CN111933693A - MOS transistor and method for manufacturing the same - Google Patents
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Abstract
本发明提供了一种MOS晶体管及其制造方法,在第一导电类型的源/漏区中形成了第二导电类型的反型掺杂区,所述源/漏区横向扩散至与栅极发生交叠,所述反型掺杂区横向扩散的边界不超过所述栅极的侧壁,纵向扩散的底部边界和所述源/漏区的底部边界具有第一垂直距离,所述反型掺杂区纵向扩散的顶部边界与所述源/漏区的顶部边界有第二垂直距离,能够降低晶体管的漏电流并提高其击穿电压。本发明的MOS晶体管的制造方法,工艺简单,成本低。
The present invention provides a MOS transistor and a method for fabricating the same, in which an inversion doped region of a second conductivity type is formed in a source/drain region of a first conductivity type, the source/drain region is laterally diffused to the point of contact with a gate electrode overlapping, the boundary of the lateral diffusion of the inversion doping region does not exceed the sidewall of the gate, the bottom boundary of the longitudinal diffusion and the bottom boundary of the source/drain region have a first vertical distance, the inversion doping region The top boundary of the vertical diffusion of the impurity region has a second vertical distance from the top boundary of the source/drain region, which can reduce the leakage current and increase the breakdown voltage of the transistor. The manufacturing method of the MOS transistor of the present invention has the advantages of simple process and low cost.
Description
技术领域technical field
本发明涉及半导体器件的制作技术领域,特别涉及一种MOS晶体管及其制造方法。The invention relates to the technical field of fabrication of semiconductor devices, in particular to a MOS transistor and a fabrication method thereof.
背景技术Background technique
目前,金属氧化物半导体(Metal Oxide Semiconductor, MOS) 场效应晶体管可分为NMOS晶体管与PMOS晶体管两大类。图1示为本领域中已知的一种 MOS(Metal OxideSemiconductor,金属氧化物半导体)晶体管的结构示意图,其衬底100中形成有源/漏区101,衬底100表面上形成有栅氧层102、栅极103。At present, Metal Oxide Semiconductor (MOS) field effect transistors can be divided into two categories: NMOS transistors and PMOS transistors. FIG. 1 is a schematic structural diagram of a MOS (Metal Oxide Semiconductor) transistor known in the art, an active/
在高电压下,要求输入输出电路或大功率集成电路具有高击穿电压的MOS晶体管。为了使得图1中所示的MOS晶体管能够应用于高压环境且能够在高压下安全运行,现有技术中通常采用两种常用的方法,一种是牺牲MOS晶体管的电性能或器件面积;另一种方法是,采用电荷平衡法的RESURF技术或对器件结构进行改进,由此在不牺牲器件电性能的前提下提高击穿电压。At high voltages, input-output circuits or high-power integrated circuits are required to have MOS transistors with high breakdown voltages. In order to enable the MOS transistor shown in FIG. 1 to be applied in a high-voltage environment and to operate safely under high-voltage, two common methods are usually adopted in the prior art, one is sacrificing the electrical performance or device area of the MOS transistor; the other One way is to use the charge balance method of RESURF technology or to improve the device structure, thereby increasing the breakdown voltage without sacrificing the electrical performance of the device.
因此,如何进一步提高MOS晶体管的电性能,成为本领域技术人员研究的热点问题之一。Therefore, how to further improve the electrical performance of the MOS transistor has become one of the hot issues studied by those skilled in the art.
发明内容SUMMARY OF THE INVENTION
本发明的一目的在于提供一种MOS晶体管,能够进一步改善MOS晶体管的电学特性。An object of the present invention is to provide a MOS transistor, which can further improve the electrical characteristics of the MOS transistor.
本发明的另一目的在于提供一种MOS晶体管的制造方法,能够通过相对简单的工艺获得具有较佳电学特性的MOS晶体管。Another object of the present invention is to provide a method for manufacturing a MOS transistor, which can obtain a MOS transistor with better electrical characteristics through a relatively simple process.
