CN102969244B - SJ-insulated gate bipolar transistor (SJ-IGBT) device structure and manufacturing method thereof - Google Patents
SJ-insulated gate bipolar transistor (SJ-IGBT) device structure and manufacturing method thereof Download PDFInfo
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Abstract
本发明提供一种SJ-IGBT器件结构及其制作方法,包括以下步骤:提供一衬底;在该衬底上形成漂移区并在该漂移区预设源端和漏端;提供一设有若干第一窗口的第一掩膜版,所述第一窗口的宽度沿源端到漏端方向依次增大;自上述第一窗口向所述漂移区进行N型离子注入;退火,在该漂移区形成离子浓度呈线性增加的N型漂移区;提供一设有若干第二窗口的第二掩膜版;自该第二窗口向所述N型漂移区进行P型离子注入,P型柱区离漏极区有一定距离,退火后形成间隔的P柱和N柱;最后形成沟道、源区、漏区和栅区域。本发明使N柱的浓度从源端到漏端逐渐增加,消除漂移区剩余电荷,由于P柱离漏极有一定的距离,因此降低了漂移区电荷不平衡对器件性能的影响,提高可靠性。<!--1-->
The present invention provides a SJ-IGBT device structure and its manufacturing method, comprising the following steps: providing a substrate; forming a drift region on the substrate and preset source and drain ends in the drift region; providing a device with several The first mask plate of the first window, the width of the first window increases sequentially along the direction from the source end to the drain end; N-type ion implantation is performed from the first window to the drift region; annealing, in the drift region Forming an N-type drift region in which the ion concentration increases linearly; providing a second mask with a plurality of second windows; performing P-type ion implantation from the second windows to the N-type drift region, and the P-type column region is separated from There is a certain distance between the drain region, and after annealing, a spaced P column and an N column are formed; finally, a channel, a source region, a drain region and a gate region are formed. The invention gradually increases the concentration of the N column from the source end to the drain end, eliminates the residual charge in the drift region, and because the P column has a certain distance from the drain, it reduces the influence of the charge imbalance in the drift area on the performance of the device, and improves reliability . <!--1-->
Description
技术领域 technical field
本发明介绍了一种SJ-IGBT器件结构,属于微电子与固体电子学技术领域。The invention introduces a SJ-IGBT device structure, which belongs to the technical field of microelectronics and solid electronics.
背景技术 Background technique
功率集成电路有时也称高压集成电路,是现代电子学的重要分支,可为各种功率变换和能源处理装置提供高速、高集成度、低功耗和抗辐照的新型电路,广泛应用于电力控制系统、汽车电子、显示器件驱动、通信和照明等日常消费领域以及国防、航天等诸多重要领域。其应用范围的迅速扩大,对其核心部分的高压器件也提出了更高的要求。Power integrated circuits are sometimes called high-voltage integrated circuits, which are an important branch of modern electronics. They can provide new circuits with high speed, high integration, low power consumption and radiation resistance for various power conversion and energy processing devices, and are widely used in electric power Daily consumption fields such as control systems, automotive electronics, display device drivers, communications and lighting, as well as many important fields such as national defense and aerospace. The rapid expansion of its application scope has also put forward higher requirements for the high-voltage devices in its core part.
对功率器件MOSFET而言,在保证击穿电压的前提下,必须尽可能地降低器件的导通电阻来提高器件性能。但击穿电压和导通电阻之间存在一种近似平方关系,形成所谓的“硅限”。为了解决这一矛盾,前人提出了基于三维RESURF技术的漂移区由P、N柱相间构成的超结结构(SJ)用于优化高压器件的漂移区电场分布。该结构在保持导通电阻不变的前提下,提高击穿电压,打破传统功率MOS器件理论的极限。该技术的理论基础是电荷补偿理论,当漂移区施加电压达到一定值时,漂移区达到完全耗尽,电场分布更加均匀,提高了器件的抗击穿能力。在保证击穿电压不变的前提下,可以大幅提高漂移区的掺杂浓度,减小导通电阻。超结结构的提出打破了传统功率MOSFET器件的“硅极限” 。For the power device MOSFET, under the premise of ensuring the breakdown voltage, the on-resistance of the device must be reduced as much as possible to improve the performance of the device. But there is an approximate quadratic relationship between breakdown voltage and on-resistance, forming the so-called "silicon limit". In order to solve this contradiction, the predecessors proposed a superjunction structure (SJ) in which the drift region is composed of P and N columns based on the three-dimensional RESURF technology to optimize the electric field distribution in the drift region of high-voltage devices. Under the premise of keeping the on-resistance constant, this structure increases the breakdown voltage and breaks the theoretical limit of traditional power MOS devices. The theoretical basis of this technology is the charge compensation theory. When the voltage applied to the drift region reaches a certain value, the drift region is completely exhausted, and the electric field distribution is more uniform, which improves the breakdown resistance of the device. Under the premise of keeping the breakdown voltage unchanged, the doping concentration of the drift region can be greatly increased to reduce the on-resistance. The proposal of the super junction structure breaks the "silicon limit" of traditional power MOSFET devices.
