CN105742346B - Double division trench gate charge storage type RC-IGBT and its manufacturing method - Google Patents
Double division trench gate charge storage type RC-IGBT and its manufacturing method Download PDFInfo
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Abstract
Description
技术领域technical field
本发明属于功率半导体器件技术领域,涉及绝缘栅双极型晶体管(IGBT),具体涉及逆导型沟槽栅电荷存储型绝缘栅双极型晶体管(RC-CSTBT)。The invention belongs to the technical field of power semiconductor devices, and relates to an insulated gate bipolar transistor (IGBT), in particular to a reverse conduction trench gate charge storage type insulated gate bipolar transistor (RC-CSTBT).
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,已成为现代电力电子电路中的核心电子元器件之一,广泛地应用在诸如通信、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。IGBT的应用对电力电子系统性能的提升起到了极为重要的作用。从IGBT发明以来,人们一直致力于改善IGBT的性能。经过二十几年的发展,相继提出了6代IGBT器件结构,使器件性能得到了稳步的提升。第6代的沟槽栅电荷存储型绝缘栅双极型晶体管(CSTBT)由于采用了较高掺杂浓度和一定厚度的N型电荷存储层结构,使IGBT器件靠近发射极端的载流子浓度分布得到了极大的改善,提高了N型漂移区的电导调制,改善了整个N型漂移区的载流子浓度分布,使IGBT获得了低的正向导通压降和改善的正向导通压降和关断损耗的折中。Insulated Gate Bipolar Transistor (IGBT) is a new type of power electronic device combining MOS field effect and bipolar transistor. It not only has the advantages of easy driving and simple control of MOSFET, but also has the advantages of low conduction voltage of power transistor, large on-state current and small loss. It has become one of the core electronic components in modern power electronic circuits and is widely used in Various fields of the national economy such as communications, energy, transportation, industry, medicine, household appliances and aerospace. The application of IGBT plays an extremely important role in improving the performance of power electronic systems. Since the invention of IGBT, people have been working on improving the performance of IGBT. After more than 20 years of development, six generations of IGBT device structures have been proposed successively, which has steadily improved device performance. The 6th generation trench gate charge storage insulated gate bipolar transistor (CSTBT) uses a higher doping concentration and a certain thickness of the N-type charge storage layer structure, so that the carrier concentration distribution of the IGBT device near the emitter terminal It has been greatly improved, improving the conductance modulation of the N-type drift region, improving the carrier concentration distribution of the entire N-type drift region, and enabling the IGBT to obtain a low forward conduction voltage drop and an improved forward conduction voltage drop tradeoff with turn-off losses.
在电力电子系统中,IGBT通常需要搭配续流二极管(Free Wheeling Diode,FWD)使用以确保系统的安全稳定。因此在传统IGBT模块或单管器件中,通常会有FWD与其反向并联,该方案不仅增加了器件的个数,模块的体积及生产成本,而且封装过程中焊点数的增加会影响器件的可靠性,金属连线所产生的寄生效应还影响器件的整体性能。为了解决这一问题实现产品的整体化,结合CSTBT器件结构,业界提出了逆导型沟槽栅电荷存储型绝缘栅双极型晶体管(RC-CSTBT),成功地将续流二极管集成在CSTBT内部,其结构如图1所示。相比于传统无续流能力的CSTBT,该结构在其背部制作了与金属集电极13和N型电场阻止层10连接的N型集电区12,该区域同器件中P型基区7、N型电荷存储层8和N-漂移区9形成了寄生二极管结构,在续流模式下该寄生二极管导通提供电流通路。In power electronic systems, IGBTs usually need to be used with Free Wheeling Diodes (FWD) to ensure the safety and stability of the system. Therefore, in traditional IGBT modules or single-tube devices, FWD is usually connected in reverse parallel with it. This solution not only increases the number of devices, the volume of the module and the production cost, but also increases the number of solder joints in the packaging process, which will affect the reliability of the device. The parasitic effects generated by the metal wiring also affect the overall performance of the device. In order to solve this problem and achieve product integration, combined with the CSTBT device structure, the industry proposed a reverse conduction trench gate charge storage type insulated gate bipolar transistor (RC-CSTBT), and successfully integrated the freewheeling diode inside the CSTBT. , whose structure is shown in Figure 1. Compared with the traditional CSTBT without freewheeling capability, this structure has an N-type collector region 12 connected to the metal collector 13 and the N-type electric field stop layer 10 on its back, which is the same as the P-type base region 7, The N-type charge storage layer 8 and the N-drift region 9 form a parasitic diode structure, and in the freewheeling mode, the parasitic diode conducts to provide a current path.
然而,对于传统的RC-CSTBT器件结构,在正向IGBT工作模式时,由于较高掺杂浓度和一定厚度的N型电荷存储层的存在,器件的击穿电压显著降低,为了有效屏蔽N型电荷存储层的不利影响获得一定的器件耐压,需要采用:1)深的沟槽栅深度,使沟槽栅的深度大于N型电荷存储层的结深,但深的沟槽栅深度不仅增大了栅极-发射极电容,也增大了栅极-集电极电容,因而,降低了器件的开关速度,增大器件的开关损耗,影响了器件的导通压降和开关损耗的折中特性;2)小的元胞宽度,使沟槽栅之间的间距尽可能减小,然而,高密度的沟槽MOS结构不仅增大了器件的栅极电容,降低了器件的开关速度,增大了器件的开关损耗,影响了器件的导通压降和开关损耗的折中特性,而且,增加了器件的饱和电流密度,使器件的短路安全工作区变差。在反向二极管续流工作模式时,由于P型基区7和N型电荷存储层8/N-漂移区9形成的PN结的内建势的存在,正向导通压降较大,同时由于在续流二极管导通时大量载流子注入进N-漂移区9,大量过剩载流子的存在使得续流二极管的反向恢复特性较差,如反向恢复时间长、反向恢复电荷大等。However, for the traditional RC-CSTBT device structure, in the forward IGBT mode, due to the presence of a higher doping concentration and a certain thickness of the N-type charge storage layer, the breakdown voltage of the device is significantly reduced. In order to effectively shield the N-type Adverse effects of the charge storage layer To obtain a certain device withstand voltage, it is necessary to adopt: 1) deep trench gate depth, so that the depth of the trench gate is greater than the junction depth of the N-type charge storage layer, but the deep trench gate depth not only increases The larger gate-emitter capacitance also increases the gate-collector capacitance, thus reducing the switching speed of the device, increasing the switching loss of the device, and affecting the compromise between the conduction voltage drop and switching loss of the device characteristics; 2) The small cell width minimizes the distance between the trench gates. However, the high-density trench MOS structure not only increases the gate capacitance of the device, but also reduces the switching speed of the device and increases the The switching loss of the device is increased, which affects the compromise characteristics of the conduction voltage drop and switching loss of the device, and increases the saturation current density of the device, making the short-circuit safe working area of the device worse. In the reverse diode freewheeling mode of operation, due to the existence of the built-in potential of the PN junction formed by the P-type base region 7 and the N-type charge storage layer 8/N-drift region 9, the forward conduction voltage drop is relatively large, and at the same time due to When the freewheeling diode is turned on, a large number of carriers are injected into the N-drift region 9. The existence of a large number of excess carriers makes the reverse recovery characteristics of the freewheeling diode poor, such as long reverse recovery time and large reverse recovery charge. Wait.