为解决上述技术问题,本发明提供一种MOS晶体管,包括衬底以及形成在所述衬底上的栅极,所述栅极两侧的衬底中形成有源/漏区,所述源/漏区横向扩散至与所述栅极发生交叠;其中,所述MOS晶体管还包括:第二导电类型的反型掺杂区,所述反型掺杂区形成在所述栅极两侧的源/漏区中,所述反型掺杂区横向扩散的边界不超过所述栅极的侧壁,所述反型掺杂区纵向扩散的底部边界和所述源/漏区的底部边界相距第一垂直距离,所述反型掺杂区纵向扩散的顶部边界与所述源/漏区的顶部边界相距第二垂直距离,所述第一垂直距离和所述第二垂直距离均大于0。In order to solve the above technical problems, the present invention provides a MOS transistor, which includes a substrate and a gate formed on the substrate, and active/drain regions are formed in the substrate on both sides of the gate, and the source/drain is formed in the substrate on both sides of the gate. The drain region is laterally diffused to overlap with the gate; wherein, the MOS transistor further includes: an inversion doping region of the second conductivity type, the inversion doping region is formed on both sides of the gate In the source/drain region, the boundary of the lateral diffusion of the inversion doping region does not exceed the sidewall of the gate, and the bottom boundary of the longitudinal diffusion of the inversion doping region is separated from the bottom boundary of the source/drain region For a first vertical distance, the top boundary of the longitudinal diffusion of the inversion doping region is separated from the top boundary of the source/drain region by a second vertical distance, and both the first vertical distance and the second vertical distance are greater than 0.
可选地,所述源/漏区包括第一导电类型的重掺杂区以及第一导电类型的延伸扩展区,所述延伸扩展区包围所述重掺杂区且顶部边界与所述重掺杂区的顶部边界齐平,所述重掺杂区面向所述栅极的边界与所述栅极的侧壁之间的横向距离大于0,所述延伸扩展区从所述重掺杂区的边界延伸到所述栅极的底部下方,并与所述栅极发生交叠,所述延伸扩展区的第一导电类型离子掺杂浓度低于所述重掺杂区的第一导电类型离子掺杂浓度。Optionally, the source/drain region includes a heavily doped region of a first conductivity type and an extension region of the first conductivity type, the extension region surrounding the heavily doped region and having a top border with the heavily doped region The top boundary of the impurity region is flush, the lateral distance between the boundary of the heavily doped region facing the gate and the sidewall of the gate is greater than 0, and the extension region extends from the edge of the heavily doped region. The boundary extends below the bottom of the gate and overlaps the gate, and the first conductive type ion doping concentration of the extension extension region is lower than that of the heavily doped region. impurity concentration.
可选地,所述反型掺杂区形成在所述延伸扩展区中。Optionally, the inversion doped region is formed in the extension region.
可选地,所述反型掺杂区的第二导电类型离子掺杂浓度高于所述重掺杂区的第一导电类型离子掺杂浓度。Optionally, the doping concentration of the second conductivity type ions of the inversion doped region is higher than the doping concentration of the first conductivity type ions of the heavily doped region.
可选地,所述第一垂直距离大于等于所述第二垂直距离。Optionally, the first vertical distance is greater than or equal to the second vertical distance.
可选地,所述的MOS晶体管还包括位于所述栅极侧壁上的侧墙以及位于所述栅极和所述衬底之间的栅氧化层;所述反型掺杂区形成于所述侧墙底部的源/漏区中。Optionally, the MOS transistor further includes a spacer on the sidewall of the gate and a gate oxide layer between the gate and the substrate; the inversion doped region is formed on the gate. in the source/drain regions at the bottom of the spacers.