SJ结构形成在器件的漂移层中,该漂移层包括N导电类型柱(column)(N柱)和P导电类型柱(column)(P柱)。N柱和P柱构成作为一对SJ结构的单元,从而多对N柱和P柱提供SJ结构。SJ结构最初应用于垂直VDMOS器件,后来扩展到横向LDMOS器件。横向结构更有利于新一代的高密度功率集成应用,是当代功率器件研究的热点。但是超结结构用于横向器件也带来了新的问题。第一,理想的能完全耗尽的p、n柱区工艺上难于形成。第二,衬底参与超结柱区的耗尽导致衬底辅助耗尽效应,而且耗尽层的宽度在器件的漏端到源端方向的不同位置不等,这就带来了漂移区电场分布不均的问题,需要对器件制作工艺和结构进行优化。The SJ structure is formed in a drift layer of the device, which includes N conductivity type columns (N columns) and P conductivity type columns (P columns). N-pillars and P-pillars constitute a unit as a pair of SJ structures, so that multiple pairs of N-pillars and P-pillars provide an SJ structure. The SJ structure was initially applied to vertical VDMOS devices and later extended to lateral LDMOS devices. The lateral structure is more conducive to the new generation of high-density power integration applications, and is a hot spot in the research of contemporary power devices. However, the use of superjunction structures in lateral devices also brings new problems. First, it is difficult to form ideal p and n column regions that can be completely depleted. Second, the depletion of the substrate participating in the superjunction column region leads to the substrate-assisted depletion effect, and the width of the depletion layer varies in different positions from the drain to the source of the device, which brings the electric field in the drift region The problem of uneven distribution requires optimization of the device manufacturing process and structure.
发明内容 Contents of the invention
鉴于以上所述现有技术的缺点,本发明的目的在于提供一种SJ-IGBT器件结构的制备方法,用于解决现有技术中漂移区电场分布不均的问题。In view of the shortcomings of the prior art described above, the purpose of the present invention is to provide a method for fabricating an SJ-IGBT device structure, which is used to solve the problem of uneven electric field distribution in the drift region in the prior art.
为实现上述目的及其他相关目的,本发明提供一种SJ-IGBT器件结构的制备方法,该方法包括以下步骤:In order to achieve the above purpose and other related purposes, the present invention provides a method for preparing a SJ-IGBT device structure, the method comprising the following steps:
提供一衬底;providing a substrate;
在该衬底上形成漂移区并在该漂移区预设源端和漏端;forming a drift region on the substrate and presetting a source terminal and a drain terminal in the drift region;
提供一设有若干第一窗口的第一掩膜版,所述第一窗口的宽度沿源端到漏端方向依次增大;providing a first mask plate provided with several first windows, the width of the first windows increases sequentially along the direction from the source end to the drain end;
将该掩膜版放置于所述漂移区之上,掩膜版和该漂移区左侧平齐,The mask plate is placed on the drift area, the mask plate is flush with the left side of the drift area,
自上述第一窗口向所述漂移区进行N型离子注入;performing N-type ion implantation from the first window to the drift region;
退火,在该漂移区形成沿源端到漏端方向N型载流子浓度呈线性增加的N型漂移区;Annealing, forming an N-type drift region in which the concentration of N-type carriers increases linearly from the source end to the drain end in the drift region;
提供一设有若干第二窗口的第二掩膜版;所述第二窗口的左侧自与源端相邻的位置,即与第一掩膜版的第一个遮挡部左侧平齐起始,截止于所述漏端附近,但是离漏端有一定的距离Provide a second reticle with several second windows; the left side of the second window is from the position adjacent to the source end, that is, flush with the left side of the first shielding part of the first reticle start and end near the drain end, but there is a certain distance from the drain end
自该第二窗口向所述N型漂移区采用三次能量和剂量依次减小的方式进行P型离子注入,形成间隔的P柱和N柱;且P柱不和漏端相连;Performing P-type ion implantation from the second window to the N-type drift region in a manner of decreasing energy and dose successively three times to form spaced P columns and N columns; and the P columns are not connected to the drain end;
最后形成沟道、源区、漏区和栅区域。Finally, channel, source, drain and gate regions are formed.
