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CN103560086B - The preparation method of the super-junction semiconductor device of avalanche capacity can be improved - Google Patents

The preparation method of the super-junction semiconductor device of avalanche capacity can be improved Download PDF

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CN103560086B
CN103560086B CN201310491435.6A CN201310491435A CN103560086B CN 103560086 B CN103560086 B CN 103560086B CN 201310491435 A CN201310491435 A CN 201310491435A CN 103560086 B CN103560086 B CN 103560086B
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CN103560086A (en
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姜贯军
陈桥梁
陈仕全
马治军
杜忠鹏
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Longteng Semiconductor Co ltd
Lonten Semiconductor Co ltd
Xi'an Longfei Electric Technology Co ltd
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XI'AN LONTEN RENEWABLE ENERGY TECHNOLOGY Inc
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/01Manufacture or treatment
    • H10D30/021Manufacture or treatment of FETs having insulated gates [IGFET]
    • H10D30/028Manufacture or treatment of FETs having insulated gates [IGFET] of double-diffused metal oxide semiconductor [DMOS] FETs
    • H10D30/0291Manufacture or treatment of FETs having insulated gates [IGFET] of double-diffused metal oxide semiconductor [DMOS] FETs of vertical DMOS [VDMOS] FETs
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/10Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
    • H10D62/102Constructional design considerations for preventing surface leakage or controlling electric field concentration
    • H10D62/103Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices
    • H10D62/105Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices by having particular doping profiles, shapes or arrangements of PN junctions; by having supplementary regions, e.g. junction termination extension [JTE] 
    • H10D62/109Reduced surface field [RESURF] PN junction structures
    • H10D62/111Multiple RESURF structures, e.g. double RESURF or 3D-RESURF structures
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/60Impurity distributions or concentrations
    • 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
    • H10D84/101Integrated devices comprising main components and built-in components, e.g. IGBT having built-in freewheel diode
    • H10D84/141VDMOS having built-in components

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Abstract

本发明涉及一种可改善雪崩能力的超结半导体器件的制备方法。传统较高的P柱掺杂浓度加剧了横向扩散使得导通电阻相应增大,且P柱与N柱电荷的失衡使得击穿电压的降低。本发明利用外延工艺,形成N型外延层;进行硼离子注入形成P型N型外延层;硼离子注入剂量逐次增加,然后在高温下推结形成P型与N型交替的外延层;注入硼离子形成Pbody区;使用干法刻蚀多晶硅形成多晶硅栅电极;注入砷离子,形成N+源区;在整个器件的上表面淀积一层铝,并刻蚀铝形成源金属电极,背面金属化形成漏电极。本发明所得的超结半导体器件在提高了超结半导体器件的雪崩能力同时减小了导通电阻。

The invention relates to a preparation method of a super junction semiconductor device capable of improving avalanche capability. The traditionally higher doping concentration of the P-column aggravates the lateral diffusion and increases the on-resistance accordingly, and the charge imbalance between the P-column and the N-column reduces the breakdown voltage. The present invention utilizes the epitaxial process to form an N-type epitaxial layer; performs boron ion implantation to form a P-type N-type epitaxial layer; the dose of boron ion implantation increases successively, and then pushes the junction at a high temperature to form a P-type and N-type alternate epitaxial layer; implants boron Ions form the Pbody region; use dry etching polysilicon to form polysilicon gate electrodes; implant arsenic ions to form N+ source regions; deposit a layer of aluminum on the upper surface of the entire device, and etch the aluminum to form source metal electrodes, and back metallization to form drain electrode. The super junction semiconductor device obtained by the invention improves the avalanche capability of the super junction semiconductor device and reduces the on-resistance at the same time.

Description

可改善雪崩能力的超结半导体器件的制备方法Preparation method of super junction semiconductor device capable of improving avalanche capability

技术领域 technical field

本发明属于半导体器件与工艺制造领域,具体涉及一种可改善雪崩能力的超结半导体器件的制备方法。 The invention belongs to the field of semiconductor devices and process manufacturing, and in particular relates to a preparation method of a super junction semiconductor device capable of improving avalanche capability.

背景技术 Background technique

超结VDMOS是一种发展迅速、应用广泛的新型功率半导体器件。它在普通垂直双扩散金属氧化物半导体(VDMOS)基础上,引入超结(Superjunction)结构,使之即具有VDMOS输入阻抗高、开关速度快、工作频率高、电压控制、热稳定性好、驱动电路简单,又克服了VDMOS的导通电阻与击穿电压成2.5次方关系急剧增加的缺点。目前超结VDMOS已广泛应用于电脑、手机、照明以及液晶或等离子电视机和游戏机等消费电子产品的电源或适配器。 Super junction VDMOS is a new type of power semiconductor device with rapid development and wide application. It introduces a superjunction (Superjunction) structure on the basis of ordinary vertical double-diffused metal oxide semiconductor (VDMOS), so that it has VDMOS high input impedance, fast switching speed, high operating frequency, voltage control, good thermal stability, and drive The circuit is simple, and overcomes the shortcoming that the on-resistance of VDMOS and the breakdown voltage increase sharply in the relationship of 2.5 powers. At present, super-junction VDMOS has been widely used in power supplies or adapters of consumer electronics products such as computers, mobile phones, lighting, LCD or plasma TVs and game consoles.