发明内容Contents of the invention
本发明的目的是为了优化传统RC-CSTBT的正向IGBT特性,同时改善反向二极管特性,提高器件的可靠性,在传统RC-CSTBT器件结构的基础上(如图1所示),本发明提供一种双分裂沟槽栅电荷存储型RC-IGBT(如图2所示)及其制作方法,所述RC-IGBT器件在正向IGBT工作模式时,在一定的器件沟槽深度和沟槽MOS结构密度的情况下,通过在器件沟槽内栅电极的底部和侧面引入与发射极等电位的双分裂电极,通过双分裂电极以及双分裂电极和栅电极之间厚介质层的屏蔽作用,减小了器件的栅极电容,特别是栅极-集电极电容,提高了器件的开关速度,减小了开关损耗,进一步改善了正向导通压降和开关损耗的折中,同时,侧面分裂电极的引入减小了MOS沟道的密度,改善了IGBT的短路安全工作区,提高了器件的性能和可靠性;此外,沟槽底部宽的底部分裂电极进一步增强了发射极端的载流子增强效应,进一步改善了整个N型漂移区的载流子浓度分布,进一步改善了正向导通压降和开关损耗的折中,提高了器件的性能;同时,通过底部分裂电极周围厚的介质层和宽的宽度在一定的器件沟槽深度和沟槽MOS结构密度的情况下进一步有效的屏蔽了N型电荷存储层以及栅电极和侧面分裂电极处薄的介质层对器件耐压的影响,提高了器件的击穿电压,改善了沟槽底部电场的集中,进一步提高了器件的可靠性。在反向二极管续流工作模式时,通过与发射极相连的侧面分裂电极的作用,使侧面分裂电极处的MOS沟道开启,使反向续流二极管工作于多子器件模式,具有低的反向二极管导通压降和优异的反向恢复特性。本发明提供的制作方法不需要增加额外的工艺步骤,与传统的沟槽栅电荷存储型RC-IGBT制作方法兼容。The purpose of the present invention is in order to optimize the forward IGBT characteristic of traditional RC-CSTBT, improve reverse diode characteristic simultaneously, improve the reliability of device, on the basis of traditional RC-CSTBT device structure (as shown in Figure 1), the present invention Provide a double-split trench gate charge storage type RC-IGBT (as shown in Figure 2) and its manufacturing method. In the case of MOS structure density, by introducing a double-split electrode with the same potential as the emitter at the bottom and side of the gate electrode in the device trench, through the shielding effect of the double-split electrode and the thick dielectric layer between the double-split electrode and the gate electrode, The gate capacitance of the device is reduced, especially the gate-collector capacitance, the switching speed of the device is improved, the switching loss is reduced, and the compromise between forward voltage drop and switching loss is further improved. At the same time, the side split The introduction of the electrode reduces the density of the MOS channel, improves the short-circuit safe operating area of the IGBT, and improves the performance and reliability of the device; in addition, the wide bottom split electrode at the bottom of the trench further enhances the carrier enhancement of the emitter terminal effect, further improving the carrier concentration distribution of the entire N-type drift region, further improving the compromise between the forward conduction voltage drop and switching loss, and improving the performance of the device; at the same time, through the thick dielectric layer around the bottom split electrode and The wide width further effectively shields the N-type charge storage layer and the influence of the thin dielectric layer at the gate electrode and the side split electrode on the device withstand voltage under the condition of a certain device trench depth and trench MOS structure density, and improves the device withstand voltage. The breakdown voltage of the device improves the concentration of the electric field at the bottom of the trench, and further improves the reliability of the device. In the reverse diode freewheeling mode, through the side split electrode connected to the emitter, the MOS channel at the side split electrode is turned on, so that the reverse freewheeling diode works in the multi-sub-device mode, with low backlash diode turn-on voltage drop and excellent reverse recovery characteristics. The manufacturing method provided by the invention does not need to add additional process steps, and is compatible with the traditional trench gate charge storage type RC-IGBT manufacturing method.
本发明的技术方案为:双分裂沟槽栅电荷存储型RC-IGBT,包括从下至上依次层叠设置的集电极金属13、P型集电极区11、N型电场阻止层10、N型漂移区9和发射极金属1;还包括与P型集电极区11并列设置的N型集电极区12;所述N型漂移区9中具有N+发射区5、P+发射区6、P型基区7、N型电荷存储层8和沟槽栅结构;所述沟槽栅结构沿垂直方向依次贯穿N+发射区5、P型基区7和N型电荷存储层8后延伸至N型漂移区中;所述P型基区7位于N型电荷存储层8上表面,N+发射区5和P+发射区6并列位于P型基区7上表面;N+发射区5和P+发射区6的上表面与发射极金属1连接;其特征在于,所述沟槽栅结构包括底部分裂电极31、栅电极32、侧面分裂电极33、栅介质层41、第二介质层42、第三介质层43、第四介质层44和第五介质层45;所述栅电极32和侧面分裂电极33之间通过第三介质层43连接;所述栅电极32通过栅介质层41与沟槽栅结构一侧的N+发射区5和P型基区7连接;所述侧面分裂电极33通过第二介质层42与沟槽栅结构另一侧的N+发射区5和P型基区7连接;所述底部分裂电极31位于栅电极32和侧面分裂电极33的下方,且底部分裂电极31的上表面深度小于N型电荷存储层8的结深,底部分裂电极31的下表面深度大于N型电荷存储层8的结深;所述底部分裂电极31的上表面与栅电极32、侧面分裂电极33的下表面之间通过第四介质层44连接;所述底部分裂电极31的下表面及侧面与N型漂移区9和N型电荷存储层8之间通过第五介质层45连接;所述底部分裂电极31的宽度大于第二介质层42、侧面分裂电极33、第三介质层43、栅电极32和栅介质层41的宽度之和,使沟槽栅结构呈倒“T”字形;所述第二介质层42、侧面分裂电极33及部分第三介质层43的上表面与发射极金属1连接;所述栅介质层41、栅电极32及部分第三介质层43的上表面具有第一介质层2;所述底部分裂电极31、侧面分裂电极33与发射极金属1等电位。The technical solution of the present invention is: double-split trench gate charge storage type RC-IGBT, including collector metal 13, P-type collector region 11, N-type electric field stop layer 10, and N-type drift region stacked sequentially from bottom to top 9 and emitter metal 1; also includes an N-type collector region 12 arranged in parallel with the P-type collector region 11; the N-type drift region 9 has an N+ emitter region 5, a P+ emitter region 6, and a P-type base region 7 , an N-type charge storage layer 8 and a trench gate structure; the trench gate structure sequentially penetrates the N+ emitter region 5, the P-type base region 7 and the N-type charge storage layer 8 along the vertical direction, and then extends into the N-type drift region; The P-type base region 7 is located on the upper surface of the N-type charge storage layer 8, and the N+ emitter region 5 and the P+ emitter region 6 are located side by side on the upper surface of the P-type base region 7; pole metal 1 connection; it is characterized in that the trench gate structure includes a bottom split electrode 31, a gate electrode 32, a side split electrode 33, a gate dielectric layer 41, a second dielectric layer 42, a third dielectric layer 43, a fourth dielectric layer 44 and the fifth dielectric layer 45; the gate electrode 32 and the side split electrode 33 are connected through the third dielectric layer 43; the gate electrode 32 is connected to the N+ emitter region on one side of the trench gate structure through the gate dielectric layer 41 5 is connected to the P-type base region 7; the side split electrode 33 is connected to the N+ emitter region 5 and the P-type base region 7 on the other side of the trench gate structure through the second dielectric layer 42; the bottom split electrode 31 is located at the gate Below the electrode 32 and the side split electrode 33, and the upper surface depth of the bottom split electrode 31 is less than the junction depth of the N-type charge storage layer 8, and the lower surface depth of the bottom split electrode 31 is greater than the junction depth of the N-type charge storage layer 8; The upper surface of the bottom split electrode 31 is connected to the lower surface of the gate electrode 32 and the side split electrode 33 through a fourth dielectric layer 44; the lower surface and side surfaces of the bottom split electrode 31 are connected to the N-type drift region 9 and the N-type The charge storage layers 8 are connected through the fifth dielectric layer 45; the width of the bottom split electrode 31 is greater than the width of the second dielectric layer 42, the side split electrodes 33, the third dielectric layer 43, the gate electrode 32 and the gate dielectric layer 41 The sum makes the trench gate structure an inverted "T" shape; the upper surface of the second dielectric layer 42, the side split electrode 33 and part of the third dielectric layer 43 is connected to the emitter metal 1; the gate dielectric layer 41 The upper surface of the gate electrode 32 and part of the third dielectric layer 43 has the first dielectric layer 2 ; the bottom split electrode 31 and the side split electrode 33 have the same potential as the emitter metal 1 .
进一步的,所述第三介质层43,第四介质层44以及第五介质层45的厚度大于栅介质层41和第二介质层42的厚度。Further, the thicknesses of the third dielectric layer 43 , the fourth dielectric layer 44 and the fifth dielectric layer 45 are greater than the thicknesses of the gate dielectric layer 41 and the second dielectric layer 42 .