基于同一发明构思,本发明还提供一种如本发明所述的MOS晶体管的制造方法,包括以下步骤:Based on the same inventive concept, the present invention also provides a method for manufacturing a MOS transistor according to the present invention, comprising the following steps:
提供一衬底,在所述衬底上形成栅极;providing a substrate on which a gate is formed;
采用第一导电类型的掺杂杂质对所述栅极两侧的衬底进行源漏离子注入,以在所述栅极两侧的衬底中形成源漏注入区;Perform source-drain ion implantation on the substrates on both sides of the gate using doping impurities of the first conductivity type, so as to form source-drain implantation regions in the substrates on both sides of the gate;
采用第二导电类型的掺杂杂质对所述源漏掺杂区进行反型离子注入,以在所述源漏掺杂区中形成反型注入区;Perform inversion ion implantation on the source and drain doped regions by using doping impurities of the second conductivity type to form inversion implantation regions in the source and drain doped regions;
对所述衬底进行退火处理,以形成源/漏区和反型掺杂区,所述源/漏区横向扩散至与所述栅极发生交叠,所述反型掺杂区横向扩散的边界不超过所述栅极的侧壁,所述反型掺杂区纵向扩散的底部边界和所述源/漏区的底部边界具有第一距离,所述反型掺杂区纵向扩散的顶部边界与所述源/漏区的顶部边界有第二距离,所述第一距离和所述第二距离均大于0。The substrate is annealed to form source/drain regions and inversion doped regions, the source/drain regions are laterally diffused to overlap the gate, and the inversion doped regions are laterally diffused The boundary does not exceed the sidewall of the gate, the bottom boundary of the longitudinal diffusion of the inversion doped region and the bottom boundary of the source/drain region have a first distance, and the top boundary of the longitudinal diffusion of the inversion doped region has a first distance There is a second distance from the top boundary of the source/drain region, and both the first distance and the second distance are greater than zero.
可选地,采用第一倾斜角度对所述栅极两侧的衬底进行源漏离子注入,采用第二倾斜角度对所述源漏掺杂区进行反型离子注入,所述第一倾斜角度和第二倾斜角度均为离子注入方向与所述衬底表面上的法线之间的夹角,且所述第一倾斜角度大于第二倾斜角度。Optionally, source-drain ion implantation is performed on the substrate on both sides of the gate using a first inclination angle, and inversion ion implantation is performed on the source-drain doped region using a second inclination angle, the first inclination angle is and the second inclination angle are both the included angle between the ion implantation direction and the normal on the surface of the substrate, and the first inclination angle is greater than the second inclination angle.
可选地,在退火处理后,所述源/漏区包括第一导电类型的重掺杂区以及第一导电类型的延伸扩展区,所述延伸扩展区包围所述重掺杂区且顶部边界与所述重掺杂区的顶部边界齐平,所述重掺杂区面向所述栅极的边界与所述栅极的侧壁之间的横向距离大于0,所述延伸扩展区从所述重掺杂区的边界延伸到所述栅极的底部下方,并与所述栅极发生交叠,所述延伸扩展区的第一导电类型离子掺杂浓度低于所述重掺杂区的第一导电类型离子掺杂浓度。Optionally, after the annealing process, the source/drain region includes a heavily doped region of the first conductivity type and an extension region of the first conductivity type, the extension region surrounding the heavily doped region and having a top border flush with the top boundary of the heavily doped region, the lateral distance between the boundary of the heavily doped region facing the gate and the sidewall of the gate is greater than 0, the extension region extends from the The boundary of the heavily doped region extends below the bottom of the gate and overlaps with the gate, and the first conductivity type ion doping concentration of the extended extension region is lower than that of the heavily doped region. A conductivity type ion doping concentration.
可选地,在形成所述栅极之后且在进行源漏离子注入之前或之后,还在所述栅极的侧壁上形成侧墙。Optionally, after the gate is formed and before or after the source-drain ion implantation, spacers are also formed on the sidewalls of the gate.