优选地,所述退火时间为600~1000分钟。所述退火温度为1000~1400度。Preferably, the annealing time is 600-1000 minutes. The annealing temperature is 1000-1400 degrees.
优选地,所述P型离子注入的三次剂量总和为N型离子注入的1.5-2.5倍,优选2倍。Preferably, the sum of the three doses of the P-type ion implantation is 1.5-2.5 times, preferably 2 times, that of the N-type ion implantation.
优选地,所述衬底为硅或SOI。Preferably, the substrate is silicon or SOI.
优选地,所述漏区为重掺杂P。Preferably, the drain region is heavily doped with P.
本发明还提供一种SJ-IGBT器件结构,该结构包括衬底;位于该衬底上的漂移区;位于该漂移区上方的栅区域、位于该漂移区两端的源端、漏端以及位于该源端和漏端之间间隔设置的若干P柱和N柱;且P柱不和漏端相连;所述P柱和N柱纵长方向与源、漏区纵长方向垂直;所述N柱沿源端到漏端方向离子浓度呈线性增加。The present invention also provides an SJ-IGBT device structure, which comprises a substrate; a drift region located on the substrate; a gate region located above the drift region, a source terminal and a drain terminal located at both ends of the drift region; A plurality of P columns and N columns arranged at intervals between the source terminal and the drain terminal; and the P column is not connected to the drain terminal; the longitudinal direction of the P column and the N column is perpendicular to the longitudinal direction of the source and drain regions; the N column The ion concentration increases linearly from source to drain.
优选地,所述衬底为硅或SOI。所述栅区域包括栅介质层以及位于栅介质层上的栅极。Preferably, the substrate is silicon or SOI. The gate region includes a gate dielectric layer and a gate located on the gate dielectric layer.
传统超结器件漂移区中交替存在的P和N柱区,为了提高耐压,要求N柱区和P柱区达到电荷平衡,在器件反向耐压时漂移区实现全耗尽,但是由于存在衬底辅助耗尽效应,引起P型柱区出现剩余电荷,本发明采用线性漂移区的N柱区取代传统的均匀分布的N型漂移区。可以有效的消除衬底辅助耗尽效应,提高器件的击穿电压。P and N column regions alternately exist in the drift region of traditional superjunction devices. In order to improve the withstand voltage, the N column region and the P column region are required to achieve charge balance. Substrate-assisted depletion effect causes residual charges to appear in the P-type column region. The present invention uses the N-column region in the linear drift region to replace the traditional uniformly distributed N-type drift region. It can effectively eliminate the substrate-assisted depletion effect and improve the breakdown voltage of the device.
本发明使N柱的浓度从源端到漏端逐渐增加,消除漂移区剩余电荷。同时,通过将漏极N+区换成P+区,器件工作时,重掺杂P区向漂移区注入空穴,增加漂移区电流能力,更好的降低器件开态电阻,由于P型柱区离漏极有一定的距离,因此降低了电荷不平衡对器件性能的影响,提高器件可靠性。The invention gradually increases the concentration of the N column from the source end to the drain end, and eliminates the residual charge in the drift region. At the same time, by replacing the N+ region of the drain with a P+ region, when the device is working, the heavily doped P region injects holes into the drift region, increasing the current capability of the drift region, and better reducing the on-state resistance of the device. There is a certain distance between the drains, thus reducing the impact of charge imbalance on device performance and improving device reliability.
附图说明 Description of drawings
图1a显示为本发明N型离子注入的结构示意图。Fig. 1a shows a schematic diagram of the structure of N-type ion implantation in the present invention.
图1b显示为图1的俯视图。Figure 1b shows a top view of Figure 1 .
图2显示为经退火再分布形成的线性N型漂移区结构示意图。FIG. 2 is a schematic diagram showing the structure of a linear N-type drift region formed by annealing and redistribution.