进一步的,所述栅介质层41的厚度大于第二介质层42的厚度。Further, the thickness of the gate dielectric layer 41 is greater than the thickness of the second dielectric layer 42 .
进一步的,所述侧面分裂电极33的底部延伸至与底部分裂电极31的上表面连接。Further, the bottom of the side split electrode 33 extends to connect with the upper surface of the bottom split electrode 31 .
进一步的,所述沟槽栅结构的两侧还具有N+层14,所述N+层14的一侧与N型电荷存储层8连接,N+层14的另一侧及底部与沟槽栅结构连接,N+层14的上表面与P型基区7的下表面连接。Further, there are N+ layers 14 on both sides of the trench gate structure, one side of the N+ layer 14 is connected to the N-type charge storage layer 8, and the other side and bottom of the N+ layer 14 are connected to the trench gate structure , the upper surface of the N+ layer 14 is connected to the lower surface of the P-type base region 7 .
进一步的,所述漂移区结构为NPT结构或FS结构;所述IGBT器件采用半导体材料Si、SiC、GaAs或者GaN制作。Further, the drift region structure is an NPT structure or an FS structure; the IGBT device is made of semiconductor materials Si, SiC, GaAs or GaN.
双分裂沟槽栅电荷存储型RC-IGBT的制造方法,其特征在于,包括以下步骤:The manufacturing method of double-split trench gate charge storage type RC-IGBT is characterized in that it comprises the following steps:
第一步:选取N型轻掺杂单晶硅片作为器件的N型漂移区9,选取的硅片厚度为300~600um,掺杂浓度为1013~1014个/cm3;在硅片背面通过离子注入N型杂质并退火制作器件的N型场阻止层10,形成的N型场阻止层的厚度为15~30微米,离子注入能量为1500keV~2000keV,注入剂量为1013~1014个/cm2,退火温度为1200-1250℃,退火时间为300~600分钟;Step 1: Select an N-type lightly doped single crystal silicon wafer as the N-type drift region 9 of the device. The thickness of the selected silicon wafer is 300-600um, and the doping concentration is 10 13 -10 14 /cm 3 ; The N-type field stop layer 10 of the device is manufactured by ion-implanting N-type impurities on the back and annealing. The thickness of the formed N-type field stop layer is 15-30 microns, the ion implantation energy is 1500keV-2000keV, and the implantation dose is 1013-1014 pieces/cm 2 , the annealing temperature is 1200-1250°C, and the annealing time is 300-600 minutes;
第二步:翻转并减薄硅片到所需的厚度,在硅片表面通过光刻、刻蚀形成沟槽;The second step: Flip and thin the silicon wafer to the required thickness, and form grooves on the surface of the silicon wafer by photolithography and etching;
第三步:在1050℃~1150℃,O2的气氛下在沟槽周围形成氧化层;接着在750℃~950℃下在沟槽内淀积填充多晶硅;再次氧化并刻蚀掉多余的氧化层;形成底部分裂电极31和第五介质层45,所述底部分类电极31位于第五介质层45中;Step 3: Form an oxide layer around the trench at 1050°C to 1150°C in an O 2 atmosphere; then deposit and fill polysilicon in the trench at 750°C to 950°C; oxidize again and etch away excess oxide layer; form the bottom split electrode 31 and the fifth dielectric layer 45, the bottom sort electrode 31 is located in the fifth dielectric layer 45;
第四步:通过外延在硅片表面形成2~6微米厚的N型掺杂层;Step 4: Form an N-type doped layer with a thickness of 2 to 6 microns on the surface of the silicon wafer by epitaxy;
第五步:在硅片表面淀积一层薄的垫氧化层和氮化硅层,光刻出窗口后,再次进行沟槽硅刻蚀,在底部电极31上方刻蚀出沟槽,第三步中多晶硅表面氧化形成的氧化层可作为本步硅刻蚀的终止层;沟槽刻蚀完成后,通过溶液将表面的氮化硅和垫氧化层漂洗干净;该步骤中形成的沟槽和第二步中形成的沟槽构成倒“T”字形沟槽;Step 5: Deposit a thin layer of pad oxide layer and silicon nitride layer on the surface of the silicon wafer. After the window is photoetched, silicon trench etching is performed again, and a trench is etched above the bottom electrode 31. The third step The oxide layer formed by oxidizing the surface of polysilicon in the step can be used as the stop layer of silicon etching in this step; after the trench etching is completed, rinse the silicon nitride and pad oxide layer on the surface with a solution; the groove and pad oxide layer formed in this step The groove formed in the second step constitutes an inverted "T" shaped groove;
第六步:通过热氧化在沟槽内壁生长氧化层,形成的氧化层厚度小于120nm;Step 6: grow an oxide layer on the inner wall of the trench by thermal oxidation, and the thickness of the formed oxide layer is less than 120nm;
第七步:采用光刻工艺,刻蚀第六步中沟槽内左侧壁形成的氧化层;在沟槽右侧侧壁形成栅介质层41;在沟槽底部形成第四介质层44;Step 7: Etching the oxide layer formed on the left side wall of the trench in the sixth step by using a photolithography process; forming a gate dielectric layer 41 on the right side wall of the trench; forming a fourth dielectric layer 44 at the bottom of the trench;
第八步:通过热氧化在沟槽内壁再次生长氧化层,形成的氧化层厚度小于40nm;在沟槽左侧侧壁形成第二栅介质层42Step 8: Re-grow an oxide layer on the inner wall of the trench by thermal oxidation, and the thickness of the formed oxide layer is less than 40nm; form a second gate dielectric layer 42 on the left side wall of the trench
第九步:在750℃~950℃下在沟槽内淀积填充多晶硅;Step 9: Deposit and fill polysilicon in the trench at 750°C to 950°C;
第十步:采用光刻工艺,刻蚀第九步中沟槽内填充的部分多晶硅,在沟槽两侧分别形成栅电极32和侧面分裂电极33;所述栅电极32与栅介质层41连接,侧面分裂电极33与第二介质层42连接;Step 10: Etching part of the polysilicon filled in the trench in step 9 by photolithography, forming gate electrodes 32 and side split electrodes 33 on both sides of the trench respectively; the gate electrodes 32 are connected to the gate dielectric layer 41 , the side split electrode 33 is connected to the second dielectric layer 42;
第十一步:淀积,在第十步中形成的栅电极32和侧面分裂电极33之间的沟槽内填充介质形成第三介质层43;The eleventh step: deposition, the trench between the gate electrode 32 and the side split electrode 33 formed in the tenth step is filled with a dielectric to form a third dielectric layer 43;
第十二步:采用光刻工艺,先通过离子注入N型杂质制作器件的N型电荷存储层8,所述N型电荷存储层8位于沟槽两侧;离子注入的能量为200~500keV,注入剂量为1013~1014个/cm2;然后通过离子注入P型杂质并退火制作P型基区7,离子注入的能量为60~120keV,注入剂量为1013~1014个/cm2,退火温度为1100-1150℃,退火时间为10~30分钟;所述P型基区7位于N型电荷存储层8上表面;形成的N型电荷存储层8的结深大于栅电极32的深度并小于底部分裂电极31的深度,形成的P型基区7的结深小于栅电极32的深度;The twelfth step: using a photolithography process, first fabricate the N-type charge storage layer 8 of the device by ion-implanting N-type impurities, and the N-type charge storage layer 8 is located on both sides of the trench; the energy of ion implantation is 200-500keV, The implantation dose is 10 13 to 10 14 pcs/cm 2 ; then the P-type base region 7 is produced by ion implantation of P-type impurities and annealing, the energy of ion implantation is 60-120keV, and the implantation dose is 10 13-10 14 pcs/cm 2 , the annealing temperature is 1100-1150°C, and the annealing time is 10-30 minutes; the P-type base region 7 is located on the upper surface of the N-type charge storage layer 8; the junction depth of the formed N-type charge storage layer 8 is greater than that of the gate electrode 32 The depth is less than the depth of the bottom split electrode 31, and the junction depth of the formed P-type base region 7 is less than the depth of the gate electrode 32;