对于功率半导体器件,雪崩能量通常在非钳位感性开关UIS条件下测量,在UIS工作条件下的雪崩损坏有两种模式,热损坏和寄生三极管导通损坏。热损坏就是功率器件在功率脉冲的作用下,由于功耗增加导致结温升高,结温升高到硅片特性允许的临界值而导致的烧毁失效。 For power semiconductor devices, avalanche energy is usually measured under the condition of unclamped inductive switching UIS. There are two modes of avalanche damage under UIS operating conditions, thermal damage and parasitic transistor conduction damage. Thermal damage is the burning failure of power devices due to the increase in power consumption caused by the increase in junction temperature under the action of power pulses, and the junction temperature rises to the critical value allowed by the characteristics of the silicon chip.

VDMOS雪崩击穿时寄生BJT引起的二次击穿效应严重制约了VDMOS器件的雪崩能力,参见图1超结VDMOS的结构及寄生三极管示意图,Pbody区附近不可避免地寄生着一个双极型晶体管BJT,Pbody区构成寄生BJT的基区,同时寄生BJT的集电极与发射极也分别为VDMOS的漏极和源极,此外寄生BJT存在从VDMOS源极到Pbody区的等效电阻RB。当VDMOS处于阻断状态时,随着漏源电压的增加,器件内部电场逐渐增大,泄漏电流也随之增大。部分泄漏电流流过BJT体区时,等效电阻RB两端产生压降,该压降等于寄生三极管BJT的VBE,VDMOS接近雪崩击穿时,泄漏电流急剧增大,如果RB上的压降足够使得寄生三极管开启,寄生BJT将引起二次击穿效应。等效电阻RB随温度增加而增加,而发射极和基极的开启电压VBE随温度的增加而降低,因此,VDMOS的雪崩能力随温度的增加而降低。与双极型晶体管的二次击穿不同,VDMOS 的二次击穿一般只在处于高压、大电流工作状态时发生,不存在局部热点的作用。 The secondary breakdown effect caused by the parasitic BJT during VDMOS avalanche breakdown seriously restricts the avalanche capability of VDMOS devices. See Figure 1 for the structure of super-junction VDMOS and the schematic diagram of parasitic triodes. A bipolar transistor BJT is inevitably parasitic near the Pbody region. , the Pbody region constitutes the base region of the parasitic BJT, and the collector and emitter of the parasitic BJT are also the drain and source of the VDMOS respectively. In addition, the parasitic BJT has an equivalent resistance RB from the source of the VDMOS to the Pbody region. When VDMOS is in the blocking state, as the drain-source voltage increases, the internal electric field of the device gradually increases, and the leakage current also increases. When part of the leakage current flows through the body region of the BJT, a voltage drop occurs at both ends of the equivalent resistance RB , which is equal to the V BE of the parasitic transistor BJT. When VDMOS is close to avalanche breakdown, the leakage current increases sharply. The voltage drop is enough to turn on the parasitic triode, and the parasitic BJT will cause secondary breakdown effect. The equivalent resistance RB increases with temperature, and the turn-on voltage V BE of the emitter and base decreases with the increase of temperature. Therefore, the avalanche capability of VDMOS decreases with the increase of temperature. Unlike the secondary breakdown of bipolar transistors, the secondary breakdown of VDMOS generally only occurs when it is in a high-voltage, high-current working state, and there is no local hot spot.

当VDMOS发生雪崩击穿,寄生三极管被激活导通发生二次击穿时,VDMOS也有急剧的发热现象。在发生雪崩击穿时,器件温度与电流大小以及器件本身的性能有关。当器件发生雪崩击穿后,如果没有适当的缓冲、抑制改善措施,随着电压电流的增大,器件散热能力会越来越差,温度急剧升高,会导致器件的损坏。寄生三极管还可能引起功率MOSFET单粒子烧毁(SEB)现象,所谓单粒子烧毁是指其内部寄生三极管在重离子电离径迹诱导下被打开而形成的局部雪崩击穿现象,这种效应严重威胁航天和卫星电子系统的安全。 When the avalanche breakdown of VDMOS occurs and the parasitic triode is activated and turned on to cause secondary breakdown, VDMOS also has a sharp heating phenomenon. When avalanche breakdown occurs, the temperature of the device is related to the magnitude of the current and the performance of the device itself. When the device undergoes avalanche breakdown, if there is no proper buffering and suppression improvement measures, as the voltage and current increase, the heat dissipation capability of the device will become worse and worse, and the temperature will rise sharply, which will cause damage to the device. The parasitic triode may also cause the single event burnout (SEB) phenomenon of the power MOSFET. The so-called single event burnout refers to the local avalanche breakdown phenomenon formed by the internal parasitic triode being opened under the induction of the heavy ion ionization track. This effect seriously threatens aerospace. and the safety of satellite electronic systems.