图3a显示为形成P柱区结构示意图。Figure 3a shows a schematic diagram of the structure for forming the P-pillar region.
图3b显示为图3a的俯视图。Figure 3b shows a top view of Figure 3a.
图4显示为P阱注入形成沟道的结构示意图。FIG. 4 shows a schematic diagram of the structure of a channel formed by P-well implantation.
图5显示为栅极形成的结构示意图。FIG. 5 shows a schematic diagram of the structure formed for the gate.
图6显示为形成重掺杂N区的结构示意图。FIG. 6 shows a schematic diagram of the structure for forming a heavily doped N region.
图7显示为形成重掺杂P区的结构示意图。FIG. 7 shows a schematic structural diagram for forming a heavily doped P region.
图8显示为体硅的超结器件结构示意图。FIG. 8 shows a schematic diagram of a superjunction device structure of bulk silicon.
元件标号说明Component designation description
具体实施方式 Detailed ways
以下通过特定的具体实例说明本发明的实施方式,本领域技术人员可由本说明书所揭露的内容轻易地了解本发明的其他优点与功效。本发明还可以通过另外不同的具体实施方式加以实施或应用,本说明书中的各项细节也可以基于不同观点与应用,在没有背离本发明的精神下进行各种修饰或改变。Embodiments of the present invention are described below through specific examples, and those skilled in the art can easily understand other advantages and effects of the present invention from the content disclosed in this specification. The present invention can also be implemented or applied through other different specific implementation modes, and various modifications or changes can be made to the details in this specification based on different viewpoints and applications without departing from the spirit of the present invention.
请参阅图1a至图8所示。需要说明的是,本实施例中所提供的图示仅以示意方式说明本发明的基本构想,遂图式中仅显示与本发明中有关的组件而非按照实际实施时的组件数目、形状及尺寸绘制,其实际实施时各组件的型态、数量及比例可为一种随意的改变,且其组件布局型态也可能更为复杂。Please refer to Figure 1a to Figure 8. It should be noted that the diagrams provided in this embodiment are only schematically illustrating the basic idea of the present invention, and only the components related to the present invention are shown in the diagrams rather than the number, shape and shape of the components in actual implementation. Dimensional drawing, the type, quantity and proportion of each component can be changed arbitrarily during actual implementation, and the component layout type may also be more complicated.
一种SJ-IGBT器件结构的制备方法,该方法包括以下步骤:提供一衬底;在该衬底上形成漂移区并在该漂移区预设源端和漏端;提供一设有若干第一窗口的第一掩膜版,所述第一窗口的宽度沿源端到漏端方向依次增大;自上述第一窗口向所述漂移区进行N型离子注入;退火,在该漂移区形成沿源端到漏端方向N型载流子浓度呈线性增加的N型漂移区;提供一设有若干第二窗口的第二掩膜版;自该第二窗口向所述N型漂移区采用三次能量和剂量依次减小的方式进行P型离子注入,形成间隔的P柱和N柱;且P柱不和漏端相连;最后形成沟道、源区、漏区和栅区域。A method for preparing a SJ-IGBT device structure, the method comprising the following steps: providing a substrate; forming a drift region on the substrate and presetting source and drain terminals in the drift region; providing a device with a plurality of first The first mask plate of the window, the width of the first window increases sequentially along the direction from the source end to the drain end; N-type ion implantation is performed from the first window to the drift region; annealing forms an edge along the drift region An N-type drift region in which the concentration of N-type carriers increases linearly from the source end to the drain end; a second mask with a plurality of second windows is provided; three times are used from the second window to the N-type drift region P-type ion implantation is carried out in a manner of decreasing energy and dose in order to form spaced P columns and N columns; and the P columns are not connected to the drain end; finally, the channel, source region, drain region and gate region are formed.
所述退火时间为600~1000分钟。所述退火温度为1000~1400度。所述P型离子注入的剂量为N型离子注入的1.5-2.5倍,优选2倍。所述衬底为硅或SOI。所述漏区为重掺杂P。The annealing time is 600-1000 minutes. The annealing temperature is 1000-1400 degrees. The dose of the P-type ion implantation is 1.5-2.5 times, preferably 2 times, that of the N-type ion implantation. The substrate is silicon or SOI. The drain region is heavily doped with P.