第十三步:采用光刻工艺,通过离子注入N型杂质制作器件的N+发射区5,离子注入的能量为30~60keV,注入剂量为1015~1016个/cm2;所述N+发射区5位于P型基区7上表面并与沟槽连接;The thirteenth step: using a photolithography process, the N+ emission region 5 of the device is manufactured by ion implantation of N-type impurities, the ion implantation energy is 30-60keV, and the implantation dose is 10 15-10 16 /cm 2 ; the N+ emission Region 5 is located on the upper surface of P-type base region 7 and connected to the trench;
第十四步:采用光刻工艺,通过离子注入P型杂质并退火制作器件的P+发射区6,离子注入的能量为60~80keV,注入剂量为1015~1016个/cm2,退火温度为900℃,时间为20~30分钟;所述P+发射区6与N+发射区5并列位于P型基区7上表面;Step 14: Using the photolithography process, the P+ emission region 6 of the device is produced by ion-implanting P-type impurities and annealing. The energy of ion implantation is 60-80keV, the implantation dose is 10 15-10 16 /cm 2 , and the annealing temperature The temperature is 900°C, and the time is 20 to 30 minutes; the P+ emitter region 6 and the N+ emitter region 5 are located side by side on the upper surface of the P-type base region 7;
第十五步:在器件表面淀积介质层,并光刻、刻蚀形成第一介质层2;所述第一介质层2位于部分第三介质层43、栅电极32和栅介质层41的上表面;Step 15: Deposit a dielectric layer on the surface of the device, and form a first dielectric layer 2 by photolithography and etching; the first dielectric layer 2 is located between a part of the third dielectric layer 43, the gate electrode 32 and the gate dielectric layer 41 upper surface;
第十六步:淀积金属,并光刻、刻蚀在N+发射区5和P+发射区6上表面以及第二介质层42、侧面分裂电极33及部分第三介质层43的上表面形成集电极金属1;The sixteenth step: deposit metal, and photolithography, etch on the upper surface of the N + emission region 5 and P + emission region 6 and the upper surface of the second dielectric layer 42, the side split electrode 33 and part of the third dielectric layer 43 to form a set electrode metal 1;
第十七步:翻转硅片,减薄硅片厚度,在硅片背面注入P型杂质形成P型集电区11,所述P型集电区11位于N型电场阻止层10下表面,注入能量为40~60keV,注入剂量为1012~1013个/cm2;再次光刻,通过离子注入N型杂质制作器件的N型集电区12,离子注入的能量为40~60keV,注入剂量为1014~1015个/cm2;接着在H2与N2混合的气氛下进行背面退火,温度为400~450℃,时间为20~30分钟;所述N型集电区12与P型集电区11并列设置;The seventeenth step: turn over the silicon wafer, reduce the thickness of the silicon wafer, inject P-type impurities on the back of the silicon wafer to form a P-type collector region 11, and the P-type collector region 11 is located on the lower surface of the N-type electric field stop layer 10, and inject The energy is 40-60keV, and the implantation dose is 10 12-10 13 pcs/cm 2 ; the N-type collector region 12 of the device is fabricated by ion-implanting N-type impurities. The ion-implantation energy is 40-60keV, and the implantation dose is 10 14 to 10 15 pieces/cm 2 ; followed by back annealing in an atmosphere of H 2 and N 2 mixed at a temperature of 400 to 450°C for 20 to 30 minutes; the N-type collector region 12 and the P Type collectors 11 are arranged side by side;
第十八步:背面淀积金属形成集电极金属13。Step 18: Deposit metal on the back to form collector metal 13 .
进一步的,所述第三步中,可通过增加光刻步骤分两次分别形成P型基区7,使靠近栅电极32一侧的P型基区7的浓度和结深大于靠近侧面分裂电极33一侧的P型基区7的浓度和结深。Further, in the third step, the P-type base region 7 can be formed in two steps by increasing the photolithography step, so that the concentration and junction depth of the P-type base region 7 on the side near the gate electrode 32 are greater than those near the side split electrode. The concentration and junction depth of the P-type base region 7 on the 33 side.
本发明的工作原理是:The working principle of the present invention is:
对于如图1所示的传统的RC-CSTBT器件,在正向IGBT工作模式时,为了提高IGBT器件的性能,改善其可靠性,需要在一定的阻断电压能力下减小器件的开关损耗并降低正向导通压降、同时改善器件的短路安全工作区。IGBT的开关过程就是对栅极电容进行冲、放电的过程,栅极电容越大冲、放电时间越长。因而,在IGBT的开关过程中,栅极电容,特别是栅极-集电极电容对器件的开关损耗具有重要的影响。在如图1所示的传统的沟槽栅电荷储存型RC-IGBT结构中,为了有效屏蔽较高掺杂浓度和一定厚度的N型电荷存储层对击穿电压的不利影响获得一定的器件耐压,需要采用:1)深的沟槽栅深度,使沟槽栅的深度大于N型电荷存储层的结深;2)小的元胞宽度,高密度的沟槽MOS结构使沟槽栅之间的间距尽可能减小。然而,深的沟槽栅深度和高密度的沟槽MOS结构两种方式都不仅增大了栅极-发射极电容,也增大了栅极-集电极电容。此外,对于传统的沟槽栅电荷储存型IGBT结构,栅氧化层是通过一次热氧化在沟槽中形成,为了保证一定的阈值电压整个栅氧化层的厚度均较小,由于MOS电容大小与氧化层的厚度成反比,传统沟槽栅电荷储存型IGBT结构中小的栅氧化层厚度极大的增大了器件的栅极电容。同时高密度的沟槽MOS结构增加了器件的饱和电流密度,使器件的短路安全工作区变差;另外,小的栅氧化层厚度使沟槽底部的电场集中,使器件的可靠性较差。For the traditional RC-CSTBT device shown in Figure 1, in the forward IGBT mode, in order to improve the performance and reliability of the IGBT device, it is necessary to reduce the switching loss of the device and reduce the switching loss of the device under a certain blocking voltage capability. Reduces the forward voltage drop while improving the short-circuit safe operating area of the device. The switching process of the IGBT is the process of charging and discharging the gate capacitance. The larger the gate capacitance is, the longer the discharge time is. Therefore, in the switching process of the IGBT, the gate capacitance, especially the gate-collector capacitance has an important influence on the switching loss of the device. In the traditional trench gate charge storage type RC-IGBT structure as shown in Figure 1, in order to effectively shield the adverse effect of higher doping concentration and certain thickness of the N-type charge storage layer on the breakdown voltage to obtain a certain device endurance Therefore, it is necessary to use: 1) Deep trench gate depth, so that the depth of the trench gate is greater than the junction depth of the N-type charge storage layer; 2) Small cell width, high-density trench MOS structure makes the trench gate The distance between them should be reduced as much as possible. However, both the deep trench gate depth and the high density trench MOS structure increase not only the gate-emitter capacitance but also the gate-collector capacitance. In addition, for the traditional trench gate charge storage type IGBT structure, the gate oxide layer is formed in the trench by one thermal oxidation. In order to ensure a certain threshold voltage, the thickness of the entire gate oxide layer is small. The thickness of the layer is inversely proportional to the thickness of the small gate oxide layer in the traditional trench gate charge storage IGBT structure, which greatly increases the gate capacitance of the device. At the same time, the high-density trench MOS structure increases the saturation current density of the device, which deteriorates the short-circuit safe operating area of the device; in addition, the small gate oxide layer thickness concentrates the electric field at the bottom of the trench, making the reliability of the device poor.