抑制VDMOS二次击穿的主要措施有:增加Pbody的结深及浓度,减小电阻RB。对寄生BJT而言,通过增加Pbody浓度,即增加了基区的净参杂浓度QB,通过增加Pbody结深,对寄生BJT而言,即是增加了未耗尽的基区宽度W,都能减小电流放大系数β,二次击穿点随Pbody 浓度增加而提高。传统的解决方法是通过在P体区中深注入P+离子,但是这种结构使得P体区的结深变深,增加了VDMOS的导通电阻。1995年 K. Fischer与K. Shenai发表文章,提出了加一个自对准浅表面扩散P+区域,可以很有效地抑制寄生晶体管效应,并且在减小电流增益和基极电阻的同时,没有消耗额外的外延层厚度。但需要指出的是,虽然自对准浅表面扩散P+区域抑制了寄生效应且不增加元胞面积,却提高了穿通击穿的可能,因此生产时还需要结合具体器件工作条件要求进行权衡。 The main measures to suppress the secondary breakdown of VDMOS are: increase the junction depth and concentration of Pbody, and reduce the resistance RB . For parasitic BJT, by increasing the concentration of Pbody, the net doping concentration Q B of the base region is increased, and by increasing the junction depth of Pbody, for parasitic BJT, that is, the width W of the undepleted base region is increased. It can reduce the current amplification factor β, and the secondary breakdown point increases with the increase of Pbody concentration. The traditional solution is to implant P + ions deeply into the P body region, but this structure makes the junction depth of the P body region deeper and increases the on-resistance of VDMOS. In 1995, K. Fischer and K. Shenai published an article, which proposed that adding a self-aligned shallow surface diffusion P + region can effectively suppress the parasitic transistor effect, and reduce the current gain and base resistance without consuming Additional epi layer thickness. However, it should be pointed out that although the self-aligned shallow surface diffusion P + region suppresses the parasitic effect and does not increase the cell area, it increases the possibility of punch-through breakdown, so the production needs to be weighed in combination with the specific device working conditions.

雪崩击穿发生在元胞区比发生在终端区可以获得更好的可靠性,而元胞区的击穿电压相对于终端区的击穿电压可以更轻松的设计实现,因而为了提高超结器件的可靠性,适当地减小元胞区的击穿电压的设计裕量比进一步提高终端区的击穿电压更加容易。使用较高的P柱掺杂浓度可以适当地提高功率半导体器件的雪崩能力,但较高的P柱掺杂浓度加剧了横向扩散使得导通电阻相应增大,且P柱与N柱电荷的失衡使得击穿电压的降低。 Avalanche breakdown occurs in the cell region than in the terminal region to obtain better reliability, and the breakdown voltage of the cell region can be designed and realized more easily than that of the terminal region. Therefore, in order to improve the super junction device Therefore, it is easier to appropriately reduce the design margin of the breakdown voltage of the cell region than to further increase the breakdown voltage of the terminal region. Using a higher P-column doping concentration can appropriately improve the avalanche capability of power semiconductor devices, but a higher P-column doping concentration intensifies the lateral diffusion and increases the on-resistance accordingly, and the charge imbalance between the P-column and N-column resulting in a reduction in breakdown voltage.

发明内容 Contents of the invention

本发明所要解决的技术问题是提供了一种可改善雪崩能力的超结半导体器件的制备方法,此种方法所得的超结半导体器件在提高了超结半导体器件的雪崩能力同时减小了导通电阻。 The technical problem to be solved by the present invention is to provide a preparation method of a super junction semiconductor device that can improve the avalanche capability, and the super junction semiconductor device obtained by this method improves the avalanche capability of the super junction semiconductor device while reducing the conduction resistance.

为解决上述的技术问题,本发明采取的技术方案:一种可改善雪崩能力的超结半导体器件的制备方法,其特别之处在于:由以下步骤实现: In order to solve the above-mentioned technical problems, the technical solution adopted by the present invention is: a method for preparing a super junction semiconductor device capable of improving avalanche capability, which is special in that it is realized by the following steps:

步骤一、利用外延工艺,在N+衬底上形成一层3~10μm的N型外延层; Step 1. Using an epitaxial process, a layer of 3-10 μm N-type epitaxial layer is formed on the N + substrate;

步骤二、利用P柱掩膜板掩膜进行硼离子注入形成一层厚度为3~6μm的P型N型外延层; Step 2, using the P-pillar mask to perform boron ion implantation to form a P-type N-type epitaxial layer with a thickness of 3-6 μm;

步骤三、分别重复步骤一和步骤二5~10次,同时硼离子注入剂量逐次增加2%~8%,然后在900~1200℃高温下推结形成厚度为30~40μm的P型与N型交替的外延层,其中N型外延层的掺杂浓度范围为0.5~2.5×1015cm-3,元胞区P柱掺杂浓度范围为1.0~5.5×1015cm-3Step 3: Repeat step 1 and step 2 5-10 times respectively, while increasing the dose of boron ion implantation by 2%-8% step by step, and then push the junction at 900-1200°C to form a P-type and N-type with a thickness of 30-40μm Alternating epitaxial layers, wherein the doping concentration range of the N-type epitaxial layer is 0.5~2.5×10 15 cm -3 , and the doping concentration range of the P column in the cell area is 1.0~5.5×10 15 cm -3 ;

步骤四、采用50~200KeV的能量注入剂量为2~8×1013cm-2硼离子,并在900~1200℃的高温下推结60~200分钟形成Pbody区; Step 4: Using 50~200KeV energy implantation dose as 2~8×10 13 cm -2 boron ions, and pushing the junction at a high temperature of 900~1200°C for 60~200 minutes to form the Pbody region;

步骤五、在1000~1200℃温度下90分钟干氧生长50~200nm厚的栅氧化层(6),之后淀积200~800nm厚的多晶硅,并使用干法刻蚀多晶硅形成多晶硅栅电极; Step 5, growing a gate oxide layer (6) with a thickness of 50 to 200 nm in dry oxygen for 90 minutes at a temperature of 1000 to 1200 ° C, and then depositing polysilicon with a thickness of 200 to 800 nm, and etching the polysilicon by dry method to form a polysilicon gate electrode;

步骤六、采用80KeV的能量注入剂量为3×1015cm-2的砷离子,并在900℃的温度下推结30分钟形成N+源区; Step 6, using 80KeV energy to implant arsenic ions with a dose of 3×10 15 cm −2 , and pushing the junction at 900° C. for 30 minutes to form an N + source region;

步骤七、淀积2~4μm厚的BPSG层,在900~1000℃氮气氛围下回流30~60分钟,并刻蚀形成接触孔; Step 7, depositing a 2-4 μm thick BPSG layer, reflowing for 30-60 minutes under a nitrogen atmosphere at 900-1000°C, and etching to form a contact hole;

步骤八、在整个器件的上表面淀积一层铝,并刻蚀铝形成源金属电极,钝化,背面金属化形成漏电极。 Step 8: Deposit a layer of aluminum on the upper surface of the entire device, etch the aluminum to form a source metal electrode, passivate, and metallize the back to form a drain electrode.

