the first polysilicon gate electrode (120) located on the upper surface of the first gate dielectric layer (110), along the longitudinal direction of the device, the lower surface of the first gate dielectric layer (110) is sequentially connected with the first N The upper surface of the first step of the N-type low-doped region (3) is in contact with the upper surface of the second N-type low-doped region (150), and the lower surface of the first gate dielectric layer (110) is also in contact with part of the N+ emitter region (5 ), the upper surface of the first polysilicon gate electrode (120) is a horizontal plane; the N-type buffer zone (7) has a P-type collector region (8), a highly doped N+ region (9) and the highly doped P+ region (10), the highly doped N+ region (9) and the highly doped P+ region (10) are in contact with each other and the highly doped N+ region (9) is located on the side close to the P-type body region (4) ; The P-type collector region (8), the highly doped N+ region (9) and the highly doped P+ region (10) are all two-level ladders; the upper surface of the P-type collector region (8) is far away from the P One side of the body region (4) has a collector metal electrode (131), and the collector metal electrode (131) is in a two-level ladder shape; the highly doped N+ region (9) and the highly doped P+ region (10 ) has a metal electrode (132) on the upper surface, and the metal electrode (132) is in a two-level ladder shape; the upper surface of the N-type buffer zone (7) has a second gate structure, and the second gate structure Consists of a second gate dielectric layer (111) and a second polysilicon electrode (124) located on the upper surface of the second gate dielectric layer (111), along the longitudinal direction of the device, the bottom of the second gate dielectric layer (111) The surface is sequentially in contact with the upper surface of the first step of the first N-type low-doped region (3) and the upper surface of the second N-type low-doped region (150), and the lower surface of the second gate dielectric layer (111) is also In contact with the upper surface of part of the P-type collector region (8) and the highly doped P+ region (10), the upper surface of the second polysilicon electrode (124) is a horizontal plane; in the P-type body region (4) and The upper surface of the device between the N-type buffer areas (7) has a dielectric layer (112), and along the longitudinal direction of the device, the lower surface of the dielectric layer (112) is sequentially connected with the first N-type low-doped region (3). The upper surface of the step is in contact with the upper surface of the second N-type low-doped region (150), and the lower surface of the dielectric layer (112) is also in contact with the upper surface of a part of the N-type buffer zone (7); the dielectric layer (112) upper surface has polysilicon P+ area (121), P type area (122) and N+ area (123), and wherein P type area (122) is positioned at polysilicon P+ area (121) and N+ area (123) and mutual Connect to form a polysilicon diode, the P+ region (121) is positioned at the side close to the P-type body region (4), the N+ region (123) is positioned at the side near the N-type buffer zone (7), and along the device longitudinal direction, the polysilicon P+ region (121 ), the upper surface of the P-type region (122) and the N+ region (123) is a horizontal plane; the electrical connection between the emitter metal electrode (130) and the polysilicon P+ region (121), the N+ region (123) and the first The two polysilicon electrodes (124) are electrically connected and the N+ region (123) is electrically connected to the second polysilicon electrode (124) through a Zener diode (140) and the collector metal (131), wherein The cathode of the Zener diode (140) is connected to the collector metal (131), and the anode of the Zener diode (140) is connected to the N+ region (123) and the second polysilicon electrode (124). 2.根据权利要求1所述的一种横向绝缘栅双极型晶体管,其特征在于,所述第二N型低掺杂区(150)的掺杂浓度等于或大于第一N型低掺杂区(3)的掺杂浓度。2. A lateral insulated gate bipolar transistor according to claim 1, characterized in that the doping concentration of the second N-type low-doped region (150) is equal to or greater than that of the first N-type low-doped region Doping concentration of region (3). 3.根据权利要求1或2所述的一种横向绝缘栅双极型晶体管,其特征在于,所述齐纳二极管集成在介质层(112)上方靠近集电极金属电极(131)一侧,相应的集电极金属电极(131)延伸至与介质层(112)侧面接触并覆盖部分齐纳二极管上表面。3. A lateral insulated gate bipolar transistor according to claim 1 or 2, characterized in that the Zener diode is integrated on the side of the dielectric layer (112) close to the collector metal electrode (131), corresponding The collector metal electrode (131) extends to contact with the side of the dielectric layer (112) and covers part of the upper surface of the Zener diode. 4.根据权利要求1或2所述的一种横向绝缘栅双极型晶体管,其特征在于,所述齐纳二极管由多个串联的二极管所取代,二极管串的阳极接集电极金属(131),阴极接N+区(123)与多晶硅电极(124),并且二极管串的开启电压值大于PMOS的阈值电压绝对值。4. A kind of lateral insulated gate bipolar transistor according to claim 1 or 2, is characterized in that, described zener diode is replaced by a plurality of diodes connected in series, and the anode of diode string connects collector metal (131) , the cathode is connected to the N+ region (123) and the polysilicon electrode (124), and the turn-on voltage value of the diode string is greater than the absolute value of the threshold voltage of the PMOS. 5.根据权利要求1或2所述的一种横向绝缘栅双极型晶体管,其特征在于,所述多晶硅P+区(121)和N+区(123)之间还具有电容(151)。5. A lateral insulated gate bipolar transistor according to claim 1 or 2, characterized in that there is a capacitor (151) between the polysilicon P+ region (121) and the N+ region (123).
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