如图2,3和4所示,本发明通过在器件沟槽内栅电极的底部和侧面引入与发射极等电位的双分裂电极以及双分裂电极和栅电极之间的厚介质层,在不影响IGBT器件阈值电压和开通的情况下:1)减小了沟槽内栅电极的深度,大大减小了包括栅极-集电极电容、栅极-发射极电容在内的栅极电容;2)通过双分裂电极的屏蔽作用,屏蔽了栅极和集电极的耦合,将栅极-集电极电容转换为栅极-发射极电容,大大减小了栅极-集电极电容,同时通过厚介质层43和44的作用使从栅极-集电极电容转换而增加的栅极-发射极电容远远小于由于侧面分裂电极33引入而减小的栅极-发射极电容,从而大大减小了包括栅极-集电极电容、栅极-发射极电容在内的栅极电容。因此,本发明结构大大减小了器件的栅极电容,特别是栅极-集电极电容,提高了器件的开关速度,降低器件的开关损耗。此外,在一定的沟槽MOS结构密度下侧面分裂电极33的引入减小了MOS沟道的密度,减小了器件的饱和电流密度,改善了器件的短路安全工作区,提高了可靠性;此外,沟槽底部宽的底部分裂电极进一步增强了发射极端的载流子浓度增强效应,进一步改善了整个N型漂移区的载流子浓度分布,进一步改善了正向导通压降和开关损耗的折中,提高了器件的性能;此外,由于侧面分裂电极33和底部分裂电极31与发射极等电位,在IGBT器件开启动态过程中,通过介质层与侧面分裂电极33和底部分裂电极31接触的半导体表面不会形成反型(浮空p型基区72)和电子积累(N型电荷存储层8和N型漂移区9),因此不会形成负微分电容效应,避免了开启动态过程中的电流、电压振荡和EMI问题,提高了可靠性;同时,通过底部分裂电极周围的厚介质层和宽的宽度在一定的器件沟槽深度和沟槽MOS结构密度的情况下进一步有效的屏蔽了N型电荷存储层以及栅电极和侧面分裂电极处薄的介质层对器件耐压的影响,特别是有效的屏蔽了为了获得小的寄生MOS结构阈值电压而设置的极薄的侧面分裂电极处介质层对器件耐压的影响,提高了器件的击穿电压,改善了沟槽底部电场的集中,进一步提高了器件的可靠性。本发明提供的复合双分裂沟槽结构,沟槽栅电极32的深度大于p型基区7的深度并且沟槽栅电极32的深度小于N型电荷存储层8的深度,这一方面在不影响IGBT器件开通的情况下尽可能的减小了栅极电容,特别是栅极-集电极电容,另一方面一定厚度的高浓度N型电荷存储层8的存在补偿了由于与发射极等电位的底部分裂电极的引入使得底部分裂电极附近载流子浓度的下降,避免了由于底部分裂电极的引入使器件的正向导通压降急剧增大而导致的器件特性变差。在反向二极管续流工作模式时,通过调整p型基区7的浓度和厚度以及介质层42的厚度和材料,使侧面分裂电极处寄生的MOS结构的阈值电压小于0.1V,通过与发射极相连的侧面分裂电极的作用,使侧面分裂电极处的MOS沟道在低于0.1V开启,使反向续流二极管工作于MOS控制二极管的多子器件模式,屏蔽了由P型基区7和N型电荷存储层8/N-漂移区9形成的PN结内建势的影响,使反向续流二极管具有低的二极管导通压降;同时由于是多子导电,不需要在反向恢复过程中对N-漂移区9中的过剩载流子进行抽取,改善了续流二极管的反向恢复特性,如反向恢复时间短、反向恢复电荷小等。此外,本发明提供的制作方法不需要增加额外的工艺步骤,与传统的沟槽栅电荷存储型RC-IGBT制作方法兼容。As shown in Figures 2, 3 and 4, the present invention introduces a double-split electrode at the same potential as the emitter and a thick dielectric layer between the double-split electrode and the gate electrode at the bottom and sides of the gate electrode in the device trench. In the case of affecting the threshold voltage and turn-on of the IGBT device: 1) the depth of the gate electrode in the trench is reduced, and the gate capacitance including gate-collector capacitance and gate-emitter capacitance is greatly reduced; 2 ) through the shielding effect of the double-split electrodes, the coupling between the gate and the collector is shielded, and the gate-collector capacitance is converted into a gate-emitter capacitance, which greatly reduces the gate-collector capacitance. At the same time, through the thick dielectric Layers 43 and 44 act to make the gate-emitter capacitance increase from the gate-collector capacitance conversion much smaller than the gate-emitter capacitance decrease due to the introduction of the side split electrode 33, thereby greatly reducing the included Gate capacitance including gate-collector capacitance, gate-emitter capacitance. Therefore, the structure of the present invention greatly reduces the gate capacitance of the device, especially the gate-collector capacitance, improves the switching speed of the device, and reduces the switching loss of the device. In addition, under a certain trench MOS structure density, the introduction of the side split electrode 33 reduces the density of the MOS channel, reduces the saturation current density of the device, improves the short-circuit safe working area of the device, and improves reliability; in addition , the wide bottom split electrode at the bottom of the trench further enhances the carrier concentration enhancement effect at the emitter end, further improves the carrier concentration distribution in the entire N-type drift region, and further improves the forward conduction voltage drop and switching loss. In addition, since the side split electrode 33 and the bottom split electrode 31 are equipotential to the emitter, during the dynamic process of turning on the IGBT device, the semiconductor layer in contact with the side split electrode 33 and the bottom split electrode 31 through the dielectric layer No inversion (floating p-type base region 72) and electron accumulation (N-type charge storage layer 8 and N-type drift region 9) will be formed on the surface, so the negative differential capacitance effect will not be formed, and the current flow during the dynamic process of turning on will not be formed. , voltage oscillation and EMI problems, improving reliability; at the same time, through the thick dielectric layer and wide width around the bottom split electrode, the N-type is further effectively shielded under the condition of a certain device trench depth and trench MOS structure density. The impact of the charge storage layer and the thin dielectric layer at the gate electrode and the side split electrode on the withstand voltage of the device, especially effectively shielding the pair of the dielectric layer at the extremely thin side split electrode for obtaining a small parasitic MOS structure threshold voltage The impact of the withstand voltage of the device increases the breakdown voltage of the device, improves the concentration of the electric field at the bottom of the trench, and further improves the reliability of the device. In the composite double-split trench structure provided by the present invention, the depth of the trench gate electrode 32 is greater than the depth of the p-type base region 7 and the depth of the trench gate electrode 32 is smaller than the depth of the N-type charge storage layer 8, which does not affect the When the IGBT device is turned on, the gate capacitance, especially the gate-collector capacitance, is reduced as much as possible. On the other hand, the existence of a high-concentration N-type charge storage layer 8 with a certain thickness compensates The introduction of the bottom split electrode reduces the carrier concentration near the bottom split electrode, avoiding the deterioration of the device characteristics caused by the sharp increase of the forward conduction voltage drop of the device due to the introduction of the bottom split electrode. In the reverse diode freewheeling mode, by adjusting the concentration and thickness of the p-type base region 7 and the thickness and material of the dielectric layer 42, the threshold voltage of the parasitic MOS structure at the side split electrode is less than 0.1V, and the The role of the connected side split electrodes makes the MOS channel at the side split electrodes open below 0.1V, so that the reverse freewheeling diode works in the multi-sub-device mode of the MOS control diode, shielding the P-type base region 7 and The impact of the built-in potential of the PN junction formed by the N-type charge storage layer 8/N-drift region 9 makes the reverse freewheeling diode have a low diode conduction voltage drop; at the same time, due to the multi-subconduction, it does not need to recover in the reverse direction During the process, the excess carriers in the N-drift region 9 are extracted, which improves the reverse recovery characteristics of the freewheeling diode, such as short reverse recovery time and small reverse recovery charge. In addition, the manufacturing method provided by the present invention does not need to add additional process steps, and is compatible with the traditional trench gate charge storage type RC-IGBT manufacturing method.
本发明的有益效果为,极大的减小了包括栅极-集电极电容、栅极-发射极电容在内的栅极电容;改善了整个N型漂移区的载流子浓度分布;提高了器件的开关速度,降低器件的开关损耗,减小了器件的饱和电流密度,改善了器件的短路安全工作区,提高了可靠性,改善了沟槽底部电场的集中,避免了由于底部分裂电极的引入使器件的正向导通压降急剧增大而导致的器件特性变差,使反向续流二极管具有低的二极管导通压降,改善了续流二极管的反向恢复特性,如反向恢复时间短、反向恢复电荷小等;此外,本发明提供的制作方法不需要增加额外的工艺步骤,与传统的沟槽栅电荷存储型RC-IGBT制作方法兼容。The beneficial effects of the present invention are that the gate capacitance including gate-collector capacitance and gate-emitter capacitance is greatly reduced; the carrier concentration distribution of the entire N-type drift region is improved; The switching speed of the device reduces the switching loss of the device, reduces the saturation current density of the device, improves the short-circuit safe working area of the device, improves the reliability, improves the concentration of the electric field at the bottom of the trench, and avoids the splitting of the electrode due to the bottom The introduction of a sharp increase in the forward conduction voltage drop of the device leads to the deterioration of the device characteristics, so that the reverse freewheeling diode has a low diode conduction voltage drop, which improves the reverse recovery characteristics of the freewheeling diode, such as reverse recovery The time is short, the reverse recovery charge is small, etc.; in addition, the manufacturing method provided by the present invention does not need to add additional process steps, and is compatible with the traditional trench gate charge storage type RC-IGBT manufacturing method.