所述步骤三通过调节P柱掩膜板来控制P柱不同区域的硼离子掺杂浓度,P柱中间掺杂浓度最高,掺杂浓度向两侧递减; In the third step, the doping concentration of boron ions in different regions of the P-pillar is controlled by adjusting the mask plate of the P-pillar. The doping concentration in the middle of the P-pillar is the highest, and the doping concentration decreases toward both sides;

所述步骤三中通过逐次增加硼离子的注入剂量来控制P柱纵向的掺杂浓度,P柱底部的掺杂浓度最低,掺杂浓度从下向上逐渐增高; In the step 3, the doping concentration in the longitudinal direction of the P column is controlled by increasing the implantation dose of boron ions successively, the doping concentration at the bottom of the P column is the lowest, and the doping concentration gradually increases from bottom to top;

每个P柱的P柱掩膜板均为一组相邻的图案组成,不同P柱的间隔大于P柱的宽度; The P-pillar mask of each P-pillar is composed of a group of adjacent patterns, and the interval between different P-pillars is greater than the width of the P-pillar;

每组P柱掩膜板的离子注入区域的图案为可制造的规则图案。 The pattern of the ion implantation region of each set of P-pillar mask plates is a manufacturable regular pattern.

每组P柱掩膜板的离子注入区域的图案的宽度从P柱中心向两侧逐渐递减。 The width of the pattern of the ion implantation region of each set of P-pillar mask plates gradually decreases from the center of the P-pillar to both sides.

所述可制造的规则图案条形、圆形或方形。 The manufacturable regular pattern is strip, circle or square.

与现有技术相比,本发明的有益效果: Compared with prior art, the beneficial effect of the present invention:

本发明的一种超结半导体器件的制备方法,将超结VDMOS器件P柱的纵向掺杂浓度由下到上逐渐递增,从而减小了源金属电极下面的寄生BJT的等效电阻RB的电阻值,并使得雪崩电流从寄生BJT的基区向沿着P柱的体内转移,从而极大程度地抑制了寄生BJT的发射结的开启,避免了寄生BJT的引起二次击穿;并且该P柱通过掩膜板来调节P柱中间与边缘的注入剂量,降低了P柱边缘区域的掺杂浓度,从而降低了P柱边缘处的掺杂浓度梯度,有效地减小了横向扩散的,因而增大了器件导通时的导电通道的有效宽度,从而在提高了超结半导体器件的雪崩能力同时减小了导通电阻;本发明兼容现有的多次外延多次注入工艺,在提升雪崩能力的同时没有增加工艺制造成本及工艺步骤。 A method for preparing a super-junction semiconductor device of the present invention gradually increases the vertical doping concentration of the P-column of the super-junction VDMOS device from bottom to top, thereby reducing the equivalent resistance RB of the parasitic BJT below the source metal electrode Resistance value, and make the avalanche current transfer from the base area of the parasitic BJT to the body along the P column, thereby greatly inhibiting the opening of the emitter junction of the parasitic BJT and avoiding the secondary breakdown caused by the parasitic BJT; and the The P column uses a mask to adjust the implantation dose in the middle and edge of the P column, which reduces the doping concentration in the edge area of the P column, thereby reducing the doping concentration gradient at the edge of the P column, effectively reducing the lateral diffusion. Therefore, the effective width of the conductive channel when the device is turned on is increased, thereby reducing the on-resistance while improving the avalanche capability of the superjunction semiconductor device; the present invention is compatible with the existing multiple epitaxy and multiple injection processes, and improves The avalanche capability does not increase the process manufacturing cost and process steps.

附图说明 Description of drawings

图1是现有超结半导体器件的结构及寄生三极管等效结构示意图; FIG. 1 is a schematic diagram of the structure of an existing super-junction semiconductor device and the equivalent structure of a parasitic triode;

图2是本发明的多次外延多次注入工艺形成的超结半导体器件的剖面结构示意图; Fig. 2 is a schematic cross-sectional structure diagram of a super junction semiconductor device formed by multiple epitaxy and multiple implantation processes of the present invention;

图3是本发明的元胞区的P柱光刻掩膜板结构示意图; Fig. 3 is a schematic structural diagram of a P-pillar photolithography mask plate in the cell region of the present invention;

图4是沿着图2中AA’线的净掺杂浓度分布图; Fig. 4 is the net doping concentration distribution figure along AA ' line in Fig. 2;

图5是沿着图2中BB’线的净掺杂浓度分布图。 Fig. 5 is a diagram of net doping concentration distribution along line BB' in Fig. 2 .

其中,1、N+衬底、2、N型外延层、3、P柱、4、Pbody区、5、N+源区、6、栅氧化层、7、多晶硅栅电极、8、BPSG介质层、9、源金属电极、10、硼离子注入区域。 Among them, 1. N + substrate, 2, N-type epitaxial layer, 3, P column, 4, Pbody region, 5, N + source region, 6, gate oxide layer, 7, polysilicon gate electrode, 8, BPSG dielectric layer , 9, source metal electrode, 10, boron ion implantation region.