请参阅图1a~图8所示,本发明提供一种SJ-IGBT器件结构的制备方法,该方法至少包括以下步骤:Please refer to Figures 1a to 8, the present invention provides a method for preparing a SJ-IGBT device structure, the method at least includes the following steps:
首先实施步骤1),提供一半导体衬底1,本实施例中,该衬底为硅或者SOI衬底。在所述半导体衬底1上形成漂移区2。First, step 1) is implemented, and a semiconductor substrate 1 is provided. In this embodiment, the substrate is a silicon or SOI substrate. A drift region 2 is formed on the semiconductor substrate 1 .
需要说明的是,在形成所述漂移区之前,还可以包括在所述半导体衬底1上形成缓冲层(未图示),以防止在阻断电压时耗尽层到达所述半导体衬底1,且所述缓冲层用于控制半导体衬底向缓冲区注入少数载流子的能力,即控制所述半导体衬底1的注入效率。It should be noted that, before forming the drift region, a buffer layer (not shown) may also be formed on the semiconductor substrate 1 to prevent the depletion layer from reaching the semiconductor substrate 1 when the voltage is blocked. , and the buffer layer is used to control the ability of the semiconductor substrate to inject minority carriers into the buffer, that is, to control the injection efficiency of the semiconductor substrate 1 .
请参阅图1a所示,在该漂移区2上预设源端和漏端(未图示)。然后提供一端自与源端相邻的位置起始的第一掩膜版3,(即该掩膜版放置于所述漂移区之上,掩膜版和该漂移区左侧平齐)。Referring to FIG. 1 a , a source terminal and a drain terminal (not shown) are preset on the drift region 2 . Then provide a first mask 3 whose end starts from a position adjacent to the source end (that is, the mask is placed on the drift region, and the mask is flush with the left side of the drift region).
该第一掩膜版上设有若干第一窗口,请参阅图1b所示,其为第一掩膜版3放置于设有漂移区2的半导体衬底1上方的俯视图。本实施例中,所述第一窗口为若干个长度l一致的矩形,该若干个第一窗口自源端到漏端的方向上宽度d逐渐增大。换句话说,第一掩膜版遮挡部的宽度自源端到漏端的方向上逐渐减小。即沿源端到漏端方向排列中,第二个窗口32的宽度比第一个窗口31的宽度大;第三个窗口33的宽度比第二个窗口32的宽度大,以此类推。换句话说,沿源端到漏端方向排列中,第一个遮挡部的宽度大于第二个遮挡部的宽度,第二个遮挡部的宽度大于第三个遮挡部的宽度,以此类推。只要所述窗口的宽度线性逐渐增大都能实现本发明。Several first windows are provided on the first mask, as shown in FIG. 1 b , which is a top view of the first mask 3 placed above the semiconductor substrate 1 provided with the drift region 2 . In this embodiment, the first windows are several rectangles with the same length l, and the width d of the several first windows gradually increases from the source terminal to the drain terminal. In other words, the width of the shielding portion of the first mask gradually decreases from the source end to the drain end. That is, in the arrangement along the direction from the source end to the drain end, the width of the second window 32 is larger than the width of the first window 31; the width of the third window 33 is larger than the width of the second window 32, and so on. In other words, in the arrangement along the direction from the source terminal to the drain terminal, the width of the first shielding portion is greater than the width of the second shielding portion, the width of the second shielding portion is greater than the width of the third shielding portion, and so on. The present invention can be implemented as long as the width of the window increases linearly.
具体的,本实施例中,第一个窗口的宽度大致为0.6um,第二个窗口的宽度大致为 0.9um,第三个窗口的宽度大致为1.8um,第四个窗口的宽度大致为2.3um,第五个窗口的宽度大致为 3.2um,第六个窗口(未图示)的宽度大致为4.5um,第七个窗口(未图示)的宽度大致为6.2um,第八个窗口(未图示)的宽度大致为9.5um,第九个窗口(未图示)的宽度大致为15.8um。 以此类推。Specifically, in this embodiment, the width of the first window is approximately 0.6um, the width of the second window is approximately 0.9um, the width of the third window is approximately 1.8um, and the width of the fourth window is approximately 2.3um. um, the width of the fifth window is approximately 3.2um, the width of the sixth window (not shown) is approximately 4.5um, the width of the seventh window (not shown) is approximately 6.2um, and the width of the eighth window ( Not shown) has a width of approximately 9.5um, and the ninth window (not shown) has a width of approximately 15.8um. And so on.