附图说明Description of drawings
图1是传统的RC-CSTBT器件元胞结构示意图;Figure 1 is a schematic diagram of the cell structure of a traditional RC-CSTBT device;
图1中,1为发射极金属,2为介质层,3为栅电极,4为栅介质层,5为N+发射区,6为P+发射区,7为P型基区,8为N型电荷存储层,9为N-漂移区,10为N型电场阻止层,11为P型集电区,12为N型集电区,13为集电极金属;In Figure 1, 1 is the emitter metal, 2 is the dielectric layer, 3 is the gate electrode, 4 is the gate dielectric layer, 5 is the N+ emitter region, 6 is the P+ emitter region, 7 is the P-type base region, and 8 is the N-type charge The storage layer, 9 is an N-drift region, 10 is an N-type electric field stop layer, 11 is a P-type collector region, 12 is an N-type collector region, and 13 is a collector metal;
图2是实施例1的双分裂沟槽栅电荷存储型RC-IGBT器件元胞结构示意图;Fig. 2 is the schematic diagram of the cell structure of the double split trench gate charge storage type RC-IGBT device of embodiment 1;
图3是实施例2的双分裂沟槽栅电荷存储型RC-IGBT器件元胞结构示意图;3 is a schematic diagram of the cell structure of the double split trench gate charge storage type RC-IGBT device of embodiment 2;
图4是实施例3的双分裂沟槽栅电荷存储型RC-IGBT器件元胞结构示意图;Fig. 4 is the schematic diagram of the cell structure of the double-split trench gate charge storage type RC-IGBT device of embodiment 3;
图2至图3中,1为发射极金属,2为介质层,31为底部分裂电极,32为栅电极,33为侧面分裂电极,41为栅介质层,42为介质层,43为介质层,44为介质层,45为介质层,5为N+发射区,6为P+发射区,7为P型基区,8为N型电荷存储层,9为N-漂移区,10为N型电场阻止层,11为P型集电区,12为N型集电区,13为集电极金属,14为N+层;In Figure 2 to Figure 3, 1 is the emitter metal, 2 is the dielectric layer, 31 is the bottom split electrode, 32 is the gate electrode, 33 is the side split electrode, 41 is the gate dielectric layer, 42 is the dielectric layer, 43 is the dielectric layer , 44 is the dielectric layer, 45 is the dielectric layer, 5 is the N+ emitter region, 6 is the P+ emitter region, 7 is the P-type base region, 8 is the N-type charge storage layer, 9 is the N-drift region, and 10 is the N-type electric field Blocking layer, 11 is a P-type collector area, 12 is an N-type collector area, 13 is a collector metal, and 14 is an N+ layer;
图5是本发明的制造方法中第一次刻蚀形成沟槽后的器件结构示意图;5 is a schematic diagram of the device structure after the first etching to form a trench in the manufacturing method of the present invention;
图6是本发明的制造方法中形成底部分裂电极后的器件结构示意图;6 is a schematic diagram of the device structure after forming bottom split electrodes in the manufacturing method of the present invention;
图7是本发明的制造方法中外延N-层后的器件结构示意图;7 is a schematic diagram of the device structure after the epitaxial N-layer in the manufacturing method of the present invention;
图8是本发明的制造方法中第二次刻蚀形成沟槽后的器件结构示意图;8 is a schematic diagram of the device structure after the trench is formed by the second etching in the manufacturing method of the present invention;
图9是本发明的制造方法中形成栅介质层后的器件结构示意图;9 is a schematic diagram of the device structure after forming a gate dielectric layer in the manufacturing method of the present invention;
图10是本发明的制造方法中形成栅电极和侧面分裂电极后的器件结构示意图;10 is a schematic diagram of the device structure after forming the gate electrode and the side split electrode in the manufacturing method of the present invention;
图11是本发明的制造方法中完全全部步骤后的器件结构示意图。Fig. 11 is a schematic diagram of the device structure after all the steps in the manufacturing method of the present invention are completed.
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
本例的一种双分裂沟槽栅电荷存储型RC-IGBT,其元胞结构如图2所示,包括:背部集电极金属13、位于背部集电极金属13之上并与其相连的P型集电区11和N型集电区12、位于P型集电区11和N型集电区12之上并与其相连的N型场阻止层10、位于N型场阻止层10之上并与其相连的N-漂移区9;位于N-漂移区9上部中间并与其相连的复合双分裂沟槽结构;位于N-漂移区9上部两侧并与其相连的N型电荷存储层8,所述N型电荷存储层8的侧壁与复合双分裂沟槽结构的侧壁相连,位于N型电荷存储层8上部并于其相连的p型基区7,所述p型基区7的侧壁与复合双分裂沟槽结构的侧壁相连;位于p型基区7上部并与其相连的彼此独立的N+发射区和P+发射区,所述N+发射区的侧壁与复合双分裂沟槽结构的侧壁相连;位于N+发射区和P+发射区上表面的发射极金属1;位于复合双分裂沟槽结构上部的介质层2;其特征在于:所述复合双分裂沟槽结构包括下层结构及上层结构;所述下层结构包括厚介质层45和设置于厚介质层45中的底部分裂电极31;所述上层结构包括沟槽栅电极32,侧面分裂电极33,介质层41,介质层42,介质层43和介质层44,所述栅电极32和侧面分裂电极33之间是介质层43,所述栅电极32和侧面分裂电极33与底部分裂电极31之间是介质层44,所述沟槽栅电极32通过介质层41与N+发射区5和p型基区7相连,所述侧面分裂电极33通过介质层42与N+发射区5和p型基区7相连;所述下层结构的宽度大于所述上层结构的宽度;所述沟槽栅电极32的深度大于p型基区7的结深,所述沟槽栅电极32的深度小于N型电荷存储层8的结深,所述沟槽栅电极32和侧面分裂电极33的宽度大于介质层45和介质层44的厚度;所述侧面分裂电极33的深度大于p型基区7的结深,所述侧面分裂电极33的深度不小于沟槽栅电极32的深度;所述底部分裂电极31上表面的深度小于N型电荷存储层8的结深,所述底部分裂电极31下表面的深度大于N型电荷存储层8的结深;所述介质层45、43和44的厚度大于介质层41和42的厚度,所述介质层42的厚度小于介质层41的厚度;所述侧面分裂电极33与发射极金属1在表面相连,所述底部分裂电极31与发射极金属1等电位。形成的所述沟槽栅电极32的深度大于p型基区7的结深0.1~0.2微米,形成的所述N型电荷存储层8的厚度为1~2微米;形成的所述底部分裂电极31上表面的深度小于N型电荷存储层8的结深0.5~1.5微米,下表面的深度大于N型电荷存储层8的结深0.5~1微米;形成的所述介质层41的厚度小于120纳米,形成的所述介质层42的厚度小于40纳米,形成的所述介质层43的宽度为0.5~1微米,形成的所述介质层44和45的厚度为0.2~0.5微米,形成的所述复合双分裂沟槽结构的下层结构比上层结构在左右两边各宽0.2~1微米;通过调整p型基区7的浓度和厚度以及介质层42的厚度和材料,使侧面分裂电极处寄生的MOS结构的阈值电压小于0.1V。A double-split trench gate charge storage type RC-IGBT in this example has a cell structure as shown in Figure 2, including: a back collector metal 13, a P-type collector located on the back collector metal 13 and connected to it. The electrical region 11 and the N-type collector region 12, the N-type field stop layer 10 located on the P-type collector region 11 and the N-type collector region 12 and connected to it, the N-type field stop layer 10 located on and connected to it The N-drift region 9; the composite double-split trench structure located in the middle of the upper part of the N-drift region 9 and connected thereto; the N-type charge storage layer 8 located on both sides of the upper part of the N-drift region 9 and connected to it, the N-type The sidewall of the charge storage layer 8 is connected to the sidewall of the composite double-split trench structure, and the p-type base region 7 located on the upper part of the N-type charge storage layer 8 and connected thereto, the sidewall of the p-type base region 7 is connected to the composite double-split trench structure. The side walls of the double-split trench structure are connected; the N+ emitter region and the P+ emitter region independent of each other are located on the top of the p-type base region 7 and connected to it, and the side walls of the N+ emitter region are connected to the side walls of the composite double-split trench structure. Connected; the emitter metal 1 located on the upper surface of the N+ emitter region and the P+ emitter region; the dielectric layer 2 located on the upper part of the composite double-split trench structure; it is characterized in that: the composite double-split trench structure includes a lower structure and an upper layer structure; The lower structure includes a thick dielectric layer 45 and the bottom split electrode 31 disposed in the thick dielectric layer 45; the upper structure includes a trench gate electrode 32, a side split electrode 33, a dielectric layer 41, a dielectric layer 42, and a dielectric layer 43 And a dielectric layer 44, between the gate electrode 32 and the side split electrode 33 is a dielectric layer 43, between the gate electrode 32 and the