具体实施方式 detailed description

下面结合附图和具体实施方式对本发明进行详细说明。 The present invention will be described in detail below in conjunction with the accompanying drawings and specific embodiments.

一种可改善雪崩能力的超结半导体器件的制备方法,由以下步骤实现: A method for preparing a super junction semiconductor device capable of improving avalanche capability, which is realized by the following steps:

步骤一、利用外延工艺,在N+衬底1上形成一层3~10μm的N型外延层2; Step 1. Using an epitaxial process, a layer of 3-10 μm N-type epitaxial layer 2 is formed on the N + substrate 1;

步骤二、利用P柱掩膜板掩膜进行硼离子注入形成一层厚度为3~6μm的P型N型外延层; Step 2, using the P-pillar mask to perform boron ion implantation to form a P-type N-type epitaxial layer with a thickness of 3-6 μm;

步骤三、分别重复步骤一和步骤二5~10次,同时硼离子注入剂量逐次增加2%-8%,然后在900~1200℃高温下推结形成厚度为30~40μm的P型与N型交替的外延层,其中N型外延层2的掺杂浓度范围为0.5~2.5×1015cm-3,元胞区P柱掺杂浓度范围为1.0~5.5×1015cm-3Step 3: Repeat step 1 and step 2 5-10 times respectively, while increasing the dose of boron ion implantation by 2%-8% step by step, and then push the junction at 900-1200°C to form a P-type and N-type with a thickness of 30-40μm Alternating epitaxial layers, wherein the doping concentration range of the N-type epitaxial layer 2 is 0.5~2.5×10 15 cm -3 , and the doping concentration range of the P column in the cell region is 1.0~5.5×10 15 cm -3 ;

步骤四、采用50~200KeV的能量注入剂量为2~8×1013cm-2硼离子,并在900~1200℃的高温下推结60~200分钟形成Pbody区4; Step 4: Using 50-200KeV energy implant dose to be 2-8×10 13 cm -2 boron ions, and pushing the junction at a high temperature of 900-1200°C for 60-200 minutes to form Pbody region 4;

步骤五、在1000~1200℃温度下90分钟干氧生长50~200nm厚的栅氧化层6,之后淀积200~800nm厚的多晶硅,并使用干法刻蚀多晶硅形成多晶硅栅电极7; Step 5, growing a gate oxide layer 6 with a thickness of 50 to 200 nm in dry oxygen for 90 minutes at a temperature of 1000 to 1200 ° C, and then depositing polysilicon with a thickness of 200 to 800 nm, and etching the polysilicon by dry method to form a polysilicon gate electrode 7 ;

步骤六、采用80KeV的能量注入剂量为3×1015cm-2的砷离子,并在900℃的温度下推结30分钟形成N+源区5; Step 6: Implanting arsenic ions with a dose of 3×10 15 cm -2 with an energy of 80 KeV, and pushing the junction at 900° C. for 30 minutes to form an N + source region 5 ;

步骤七、淀积2~4μm厚的BPSG层,在900~1000℃氮气氛围下回流30~60分钟,并刻蚀形成接触孔; Step 7, depositing a 2-4 μm thick BPSG layer, reflowing for 30-60 minutes under a nitrogen atmosphere at 900-1000°C, and etching to form a contact hole;

步骤八、在整个器件的上表面淀积一层铝,并刻蚀铝形成源金属电极,钝化,背面金属化形成漏金属电极9。 Step 8: Deposit a layer of aluminum on the upper surface of the entire device, etch the aluminum to form a source metal electrode, passivate, and metallize the back to form a drain metal electrode 9 .

所述步骤三通过调节P柱掩膜板来控制P柱不同区域的硼离子掺杂浓度,P柱中间掺杂浓度最高,掺杂浓度向两侧递减。 In the third step, the doping concentration of boron ions in different regions of the P-pillar is controlled by adjusting the mask plate of the P-pillar.

所述步骤三中通过逐次增加硼离子的注入剂量来控制P柱纵向的掺杂浓度,P柱底部的掺杂浓度最低,掺杂浓度从下向上逐渐增高。 In the third step, the doping concentration in the longitudinal direction of the P column is controlled by increasing the implantation dose of boron ions successively, the doping concentration at the bottom of the P column is the lowest, and the doping concentration gradually increases from bottom to top.

每个P柱的P柱掩膜板均为一组相邻的图案组成,不同P柱的间隔大于P柱的宽度。 The P-pillar mask of each P-pillar is composed of a group of adjacent patterns, and the interval between different P-pillars is greater than the width of the P-pillar.

每组P柱掩膜板的离子注入区域的图案可以为条形、圆形或方形及其它可制造的规则图案。 The pattern of the ion implantation area of each group of P-pillar mask plates can be strip, circle or square or other manufacturable regular patterns.

每组P柱掩膜板的离子注入区域的图案的宽度从P柱中心向两侧逐渐递减。 The width of the pattern of the ion implantation region of each set of P-pillar mask plates gradually decreases from the center of the P-pillar to both sides.

通过调整P柱掩膜板的离子注入图形的大小、数目与间距从而来控制P柱不同区域的硼离子掺杂浓度,P柱掩膜板中间条形图案最宽,图案宽度向P柱两侧依次递减,使得掺杂后得到的离子数目中间最多,依次向两侧递减。 By adjusting the size, number and spacing of the ion implantation patterns of the P-pillar mask, the boron ion doping concentration in different regions of the P-pillar is controlled. The strip pattern in the middle of the P-pillar mask is the widest, and the width of the pattern extends to both sides of the P-pillar. Decrease in order, so that the number of ions obtained after doping is the largest in the middle, and then decrease to both sides.