第一个遮挡部的宽度大致为14.7 um,第二个遮挡部的宽度大致为10.6um,第三个遮挡部的宽度大致为7.5um ,第四个遮挡部的宽度大致为5.2um,第五个遮挡部的宽度大致为3.1um,第六个遮挡部(未图示)的宽度大致为1.9um,第七个遮挡部(未图示)的宽度大致为1.1um,第八个遮挡部(未图示)的宽度大致为0.6um。以此类推。The width of the first shading part is about 14.7um, the width of the second shading part is about 10.6um, the width of the third shading part is about 7.5um, the width of the fourth shading part is about 5.2um, and the width of the fifth The width of the first shielding part is approximately 3.1um, the width of the sixth shielding part (not shown) is approximately 1.9um, the width of the seventh shielding part (not shown) is approximately 1.1um, and the eighth shielding part ( Not shown) has a width of approximately 0.6um. and so on.
将该第一掩膜版放置在所述漂移区2之上,掩膜版和该漂移区左侧平齐,自上述窗口向该漂移区进行N型离子注入后退火,由于自源端到漏端方向排列中,第一个窗口31到第二个窗口32之间的距离大于第三个窗口33到第二个窗口32的距离,所以退火后N型离子扩散,第一个窗口和第二个窗口之间的扩散区离子浓度小于第三个窗口和第二个窗口之间的扩散区离子浓度,以此类推,在整个漂移区形成离子浓度自源端到漏端方向上呈线性分布的N型漂移区。如图2所示。The first mask plate is placed on the drift region 2, the mask plate is flush with the left side of the drift region, and annealing is performed after N-type ion implantation from the above-mentioned window to the drift region. In the end direction arrangement, the distance between the first window 31 and the second window 32 is greater than the distance between the third window 33 and the second window 32, so after annealing, N-type ions diffuse, and the first window and the second window The ion concentration in the diffusion region between the two windows is less than the ion concentration in the diffusion region between the third window and the second window, and so on, forming a linear distribution of ion concentration in the direction from the source end to the drain end in the entire drift region. N-type drift region. as shown in picture 2.
本实施例中,进行N型离子注入后退火的时间为600~900分钟。最好是900分钟。退火温度为1000~1200度。最好是1200度。In this embodiment, the annealing time after the N-type ion implantation is 600-900 minutes. Preferably 900 minutes. The annealing temperature is 1000-1200 degrees. Preferably 1200 degrees.
接着提供一第二掩膜版(未图示),该第二掩膜版上横向均匀的设有若干窗口4,本实施例中,所述第二掩膜版上的窗口纵长方向为自源端到漏端的方向。其中所述窗口41的左侧自与源端相邻的位置即与第一掩膜版的第一个遮挡部(自源端向漏端数第一个最宽的遮挡部)左侧平齐起始,截止于所述漏端附近,但是离漏端有一定的距离。请参照图3b所示。Then provide a second mask plate (not shown), the second mask plate is uniformly provided with a number of windows 4 in the horizontal direction, in this embodiment, the longitudinal direction of the window on the second mask plate is from direction from source to drain. Wherein the left side of the window 41 is flush with the left side of the first shielding part (the first and widest shielding part counting from the source end to the drain end) of the first mask from the position adjacent to the source end It starts and ends near the drain end, but there is a certain distance from the drain end. Please refer to Figure 3b.
自所述第二掩膜版的窗口采用三次能量和剂量依次减小的方式进行P型离子注入,请参照图3a所示。具体的,第一次P型离子注入的能量为3E12-5E12,优选的是4E12,剂量为300-500kev,优选的是400 kev;第二次P型离子注入的能量为2E12-4E12,优选的是3E12;剂量为200-300kev,优选的为250kev;第三次P型离子注入的能量为0.5E12-2 E12,优选的是1E12 ,剂量为50-100kev,优选的是80kev。The P-type ion implantation is performed from the window of the second mask using three times of sequentially decreasing energy and dose, as shown in FIG. 3 a . Specifically, the energy of the first P-type ion implantation is 3E12-5E12, preferably 4E12, and the dose is 300-500kev, preferably 400kev; the energy of the second P-type ion implantation is 2E12-4E12, preferably It is 3E12; the dose is 200-300kev, preferably 250kev; the energy of the third P-type ion implantation is 0.5E12-2 E12, preferably 1E12, and the dose is 50-100kev, preferably 80kev.