side split electrode 33 and the bottom split electrode 31 is a dielectric layer 44, the trench gate electrode 32 is connected with the N+ emitter region 5 and the p-type base region 7 through the dielectric layer 41, and the side split electrode 33 is connected with the N+ emitter region 5 and the p-type base region 7 through the dielectric layer 42; the width of the lower structure is larger than the The width of the upper structure; the depth of the trench gate electrode 32 is greater than the junction depth of the p-type base region 7, the depth of the trench gate electrode 32 is less than the junction depth of the N-type charge storage layer 8, and the trench gate electrode 32 and the width of the side split electrode 33 are greater than the thickness of the dielectric layer 45 and the dielectric layer 44; the depth of the side split electrode 33 is greater than the junction depth of the p-type base region 7, and the depth of the side split electrode 33 is not less than the trench gate The depth of the electrode 32; the depth of the upper surface of the bottom split electrode 31 is less than the junction depth of the N-type charge storage layer 8, and the depth of the lower surface of the bottom split electrode 31 is greater than the junction depth of the N-type charge storage layer 8; the medium The thickness of the layers 45, 43 and 44 is greater than the thickness of the dielectric layer 41 and 42, and the thickness of the dielectric layer 42 is smaller than the thickness of the dielectric layer 41; the side split electrode 33 is connected with the emitter metal 1 on the surface, and the bottom split The electrode 31 is at the same potential as the emitter metal 1 . The formed trench gate electrode 32 has a depth greater than the junction depth of the p-type base region 7 by 0.1 to 0.2 microns, and the formed N-type charge storage layer 8 has a thickness of 1 to 2 microns; the formed bottom split electrode The depth of the upper surface of 31 is 0.5-1.5 microns less than the junction depth of the N-type charge storage layer 8, and the depth of the lower surface is 0.5-1 microns greater than the junction depth of the N-type charge storage layer 8; the thickness of the formed dielectric layer 41 is less than 120 nanometer, the thickness of the formed dielectric layer 42 is less than 40 nanometers, the formed width of the dielectric layer 43 is 0.5-1 micron, the formed thickness of the described dielectric layers 44 and 45 is 0.2-0.5 micron, and the formed The lower structure of the composite double-split trench structure is 0.2-1 micron wider than the upper structure on the left and right sides; by adjusting the concentration and thickness of the p-type base region 7 and the thickness and material of the dielectric layer 42, the parasitic The threshold voltage of the MOS structure is less than 0.1V.
实施例2Example 2
本例的一种双分裂沟槽栅电荷存储型RC-IGBT,其元胞结构如图3所示,与实施例1不同的是,侧面分裂电极33的下部直接延伸到底部分裂电极31的上表面,使侧面分裂电极33与底部分裂电极31直接相连进一步减小器件的栅极电容。A double-split trench gate charge storage type RC-IGBT in this example has a cell structure as shown in Figure 3. The difference from Example 1 is that the lower part of the side split electrode 33 extends directly to the top of the bottom split electrode 31. On the surface, the side split electrode 33 is directly connected to the bottom split electrode 31 to further reduce the gate capacitance of the device.
实施例3Example 3
本例的一种双分裂沟槽栅电荷存储型RC-IGBT,其元胞结构如图3所示,与实施例1不同的是,在所述复合沟槽结构的下层结构与p型基区7之间的部分区域还具有一层N+层14,所述N+层14的浓度大于N型电荷存储层8的浓度并且其侧壁与复合沟槽结构相连,形成的所述N+层14进一步减小了所述复合沟槽结构下层结构与p型基区7之间区域的电阻,进一步提高了发射极端的载流子注入增强效应,可获得更好的器件正向导通压降和开关损耗的折中。A double-split trench gate charge storage type RC-IGBT in this example has a cell structure as shown in Figure 3. The difference from Example 1 is that the underlying structure of the composite trench structure and the p-type base region Part of the region between 7 also has a layer of N+ layer 14, the concentration of the N+ layer 14 is greater than the concentration of the N-type charge storage layer 8 and its sidewall is connected to the composite trench structure, the formed N+ layer 14 further reduces The resistance of the area between the lower layer structure of the composite trench structure and the p-type base region 7 is reduced, the carrier injection enhancement effect of the emitter terminal is further improved, and better forward voltage drop and switching loss of the device can be obtained. compromise.
本发明工艺制作方法的具体实施方案以600V电压等级的双分裂沟槽栅电荷存储型RC-IGBT为例进行阐述,具体工艺制作方法如下:The specific implementation scheme of the process manufacturing method of the present invention is described by taking the double-split trench gate charge storage type RC-IGBT with a voltage level of 600V as an example, and the specific process manufacturing method is as follows:
第一步:选取掺杂浓度为2×1014个/cm3,厚度为300~600微米的轻掺杂FZ硅片用以形成器件的N-漂移区9;在硅片背面通过离子注入N型杂质并退火制作器件的N型场阻止层10,形成的N型场阻止层的厚度为15~20微米,离子注入能量为1500keV~2000keV,注入剂量为5×1013个/cm2,退火温度为1200℃,退火时间为400分钟;Step 1: Select a lightly doped FZ silicon wafer with a doping concentration of 2×10 14 /cm 3 and a thickness of 300-600 microns to form the N-drift region 9 of the device; Type impurity and annealing to make the N-type field stop layer 10 of the device, the thickness of the formed N-type field stop layer is 15-20 microns, the ion implantation energy is 1500keV-2000keV, the implantation dose is 5× 1013 / cm2 , annealing The temperature is 1200°C, and the annealing time is 400 minutes;
第二步:翻转并减薄硅片至90~95微米的厚度,在硅片表面通过光刻、刻蚀形成均匀分布的沟槽,沟槽深度为0.5~2微米,宽度为2~3微米,沟槽之间的间距为0.5~1.5微米;Step 2: Flip and thin the silicon wafer to a thickness of 90-95 microns, and form evenly distributed grooves on the surface of the silicon wafer by photolithography and etching. The groove depth is 0.5-2 microns and the width is 2-3 microns , the distance between the grooves is 0.5-1.5 microns;
第三步:在1050℃~1150℃,O2的气氛下在沟槽周围形成厚度为0.2~0.5微米的厚氧化层;接着在850℃下在沟槽内积淀填充多晶硅;再次氧化并刻蚀掉多余的氧化层,在多晶硅表面形成0.2~0.3微米的厚氧化层;The third step: form a thick oxide layer with a thickness of 0.2 to 0.5 microns around the trench at 1050 ° C to 1150 ° C in an O2 atmosphere; then deposit and fill polysilicon in the trench at 850 ° C; oxidize and etch again Remove the excess oxide layer and form a thick oxide layer of 0.2 to 0.3 microns on the surface of polysilicon;
第四步:通过外延在硅片表面形成厚度为3~5微米,掺杂浓度为2×1014个/cm3的N型掺杂层;Step 4: Form an N-type doped layer with a thickness of 3-5 microns and a doping concentration of 2×10 14 /cm 3 on the surface of the silicon wafer by epitaxy;