本发明的工作原理是:源金属电极9下面P柱顶端的掺杂浓度最高,从而减小了源金属电极9下面的寄生BJT的等效电阻RB的电阻值,并使得雪崩电流从寄生BJT的基区向沿着P柱的体内转移,从而极大程度地抑制了寄生BJT的发射结的开启,避免了寄生BJT的引起二次击穿;通过调整P柱掩膜板的图形,采用不连续的掩膜板图形,使得P柱3的中部注入硼离子剂量最大,通过长时间高温推结其横向掺杂浓度向两侧逐渐递减,调节P柱中间与P柱的边缘的掺杂浓度,有效地减小了横向扩散的,增大了器件导通时的导电通道的有效宽度,从而在提高了超结半导体器件的雪崩能力同时减小了导通电阻。 The working principle of the present invention is: the doping concentration at the top of the P column below the source metal electrode 9 is the highest, thereby reducing the resistance value of the equivalent resistance RB of the parasitic BJT below the source metal electrode 9, and making the avalanche current flow from the parasitic BJT The base region of the P-pillar is transferred to the body along the P-pillar, thereby greatly suppressing the opening of the emitter junction of the parasitic BJT and avoiding the secondary breakdown caused by the parasitic BJT; by adjusting the pattern of the P-pillar mask, different The continuous pattern of the mask makes the dose of boron ions implanted in the middle of the P-pillar 3 the largest, and its lateral doping concentration gradually decreases to both sides through long-term high-temperature push junction, and the doping concentration in the middle of the P-pillar and the edge of the P-pillar is adjusted. The lateral diffusion is effectively reduced, and the effective width of the conduction channel when the device is turned on is increased, thereby improving the avalanche capability of the super junction semiconductor device and reducing the on-resistance at the same time.

参见图1,超结VDMOS的结构中本征地寄生着双极型晶体管NPN结构,为避免该寄生三极管开启,必须减小其基极等效电阻RB的两端的压降使其发射结无法开启。 See Figure 1. In the structure of the super-junction VDMOS, there is an intrinsically parasitic bipolar transistor NPN structure. In order to prevent the parasitic transistor from being turned on, the voltage drop across the base equivalent resistance RB must be reduced so that the emitter junction cannot be turned on. .

参见图2,本发明的超结器件采用了一种不均匀掺杂P柱,该P柱的掺杂浓度沿着AA’线及BB’线方向都不均匀。 Referring to Fig. 2, the super junction device of the present invention adopts a non-uniformly doped P column, and the doping concentration of the P column is not uniform along the directions of the AA' line and the BB' line.

参见图3,本发明的超结器件采用的不均匀掺杂P柱的掩膜版,采用不连续的掩膜板图形,通过调整P柱掩膜板的图形,由于采用负性光刻胶,因而P柱中部的离子注入的区域最大,从而使得P柱的中部注入硼离子剂量最大,通过长时间高温推结其横向掺杂浓度从中间向两侧逐渐递减,图中填充区为硼离子注入区域。 Referring to Fig. 3, the mask of the unevenly doped P-column used in the superjunction device of the present invention adopts a discontinuous mask pattern, and by adjusting the pattern of the P-column mask, due to the use of negative photoresist, Therefore, the ion implantation area in the middle of the P column is the largest, so that the dose of boron ions implanted in the middle of the P column is the largest. After a long time and high temperature, the lateral doping concentration gradually decreases from the middle to both sides. The filling area in the figure is boron ion implantation. area.

参见图4,图1中所示AA’线经过长时间高温推结后P柱掺杂浓度从中间向两侧逐渐递减,调节P柱中间与P柱的边缘的掺杂浓度,有效地减小了横向扩散的,增大了器件导通时的导电通道的有效宽度,从而在提高了超结半导体器件的雪崩能力同时减小了导通电阻。 See Figure 4. The doping concentration of the P column gradually decreases from the middle to both sides after the AA' line shown in Figure 1 has been pushed for a long time at high temperature, and the doping concentration in the middle of the P column and the edge of the P column is adjusted to effectively reduce the The lateral diffusion increases the effective width of the conduction channel when the device is turned on, thereby improving the avalanche capability of the super junction semiconductor device and reducing the on-resistance at the same time.

参见图5,图1中所示BB’线所示P柱的掺杂浓度由表面到体内逐渐递减,源金属电极下面P柱顶端的掺杂浓度最高,从而减小了源金属电极下面的寄生BJT的等效电阻RB的电阻值,并使得雪崩电流从寄生BJT的基区向沿着P柱的体内转移,从而极大程度地抑制了寄生BJT的发射结的开启,避免了寄生BJT的引起二次击穿。 Referring to Fig. 5, the doping concentration of the P-pillar indicated by line BB' in Fig. 1 gradually decreases from the surface to the body, and the doping concentration at the top of the P-pillar under the source metal electrode is the highest, thereby reducing the parasitic under the source metal electrode. The resistance value of the equivalent resistance R B of the BJT, and makes the avalanche current transfer from the base area of the parasitic BJT to the body along the P column, thereby greatly inhibiting the opening of the emitter junction of the parasitic BJT and avoiding the parasitic BJT cause secondary breakdown.