该P型离子三次注入的剂量总和为该N型离子注入剂量的1.5-2.5倍,最好是2倍的剂量。这样就形成了P柱N柱、P柱N柱间隔的出现的区域。所述第二掩膜版上的窗口不贯通漂移区,即该第二掩膜版的窗口离漏端有一定的距离,从而使得P柱不和漏端相连。由于P型柱区离漏端有一定的距离,因此降低了电荷不平衡对器件性能的影响,提高器件可靠性。The sum of the three implanted doses of the P-type ions is 1.5-2.5 times, preferably twice, the dose of the N-type ion implanted. In this way, the area where the P-pillar, N-column, and P-pillar-N-column intervals appear is formed. The window on the second mask plate does not penetrate the drift region, that is, the window of the second mask plate has a certain distance from the drain end, so that the P column is not connected to the drain end. Since there is a certain distance between the P-type column region and the drain end, the influence of the charge imbalance on the performance of the device is reduced, and the reliability of the device is improved.
接下来经过一个10-30分钟(最好是20分钟左右)的高温退火,形成超结的漂移区。高温退火形成超结的漂移区属于本领域的公知常识,在此不再赘述。Next, after a high temperature annealing for 10-30 minutes (preferably about 20 minutes), the drift region of the super junction is formed. The formation of the drift region of the superjunction by high temperature annealing belongs to the common knowledge in the field, and will not be repeated here.
接着请参照图4所示,制备P阱。本实施例中的衬底选择为SOI衬底,其包括底硅11、位于低位上的埋层氧化层12,以及位于埋层氧化层12上的顶层硅,用于作为漂移区。在预设的源端进行P离子注入,形成P阱。Next, please refer to FIG. 4 to prepare a P well. The substrate in this embodiment is selected to be an SOI substrate, which includes bottom silicon 11 , buried oxide layer 12 on the lower position, and top silicon on the buried oxide layer 12 for use as a drift region. Perform P ion implantation at the preset source to form a P well.
然后在P阱、P柱和N柱近源端的上方制备栅区域,该栅区域包括栅介质层51以及位于栅介质层51上的栅极52。本实施例中栅介质层的材质为二氧化硅、氮化硅等本领域常用材质。请参照图5所示。Then prepare a gate area above the P well, P column and N column near the source end, the gate area includes a gate dielectric layer 51 and a gate 52 on the gate dielectric layer 51 . In this embodiment, the material of the gate dielectric layer is silicon dioxide, silicon nitride and other commonly used materials in the field. Please refer to Figure 5.
接着在源端靠近栅区域的位置进行重掺杂N型注入,形成N+区域。请参照图6所示。Next, a heavily doped N-type implant is performed at a position close to the gate region at the source end to form an N + region. Please refer to Figure 6.
最后,请参照图7所示,在P阱上、N+区域的一侧(远离栅区域的一侧)以及漏端进行重掺杂P型离子注入,各自分别形成P+区域。形成沟道、源区、漏区。所述漏区为重掺杂P。该部分属于本领域的公知常识,在此不再赘述。Finally, please refer to FIG. 7, perform heavily doped P-type ion implantation on the P well, the side of the N + region (the side away from the gate region), and the drain end to form a P + region respectively. Channel, source and drain regions are formed. The drain region is heavily doped with P. This part belongs to the common knowledge in this field, and will not be repeated here.
由于传统的超结器件漂移区中交替存在的P和N柱区,为了提高耐压,要求N柱区和P柱区达到电荷平衡,在器件反向耐压时漂移区实现全耗尽,但是由于存在衬底辅助耗尽效应,引起P型柱区出现剩余电荷,本发明采用线性漂移区的N柱取代传统的均匀分布的N型漂移区,N型柱区的浓度从源到漏线性增加,消除了衬底辅助耗尽效应,使器件达到电荷平衡,提高器件耐压,此结构也可应用于体硅技术。如图8所示。Due to the alternate existence of P and N column regions in the drift region of traditional superjunction devices, in order to improve the withstand voltage, the N column region and the P column region are required to achieve charge balance, and the drift region is fully depleted when the device reverses the withstand voltage, but Due to the existence of the substrate-assisted depletion effect, residual charges appear in the P-type column region. The present invention uses the N-type column in the linear drift region to replace the traditional uniformly distributed N-type drift region, and the concentration of the N-type column region increases linearly from the source to the drain. , eliminates the substrate-assisted depletion effect, enables the device to achieve charge balance, and improves the withstand voltage of the device. This structure can also be applied to bulk silicon technology. As shown in Figure 8.