第五步:在硅片表面淀积一层薄的垫氧化层和氮化硅层,光刻出窗口后,再次进行沟槽(trench)硅刻蚀,刻蚀出沟槽,第三步多晶硅表面氧化形成的氧化层可作为本步硅刻蚀的终止层;沟槽刻蚀完成后,通过溶液将表面的氮化硅和垫氧化层漂洗干净;本步形成的沟槽中线与第二步形成的沟槽中线重合,形成的沟槽宽度为0.6~1.5微米;Step 5: Deposit a thin layer of pad oxide layer and silicon nitride layer on the surface of the silicon wafer. After the window is photolithographically etched, perform trench silicon etching again to etch the trench. The third step is polysilicon The oxide layer formed by surface oxidation can be used as the stop layer of silicon etching in this step; after the trench etching is completed, rinse the silicon nitride and pad oxide layer on the surface with a solution; the centerline of the trench formed in this step and the second step The center lines of the formed grooves coincide, and the width of the formed grooves is 0.6-1.5 microns;
第六步:通过热氧化在沟槽内壁生长高质量的薄氧化层,形成的氧化层厚度小于60nm;Step 6: grow a high-quality thin oxide layer on the inner wall of the trench by thermal oxidation, and the thickness of the formed oxide layer is less than 60nm;
第七步:光刻,刻蚀第六步中沟槽内左侧壁形成的氧化层;The seventh step: photolithography, etching the oxide layer formed on the left side wall of the trench in the sixth step;
第八步:通过热氧化在沟槽内壁再次生长高质量的薄氧化层,形成的氧化层厚度小于20nm;Step 8: Re-grow a high-quality thin oxide layer on the inner wall of the trench by thermal oxidation, and the thickness of the formed oxide layer is less than 20nm;
第九步:在850℃下在沟槽内淀积填充多晶硅;Step 9: Deposit and fill polysilicon in the trench at 850°C;
第十步:光刻,刻蚀第九步中沟槽内填充的部分多晶硅,形成栅电极32和侧面分裂电极33;The tenth step: photolithography, etching part of the polysilicon filled in the trench in the ninth step to form the gate electrode 32 and the side split electrode 33;
第十一步:淀积,在第十步形成的栅电极32和侧面分裂电极33之间沟槽内填充介质形成介质层43;The eleventh step: depositing, filling the trench between the gate electrode 32 and the side split electrode 33 formed in the tenth step with a dielectric to form a dielectric layer 43;
第十二步:光刻,先通过离子注入N型杂质制作器件的N型电荷存储层8,离子注入的能量为500keV,注入剂量为5×1013个/cm2;然后通过离子注入P型杂质并退火制作器件的p型基区7,离子注入的能量为120keV,注入剂量为1×1014个/cm2,退火温度为1100-1150℃,退火时间为15~30分钟;形成的p型基区7的结深比栅电极32的深度浅0.1~0.2微米,形成的所述N型电荷存储层8的结深大于栅电极32的深度并小于底部分裂电极31的深度,形成的N型电荷存储层8的厚度为1~2微米;The twelfth step: photolithography, first fabricate the N-type charge storage layer 8 of the device by ion implantation of N-type impurities, the energy of ion implantation is 500keV, and the implantation dose is 5×10 13 /cm 2 ; and then by ion implantation of P-type impurity and annealed to make the p-type base region 7 of the device, the ion implantation energy is 120keV, the implantation dose is 1×10 14 /cm 2 , the annealing temperature is 1100-1150°C, and the annealing time is 15-30 minutes; the formed p The junction depth of the N-type base region 7 is 0.1-0.2 microns shallower than the depth of the gate electrode 32, and the junction depth of the formed N-type charge storage layer 8 is greater than the depth of the gate electrode 32 and smaller than the depth of the bottom split electrode 31. The thickness of the type charge storage layer 8 is 1-2 micrometers;
第十三步:光刻,通过离子注入N型杂质制作器件的N+发射区,离子注入的能量为40keV,注入剂量为1×1015个/cm2;The thirteenth step: photolithography, fabricate the N+ emission region of the device by ion implantation of N-type impurities, the ion implantation energy is 40keV, and the implantation dose is 1×10 15 /cm 2 ;
第十四步:光刻,通过离子注入P型杂质并退火制作器件的P+发射区,离子注入的能量为60keV,注入剂量为5×1015个/cm2,退火温度为900℃,时间为30分钟;The fourteenth step: photolithography, the P+ emission region of the device is manufactured by ion implantation of P-type impurities and annealing. The ion implantation energy is 60keV, the implantation dose is 5×10 15 /cm 2 , the annealing temperature is 900°C, and the time is 30 minutes;
第十五步:淀积介质层,并光刻、刻蚀形成介质层2;Step 15: Deposit a dielectric layer, and form a dielectric layer 2 by photolithography and etching;
第十六步:淀积金属,并光刻、刻蚀形成金属集电极1;Step 16: Deposit metal, and form metal collector 1 by photolithography and etching;
第十七步:翻转硅片,减薄硅片厚度,光刻并在硅片背面注入P型杂质制作器件的P型集电区11,注入能量为60keV,注入剂量为5×1012个/cm2;再次光刻,通过离子注入N型杂质制作器件的N型集电区12,离子注入的能量为60keV,注入剂量为2×1014个/cm2;接着在H2与N2混合的气氛下进行背面退火,温度为450℃,时间为30分钟;Step 17: Turn over the silicon wafer, reduce the thickness of the silicon wafer, photolithography and implant P-type impurities on the back of the silicon wafer to make the P-type collector region 11 of the device, the implantation energy is 60keV, and the implantation dose is 5×10 12 / cm 2 ; photolithography again, by ion-implanting N-type impurities to fabricate the N-type collector region 12 of the device, the ion implantation energy is 60keV, and the implantation dose is 2×10 14 /cm 2 ; then mix H 2 and N 2 The back annealing is carried out under the atmosphere, the temperature is 450 ℃, and the time is 30 minutes;
第十八步:背面淀积金属形成金属集电极13。Step 18: Deposit metal on the back to form the metal collector 13 .
即制备得双分裂沟槽栅电荷存储型RC-IGBT。That is, a double-split trench gate charge storage type RC-IGBT is prepared.
进一步的,所述工艺步骤中第一步N型场阻止层10的制备可在器件的正面结构制备完成之后进行;或可直接选用具有N型场阻止层10和N-漂移区9的双层外延材料作为工艺起始的硅片材料;Further, the preparation of the N-type field stop layer 10 in the first step of the process steps can be carried out after the preparation of the front structure of the device is completed; or a double layer with the N-type field stop layer 10 and the N-drift region 9 can be directly selected. The epitaxial material is used as the silicon wafer material at the beginning of the process;
进一步的,所述工艺步骤中第一步N型场阻止层10的制备可省略;Further, the preparation of the N-type field stop layer 10 in the first step in the process steps can be omitted;
进一步的,第九步多晶硅淀积前可增加一步刻蚀工艺,刻蚀去除侧面分裂电极33下的氧化层,即形成如图3所示的器件结构;Further, before the ninth step of polysilicon deposition, an etching process can be added to remove the oxide layer under the side split electrode 33 by etching to form the device structure as shown in FIG. 3 ;
进一步的,在第六步氧化工艺之前通过带角度的离子注入N型杂质形成高掺杂浓度的N+层14或在第十二步N型电荷存储层8的形成过程中,通过增加一步光刻和离子注入工艺形成高掺杂浓度的N+层14,即形成如图4所示的器件结构;Further, before the sixth step of the oxidation process, the N+ layer 14 with high doping concentration is formed by implanting N-type impurities with angled ions or in the formation process of the N-type charge storage layer 8 in the twelfth step, by adding a step of photolithography and an ion implantation process to form a highly doped N+ layer 14, that is, to form a device structure as shown in FIG. 4;
进一步的,所述工艺步骤中第十二步,可通过增加光刻步骤分两次在沟槽两侧分别形成p型基区7,使靠近栅电极32一侧的P型基区7的浓度和结深大于靠近侧面分裂电极33一侧的P型基区7的浓度和结深;Further, in the twelfth step of the process steps, the p-type base region 7 can be formed on both sides of the trench respectively by increasing the photolithography step twice, so that the concentration of the p-type base region 7 on the side close to the gate electrode 32 and the junction depth are greater than the concentration and junction depth of the P-type base region 7 near the side split electrode 33;
进一步的,所述介质层41,42,43,44和45的材料可以相同也可以不同。Further, the materials of the dielectric layers 41 , 42 , 43 , 44 and 45 can be the same or different.
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