实施例: Example:

本实施例采用用具有超结结构的MOSFET来说明,但本发明不局限于MOSFET。 This embodiment is described using a MOSFET having a superjunction structure, but the present invention is not limited to MOSFETs.

一、衬底材料准备,采用电阻率为0.001Ω· cm的N+区熔单晶硅衬底1,其晶向为<100>; 1. Substrate material preparation, using an N + zone-fused monocrystalline silicon substrate 1 with a resistivity of 0.001Ω·cm, and its crystal orientation is <100>;

二、在N+衬底上外延生长5μm电阻率为4Ω· cm的N型外延层,作为P柱与N+衬底间的缓冲层; 2. Epitaxially grow a 5 μm N-type epitaxial layer with a resistivity of 4Ω·cm on the N + substrate as a buffer layer between the P column and the N + substrate;

三、在硅片表面外延生长5μm电阻率为4Ω· cm的N型外延层; 3. Epitaxial growth of a 5 μm N-type epitaxial layer with a resistivity of 4Ω·cm on the surface of the silicon wafer;

四、在硅片表面淀积6μm的负性光刻胶(即有P柱图形的地方进行硼离子注入),使用P柱掩膜板进行曝光并显影,然后进行四次高能硼离子注入,注入硼离子能量依次采用3.5MeV、2.5MeV、1.2KeV与200KeV,注入的硼离子剂量均为6×1011cm-24. Deposit 6 μm negative photoresist on the surface of the silicon wafer (i.e., perform boron ion implantation where there is a P-pillar pattern), use a P-pillar mask to expose and develop, and then perform four high-energy boron ion implantations. The energy of boron ions is 3.5MeV, 2.5MeV, 1.2KeV and 200KeV in sequence, and the dose of implanted boron ions is 6×10 11 cm -2 ;

五、重复6次步骤三和步骤四,但是重复步骤四时注入的硼离子剂量每次在前一次注入的基础上增加5%的硼离子剂量,最后在1100℃温度的氮气氛围下进行30分钟的高温推结,形成长度约为35μm的连续P柱,其中N型外延层的典型掺杂浓度为1.1×1015cm-3,元胞区P柱典型掺杂浓度为3.6×1015cm-35. Repeat step 3 and step 4 6 times, but the dose of boron ions implanted when repeating step 4 is increased by 5% of the dose of boron ions on the basis of the previous implantation each time, and finally carried out in a nitrogen atmosphere at a temperature of 1100 ° C for 30 minutes The high-temperature pushing junction forms a continuous P column with a length of about 35 μm, where the typical doping concentration of the N-type epitaxial layer is 1.1×10 15 cm -3 , and the typical doping concentration of the P column in the cell region is 3.6×10 15 cm - 3 ;

六、采用120KeV的能量注入剂量为5.2×1013cm-2硼离子,并在1000℃的高温下推结120分钟形成Pbody区4; 6. The energy implant dose of 120KeV is 5.2×10 13 cm -2 boron ions, and the Pbody region 4 is formed at a high temperature of 1000°C for 120 minutes;

七、在1100℃温度下90分钟干氧生长100nm厚的栅氧化层6,之后淀积400nm厚的多晶硅,并使用干法刻蚀多晶硅形成多晶硅栅电极7; 7. Dry oxygen growth of a gate oxide layer 6 with a thickness of 100 nm at a temperature of 1100° C. for 90 minutes, and then deposit polysilicon with a thickness of 400 nm, and dry-etch the polysilicon to form a polysilicon gate electrode 7;

八、采用80KeV的能量注入剂量为3×1015cm-2的砷离子,并在900℃的温度下推结30分钟形成N+源区5; 8. Using 80KeV energy to implant arsenic ions with a dose of 3×10 15 cm -2 , and pushing the junction at 900° C. for 30 minutes to form N + source region 5 ;

九、淀积2μm厚的BPSG层8,在950℃氮气氛围下回流30分钟,并刻蚀形成接触孔; 9. Deposit a BPSG layer 8 with a thickness of 2 μm, reflow for 30 minutes under a nitrogen atmosphere at 950° C., and etch to form a contact hole;

十、在整个器件的上表面淀积一层铝,并刻蚀铝形成源金属电极9,钝化,背面金属化形成漏电极。 10. Deposit a layer of aluminum on the upper surface of the entire device, etch the aluminum to form the source metal electrode 9, passivate, and metallize the back to form the drain electrode.

本发明可以形成从源端表面到外延层内部掺杂浓度逐步递减的P柱,使得寄生三极管效应得到抑制,从而改善了超结半导体器件的雪崩能力,并且有效地减小了P柱的横向扩散,增大了器件导通时的导电通道的横向宽度,使得器件的导通电阻得到了减小。 The present invention can form a P column whose doping concentration gradually decreases from the surface of the source end to the interior of the epitaxial layer, so that the parasitic triode effect is suppressed, thereby improving the avalanche capability of the super junction semiconductor device, and effectively reducing the lateral diffusion of the P column , increasing the lateral width of the conductive channel when the device is turned on, so that the on-resistance of the device is reduced.