与现有技术相比,本发明的技术方案至少具有以下有益效果:Compared with the prior art, the technical solution of the present invention has at least the following beneficial effects:
1、本发明的MOS 晶体管结构,在第一导电类型的源/漏区中形成了第二导电类型的反型掺杂区,所述源/漏区横向扩散至与栅极发生交叠,所述反型掺杂区横向扩散的边界不超过所述栅极的侧壁,纵向扩散的底部边界和所述源/漏区的底部边界具有第一垂直距离,所述反型掺杂区纵向扩散的顶部边界与所述源/漏区的顶部边界有第二垂直距离,能够降低晶体管的漏电流并提高其击穿电压。1. In the MOS transistor structure of the present invention, inversion doped regions of the second conductivity type are formed in the source/drain regions of the first conductivity type, and the source/drain regions are laterally diffused to overlap with the gate, so The boundary of the lateral diffusion of the inversion doping region does not exceed the sidewall of the gate, the bottom boundary of the longitudinal diffusion and the bottom boundary of the source/drain region have a first vertical distance, and the inversion doping region is longitudinally diffused The top boundary of the source/drain region has a second vertical distance from the top boundary of the source/drain region, which can reduce the leakage current of the transistor and increase its breakdown voltage.
2、本发明的MOS 晶体管的制造方法,通过高能量离子注入工程,可以在源/漏区中形成用于改善器件电学特性的反型掺杂区,工艺简单,成本低。2. In the manufacturing method of the MOS transistor of the present invention, through high-energy ion implantation, an inversion doped region for improving the electrical characteristics of the device can be formed in the source/drain region, the process is simple, and the cost is low.
附图说明Description of drawings
图1是现有的一种MOS晶体管的剖面结构示意图。FIG. 1 is a schematic cross-sectional structure diagram of a conventional MOS transistor.
图2是本发明一实施例的MOS晶体管的剖面结构示意图。FIG. 2 is a schematic cross-sectional structure diagram of a MOS transistor according to an embodiment of the present invention.
图3是图1和图2所示的MOS晶体管的BVDss(源漏击穿电压)-Idsat(饱和源漏电流)特性曲线。FIG. 3 is a BVDss (source-drain breakdown voltage)-Idsat (saturated source-drain current) characteristic curve of the MOS transistor shown in FIGS. 1 and 2 .
图4是图1和图2所示的MOS晶体管的Ioff(漏电流)-Idsat(饱和源漏电流)特性曲线。FIG. 4 is an Ioff (drain current)-Idsat (saturated source-drain current) characteristic curve of the MOS transistor shown in FIGS. 1 and 2 .
图5是本发明具体实施例的MOS晶体管的制造方法流程图。FIG. 5 is a flowchart of a method for manufacturing a MOS transistor according to a specific embodiment of the present invention.
图6至图9是本发明具体实施例的MOS晶体管的制造方法中的器件剖面结构示意图。FIG. 6 to FIG. 9 are schematic cross-sectional structural diagrams of a device in a method for manufacturing a MOS transistor according to an embodiment of the present invention.
其中,附图标记如下:Among them, the reference numerals are as follows:
100-衬底,101-源/漏区,102-栅氧层,103-栅极;100-substrate, 101-source/drain region, 102-gate oxide layer, 103-gate;
200-衬底,201-栅氧层,202-栅极,203-侧墙,204-源/漏区,204a-重掺杂区,204b-延伸扩展区,205-反型掺杂区,204’-源漏注入区,205’ -反型注入区;200-substrate, 201-gate oxide, 202-gate, 203-spacer, 204-source/drain region, 204a-heavy doped region, 204b-extension region, 205-inversion doped region, 204 '-source-drain implantation region, 205'-inversion implantation region;
D1-第一垂直距离,D2-第二垂直距离,D3-横向距离。D1-first vertical distance, D2-second vertical distance, D3-lateral distance.