本发明通过采用掩膜版的窗口从源端到漏端方向上宽度依次增加,遮挡部分宽度依次减小,对整个漂移区进行用于形成线性N柱区的离子注入,调节离子注入能量和剂量,然后进行一个长时间的高温退火,使N柱区形成一个线性漂移区。线性漂移区形成以后,再通过P型掩膜版分三次进行P型离子注入,P型离子注入的计量接近于N柱区的2倍,然后经过一个短暂的20分钟高温退火后形成超结的漂移区,然后再进行常规的沟道,源区,漏区,栅极的制作。In the present invention, the width of the window of the mask plate increases sequentially from the source end to the drain end, and the width of the shielding part decreases sequentially, and ion implantation is performed on the entire drift area to form a linear N-column area, and the ion implantation energy and dose are adjusted. , and then perform a long-time high-temperature annealing to make the N-column region form a linear drift region. After the linear drift region is formed, P-type ion implantation is performed three times through the P-type mask. The metering of P-type ion implantation is close to twice that of the N-column region, and then a short 20-minute high-temperature annealing is performed to form a superjunction The drift region, and then the conventional channel, source region, drain region, and gate are fabricated.
横向SOI超结器件由于存在衬底辅助耗尽效应,导致从器件源端到漏端,P型柱区的剩余电荷逐渐增加,P型剩余电荷的存在,降低了器件耐压。根据现有的研究结果,P型区的剩余电荷从源到漏近似线性分布,因此,本发明中横向SOI超结功率器件的N型区采用线性分布,使N柱区的浓度从源到漏逐渐增加,消除漂移区剩余电荷,而P型柱区不和漏极相连。同时,通过将传统超结器件的漏极N+区换成P+区,将IGBT的引入到超结器件设计中,器件工作在开态时,P+区向漂移区注入空穴,增加漂移区电流能力,可以更好的降低器件开态电阻。由于P型柱区离漏极有一定的距离,因此降低了电荷不平衡对器件性能的影响,提高器件可靠性。同时,通过将漏极N+区换成P+区,器件工作时,重掺杂P区向漂移区注入空穴,增加漂移区电流能力,更好的降低器件开态电阻。Due to the substrate-assisted depletion effect of lateral SOI superjunction devices, the residual charge in the P-type column region gradually increases from the source end to the drain end of the device. The existence of P-type residual charge reduces the withstand voltage of the device. According to the existing research results, the residual charge in the P-type region is approximately linearly distributed from source to drain. Therefore, the N-type region of the lateral SOI superjunction power device in the present invention adopts a linear distribution, so that the concentration of the N column region is from source to drain. Gradually increase to eliminate the residual charge in the drift region, while the P-type column region is not connected to the drain. At the same time, by replacing the drain N+ region of the traditional super-junction device with a P+ region, the IGBT is introduced into the design of the super-junction device. When the device is in the on state, the P+ region injects holes into the drift region to increase the current capability of the drift region. , can better reduce the on-state resistance of the device. Since there is a certain distance between the P-type column region and the drain, the influence of the charge imbalance on the device performance is reduced, and the reliability of the device is improved. At the same time, by replacing the drain N+ region with a P+ region, when the device is working, the heavily doped P region injects holes into the drift region, increasing the current capability of the drift region, and better reducing the on-state resistance of the device.
综上所述,本发明有效克服了现有技术中的种种缺点而具高度产业利用价值。To sum up, the present invention effectively overcomes various shortcomings in the prior art and has high industrial application value.
上述实施例仅例示性说明本发明的原理及其功效,而非用于限制本发明。任何熟悉此技术的人士皆可在不违背本发明的精神及范畴下,对上述实施例进行修饰或改变。因此,举凡所属技术领域中具有通常知识者在未脱离本发明所揭示的精神与技术思想下所完成的一切等效修饰或改变,仍应由本发明的权利要求所涵盖。The above-mentioned embodiments only illustrate the principles and effects of the present invention, but are not intended to limit the present invention. Anyone skilled in the art can modify or change the above-mentioned embodiments without departing from the spirit and scope of the present invention. Therefore, all equivalent modifications or changes made by those skilled in the art without departing from the spirit and technical ideas disclosed in the present invention should still be covered by the claims of the present invention.
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