Claims (6)

1.一种可改善雪崩能力的超结半导体器件的制备方法,其特征在于:由以下步骤实现: 1. A method for preparing a superjunction semiconductor device capable of improving avalanche capability, characterized in that: it is realized by the following steps: 步骤一、利用外延工艺,在N+衬底(1)上形成一层3~10μm的N型外延层(2); Step 1. Using an epitaxial process, a layer of 3-10 μm N-type epitaxial layer (2) is formed on the N + substrate (1); 步骤二、利用P柱掩膜板掩膜进行硼离子注入形成一层厚度为3~6μm的P型区域; Step 2, using the P-pillar mask to perform boron ion implantation to form a P-type region with a thickness of 3-6 μm; 步骤三、分别重复步骤一和步骤二5~10次,同时硼离子注入剂量逐次增加2%~8%,然后在900~1200℃高温下推结形成厚度为30~40μm的P型与N型交替的外延层,其中N型外延层(2)的掺杂浓度范围为0.5~2.5×1015cm-3,元胞区P柱掺杂浓度范围为1.0~5.5×1015cm-3Step 3: Repeat step 1 and step 2 5-10 times respectively, while increasing the dose of boron ion implantation by 2%-8% step by step, and then push the junction at 900-1200°C to form a P-type and N-type with a thickness of 30-40μm Alternating epitaxial layers, wherein the doping concentration of the N-type epitaxial layer (2) ranges from 0.5 to 2.5×10 15 cm -3 , and the doping concentration of P columns in the cell region ranges from 1.0 to 5.5×10 15 cm -3 ; 步骤四、采用50~200KeV的能量注入剂量为2~8×1013cm-2硼离子,并在900~1200℃的高温下推结60~200分钟形成Pbody区(4); Step 4: Using 50~200KeV energy implantation dose as 2~8×10 13 cm -2 boron ions, and pushing the junction at a high temperature of 900~1200°C for 60~200 minutes to form the Pbody region (4); 步骤五、在1000~1200℃温度下90分钟干氧生长50~200nm厚的栅氧化层(6),之后淀积200~800nm厚的多晶硅,并使用干法刻蚀多晶硅形成多晶硅栅电极(7); Step 5. Dry oxygen growth of 50-200nm thick gate oxide layer (6) at a temperature of 1000-1200°C for 90 minutes, and then deposit polysilicon with a thickness of 200-800nm, and dry-etch the polysilicon to form a polysilicon gate electrode (7 ); 步骤六、采用80KeV的能量注入剂量为3×1015cm-2的砷离子,并在900℃的温度下推结30分钟形成N+源区(5); Step 6: Implanting arsenic ions with a dose of 3×10 15 cm −2 with 80 KeV energy, and pushing the junction at 900° C. for 30 minutes to form an N + source region ( 5 ); 步骤七、淀积2~4μm厚的BPSG层,在900~1000℃氮气氛围下回流30~60分钟,并刻蚀形成接触孔; Step 7, depositing a 2-4 μm thick BPSG layer, reflowing for 30-60 minutes under a nitrogen atmosphere at 900-1000°C, and etching to form a contact hole; 步骤八、在整个器件的上表面淀积一层铝,并刻蚀铝形成源金属电极(9),钝化,背面金属化形成漏电极; Step 8. Deposit a layer of aluminum on the upper surface of the entire device, etch the aluminum to form a source metal electrode (9), passivate, and metallize the back to form a drain electrode; 所述步骤三通过调节P柱掩膜板来控制P柱(3)不同区域的硼离子掺杂浓度,P柱(3)中间掺杂浓度最高,掺杂浓度向两侧递减。 In the third step, the doping concentration of boron ions in different regions of the P-pillar (3) is controlled by adjusting the mask plate of the P-pillar. 2.根据权利要求1所述的可改善雪崩能力的超结半导体器件的制备方法,其特征在于:所述步骤三中通过逐次增加硼离子的注入剂量来控制P柱(3)纵向的掺杂浓度,P柱(3)底部的掺杂浓度最低,掺杂浓度从下向上逐渐增高。 2. The method for manufacturing a super-junction semiconductor device capable of improving avalanche capability according to claim 1, characterized in that: in the third step, the doping in the vertical direction of the P column (3) is controlled by increasing the implantation dose of boron ions successively Concentration, the doping concentration at the bottom of the P column (3) is the lowest, and the doping concentration gradually increases from bottom to top. 3.根据权利要求1或2所述的可改善雪崩能力的超结半导体器件的制备方法,其特征在于:每个P柱(3)的P柱掩膜板均为一组相邻的图案组成,不同P柱的间隔大于P柱(3)的宽度。 3. The method for manufacturing a super-junction semiconductor device capable of improving avalanche capability according to claim 1 or 2, characterized in that: the P-pillar mask of each P-pillar (3) is composed of a group of adjacent patterns , the interval between different P columns is greater than the width of the P column (3). 4.根据权利要求3所述的可改善雪崩能力的超结半导体器件的制备方法,其特征在于:每组P柱掩膜板的离子注入区域的图案为可制造的规则图案。 4 . The method for manufacturing a superjunction semiconductor device capable of improving avalanche capability according to claim 3 , wherein the pattern of the ion implantation region of each group of P-pillar mask plates is a manufacturable regular pattern. 5.根据权利要求4所述的可改善雪崩能力的超结半导体器件的制备方法,其特征在于:每组P柱掩膜板的离子注入区域的图案的宽度从P柱中心向两侧逐渐递减。 5. The method for preparing a superjunction semiconductor device capable of improving avalanche capability according to claim 4, characterized in that: the width of the pattern of the ion implantation region of each group of P-pillar mask plates gradually decreases from the center of the P-pillar to both sides . 6.根据权利要求4所述的可改善雪崩能力的超结半导体器件的制备方法,其特征在于:所述可制造的规则图案是条形、圆形或方形。 6 . The method for manufacturing a super junction semiconductor device capable of improving avalanche capability according to claim 4 , wherein the manufacturable regular patterns are strips, circles or squares.
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