具体实施方式Detailed ways
以下结合附图2至附图9和具体实施例对本发明提出的技术方案作进一步详细说明。根据下面说明,本发明的优点和特征将更清楚。需说明的是,附图均采用非常简化的形式且均使用非精准的比例,仅用以方便、明晰地辅助说明本发明实施例的目的。The technical solution proposed by the present invention will be further described in detail below with reference to Fig. 2 to Fig. 9 and specific embodiments. The advantages and features of the present invention will become more apparent from the following description. It should be noted that, the accompanying drawings are all in a very simplified form and in inaccurate scales, and are only used to facilitate and clearly assist the purpose of explaining the embodiments of the present invention.
请参考图2,本发明一实施例提供一种MOS晶体管,包括衬底200、栅氧层201、栅极202、侧墙203、源/漏区204以及反型掺杂区205。Referring to FIG. 2 , an embodiment of the present invention provides a MOS transistor including a
其中,衬底200可以是本领域技术人员所熟知的任意合适的衬底材料,例如体硅衬底或者绝缘体上硅衬底等,本实施例在此不对其进行限制。The
栅氧层201和栅极202依次堆叠在衬底200的表面上,形成栅极堆叠结构,且侧墙203形成在栅极堆叠结构的侧壁上。栅氧层201的材质可以是二氧化硅,栅极202的材料可以是掺杂多晶硅等。The
栅极堆叠结构两侧的衬底200中形成有第一导电类型(例如为N型)的源/漏区204,且栅极202一侧的所述源/漏区204作为MOS晶体管的源区,另一侧的所述源/漏区204作为所述MOS晶体管的漏区。栅极202两侧的所述源/漏区204均横向扩散至与所述栅极203发生部分交叠。栅极202两侧的源/漏区204向着栅极203方向延伸的程度越大(即源/漏区204与栅极203交叠的区域越大),同样的栅极电压Vgate下,MOS晶体管的漏端电流Idrain越大,且同样的漏极电压Vdrain下,MOS晶体管的漏端电流Idrain越大。Source/
反型掺杂区205为第二导电类型(例如P型),其导电类型与源/漏区204相反。所述反型掺杂区205形成在所述栅极202两侧的源/漏区204中,所述栅极202两侧的所述反型掺杂区205横向扩散的边界均不超过所述栅极202的侧壁,作为一种示例,所述反型掺杂区205向着栅极202方向横向扩散的边界与栅极202的侧壁之间具有横向距离D3,且D3大于0。The inversion-doped
在向着衬底200底部扩散的方向上,所述反型掺杂区205纵向扩散的底部边界和所述源/漏区204的底部边界相距第一垂直距离D1,在向着衬底200的顶部扩散的方向上,所述反型掺杂区205纵向扩散的顶部边界与所述源/漏区204的顶部边界相距第二垂直距离D2,所述第一垂直距离D1和所述第二垂直距离D2均大于0。可选地,所述第一垂直距离D1大于等于所述第二垂直距离D2,有利于形成更浅的结,提高器件电学特性。In the direction of diffusion toward the bottom of the
此外,所述反型掺杂区205在所述源/漏区204中的区域占比越大,同样的栅极电压Vgate下,MOS晶体管的漏端电流Idrain越大,且同样的漏极电压Vdrain下,MOS晶体管的漏端电流Idrain越大。因此,最佳的是,控制反型掺杂区205在源/漏区204中为工艺所允许的最小反型掺杂区域。In addition, the larger the proportion of the inversion doped
可选地,所述源/漏区204包括第一导电类型的重掺杂区204a以及第一导电类型的延伸扩展区204b,所述延伸扩展区204b包围所述重掺杂区204a的侧壁和底壁,且所述延伸扩展区204b的顶部边界与所述重掺杂区204a的顶部边界齐平,并共同构成源/漏区204的顶部边界。所述重掺杂区204a面向所述栅极202的边界与所述栅极202的侧壁之间相距大于0的横向距离D4,所述延伸扩展区204b从所述重掺杂区204a的边界延伸到所述栅极202的底部下方,并与所述栅极202发生交叠,所述延伸扩展区204b的第一导电类型离子掺杂浓度低于所述重掺杂区204a的第一导电类型离子掺杂浓度。所述反型掺杂区205形成在侧墙203底部的所述延伸扩展区204b中,因此D3小于D4。Optionally, the source/
可选地,所述反型掺杂区205的第二导电类型离子掺杂浓度高于所述重掺杂区204a的第一导电类型离子掺杂浓度。Optionally, the ion doping concentration of the second conductivity type of the inversion doped
作为一种示例,MOS晶体管为PMOS晶体管,衬底200为P型半导体衬底,源/漏区204为N型掺杂区,反型掺杂区205为P型掺杂区,反型掺杂区205中的P离子掺杂浓度大于栅极202底部的沟道区(即衬底)中的P离子掺杂浓度,也大于源/漏区204的重掺杂区204a中的N型离子的掺杂浓度。例如,栅极202底部的沟道区(即衬底)中的P离子掺杂浓度的数量级为1012/cm2,源/漏区204的离子掺杂浓度的数量级均为1013~1014/cm2,反型掺杂区205的离子掺杂浓度的数量级不低于1015/cm2。As an example, the MOS transistor is a PMOS transistor, the
可选地,栅极202两侧的源/漏区204对称分布,栅极202两侧的反型掺杂区205也对称分布。Optionally, the source/
由于反型掺杂区205的存在,因此可以利用杂质补偿效应在源/漏区204中形成耗尽区,增大了耗尽区的宽度,并减小了晶体管的源/漏结电容,改善了源/漏区204中的电场分布,减小了源/漏结漏电流,提高了源漏击穿电压,进而改善了MOS晶体管的电学特性。 此外,由于反型掺杂区205的上、下边界(即顶部边界和底部边界)以及面向沟道的边界均与源/漏区204的相应边界有距离,因此,可以避免反型掺杂区205的加入对沟道带来不利影响。Due to the existence of the inversion doped
为了验证本实施例的MOS晶体管的性能,将图1至图2所示的MOS晶体管进行了性能测试,这两种MOS晶体管中,图2所示的MOS晶体管相对图1所示的MOS晶体管,仅仅在源/漏区204中增加了反型掺杂区205。测试结果如图3和图4所示,图3和图4中,“现有技术”表示的是图1所示的MOS晶体管的测试结果, “本发明”表示的是图2所示的MOS晶体管的测试结果。In order to verify the performance of the MOS transistor in this embodiment, the performance test of the MOS transistor shown in FIG. 1 to FIG. 2 is carried out. Among the two MOS transistors, the MOS transistor shown in FIG. Only inversion doped
从图3中可以看出,具有相同的饱和源漏电流Idsat的情况下,本发明的MOS晶体管具有更高的击穿电压BVDss,即相比现有技术,本发明的MOS晶体管具有更好的BVDss-Idsat特性,这说明,本发明中添加的反型掺杂区205能够改善MOS晶体管的BVDss-Idsat特性,提高器件的击穿电压。It can be seen from FIG. 3 that under the condition of the same saturated source-drain current Idsat, the MOS transistor of the present invention has a higher breakdown voltage BVDss, that is, compared with the prior art, the MOS transistor of the present invention has better The BVDss-Idsat characteristic shows that the
从图4中可以看出,具有相同的饱和源漏电流Idsat的情况下,本发明的MOS晶体管相比现有技术具有更低的漏电流Ioff,即相比现有技术,本发明的MOS晶体管具有更好的Ioff-Idsat特性,能够降低器件漏电流。It can be seen from FIG. 4 that under the condition of the same saturated source-drain current Idsat, the MOS transistor of the present invention has a lower leakage current Ioff than the prior art, that is, the MOS transistor of the present invention has a lower leakage current Ioff than the prior art. It has better Ioff-Idsat characteristics and can reduce device leakage current.
综合上述测试结果可知,本实施例的MOS 晶体管结构,在第一导电类型的源/漏区中形成第二导电类型的反型掺杂区,能够在不增大MOS晶体管占用面积、不牺牲导通电流以及不影响器件其他电气性能的情况下,显著提高MOS晶体管的BVDss-Idsat电学特性以及Ioff-Idsat电学特性。Based on the above test results, it can be seen that in the MOS transistor structure of this embodiment, inversion doped regions of the second conductivity type are formed in the source/drain regions of the first conductivity type, which can reduce the occupied area of the MOS transistor without sacrificing conduction. The BVDss-Idsat electrical characteristics and the Ioff-Idsat electrical characteristics of the MOS transistor are significantly improved under the condition of passing current and without affecting other electrical properties of the device.
需要说明的是,上述实施例中仅仅列出了本发明MOS晶体管的部分结构,本发明的技术方案并不仅仅限定于此,在本发明的其他实施例中,所述MOS晶体管还可以具有其他结构,例如浅沟槽隔离结构等。It should be noted that the above embodiments only list part of the structure of the MOS transistor of the present invention, and the technical solution of the present invention is not limited to this. In other embodiments of the present invention, the MOS transistor may also have other structures, such as shallow trench isolation structures, etc.
请参考图5,本发明一实施例还提供一种上述的MOS晶体管的制造方法,包括以下步骤:Please refer to FIG. 5 , an embodiment of the present invention further provides a method for manufacturing the above-mentioned MOS transistor, including the following steps:
S1,提供一衬底,在所述衬底上形成栅极;S1, providing a substrate, and forming a gate on the substrate;
S2,采用第一导电类型的掺杂杂质对所述栅极两侧的衬底进行源漏离子注入,以在所述栅极两侧的衬底中形成源漏注入区;S2, using doping impurities of the first conductivity type to perform source-drain ion implantation on the substrates on both sides of the gate to form source-drain implantation regions in the substrates on both sides of the gate;
S3,采用第二导电类型的掺杂杂质对所述源漏掺杂区进行反型离子注入,以在所述源漏掺杂区中形成反型注入区;S3, performing inversion ion implantation on the source and drain doped regions by using doping impurities of the second conductivity type to form inversion implantation regions in the source and drain doped regions;
S4,对所述衬底进行退火处理,以形成源/漏区和反型掺杂区,所述源/漏区横向扩散至与所述栅极发生交叠,所述反型掺杂区横向扩散的边界不超过所述栅极的侧壁,所述反型掺杂区纵向扩散的底部边界和所述源/漏区的底部边界具有第一距离,所述反型掺杂区纵向扩散的顶部边界与所述源/漏区的顶部边界有第二距离,所述第一距离和所述第二距离均大于0。S4, annealing the substrate to form source/drain regions and inversion doping regions, the source/drain regions are laterally diffused to overlap the gate, and the inversion doping regions are laterally diffused The boundary of the diffusion does not exceed the sidewall of the gate, the bottom boundary of the longitudinal diffusion of the inversion doping region and the bottom boundary of the source/drain region have a first distance, and the longitudinal diffusion of the inversion doping region has a first distance. The top boundary has a second distance from the top boundary of the source/drain regions, and both the first distance and the second distance are greater than zero.
在步骤S1中,首先,请参考图6,提供一衬底200,所述衬底200可以是本领域技术人员所熟知的任意合适的衬底材料,例如体硅衬底、绝缘体上硅衬底、硅锗衬底等等;然后通过热氧化或者化学气相沉积工艺,在衬底200上形成栅氧层201,并进一步通过多晶硅沉积、光刻和刻蚀等一系列工艺,去除多余的多晶硅以及栅氧层201,以在所述衬底200上形成栅极202,栅极202及其下方的栅氧层201堆叠形成栅极堆叠结构。In step S1, first, referring to FIG. 6, a
可选地,在形成栅极202之后,通过绝缘介质材料沉积和侧墙刻蚀,来形成侧墙203,侧墙203覆盖在栅极202及栅极202下方的栅氧层201的侧壁上,侧墙203的材料可以是氧化硅或氮化硅等单层结构,或者为氧化硅和氮化硅等多个膜层堆叠而成的复合结构。Optionally, after the
请参考图7,在步骤S2中,以栅极堆叠结构和侧墙203为掩膜,采用第一倾斜角度A、第一注入能量和单位面积内的第一注入剂量,向栅极203两侧的衬底200中注入第一导电类型离子,例如磷离子、砷离子或锑离子等N型离子,由此一部分第一导电类型离子能被注入到栅极202底部下方的衬底200中,一部分第一导电类型离子能被注入到栅极202外侧的衬底200中,以形成与栅极202部分交叠的源漏注入区204’。Referring to FIG. 7 , in step S2 , the gate stack structure and the
请参考图8,在步骤S3中,以栅极堆叠结构和侧墙203为掩膜,采用第二倾斜角度B、第二注入能量和单位面积内的第二注入剂量,向所述源漏注入区204’中注入第二导电类型离子,例如硼离子、二氟化硼离子等P型离子,以形成反型注入区205’。Please refer to FIG. 8 , in step S3 , the gate stack structure and the
其中,请结合图7和图8,所述第一倾斜角度A和第二倾斜角度B均为离子注入方向与所述衬底200表面上的法线之间的夹角,且所述第一倾斜角度A大于第二倾斜角度B,第二倾斜角度B可以为0~30°,由此使得反型注入区205’在横向上的注入深度比源漏注入区204’浅,反型注入区205’不与栅极202交叠,进一步地,反型注入区205’可以位于侧墙203的底部;第二注入能量小于第一注入能量,由此使得反型注入区205’在纵向上的注入深度比源漏注入区204’的注入深度浅;单位面积内的第二注入剂量大于单位面积内的第一注入剂量,由此使得反型注入区205’不仅能够中和掉源漏注入区204’在此区域中的第一导电类型离子,还能形成要求掺杂浓度的第二导电类型离子掺杂区。Wherein, please refer to FIG. 7 and FIG. 8 , the first inclination angle A and the second inclination angle B are both the angle between the ion implantation direction and the normal on the surface of the
此外,本实施例中,侧墙203可以起到限定反型注入区205’向着栅极202方向的横向注入深度的作用。在本发明的其他实施例中,在步骤S1中可以先不制作侧墙203,在步骤S2中可以直接以栅极堆叠结构为掩膜,进行源漏离子注入,形成要求横向注入深度的源漏注入区204’,在步骤S3中,先形成侧墙203,然后以侧墙203和栅极堆叠结构为掩膜,进行反型离子注入,以形成要求横向延伸深度的反型注入区205’。显然,在该实施例中,由于侧墙203是在形成源漏注入区204’之后形成的,因此反型注入区205’的横向注入深度小于源漏注入区204’的横向注入深度。In addition, in this embodiment, the
请参考图9,在步骤S4中,通过快速退火工艺,对衬底200进行退火处理,以使得源漏注入区204’的离子在横向上和纵向上继续扩散,反型注入区205’在横向和纵向上继续扩散。由此,源漏注入区204’经扩散后形成为重掺杂区204a以及包围重掺杂区204a的延伸扩展区204b,重掺杂区204a的掺杂浓度高于延伸扩展区204b,反型注入区205’经扩散和离子中和后形成为反型掺杂区205。其中,在退火处理过程中,一方面,由于反型注入区205’的存在,源漏注入区204’在横向和纵向上的延伸扩展,均会受到反型注入区205’的杂质补偿效应影响,因此能够在栅极202下方形成更浅的结,并在延伸扩展区204b中形成耗尽区;另一方面,反型注入区205’在横向和纵向上的延伸扩展,也会受到源漏注入区204’的杂质补偿效应影响,因此能够使得反型掺杂区205在源/漏区204中的区域占比得到控制,进而阻止反型掺杂区205扩散延伸到栅极202下方。Referring to FIG. 9, in step S4, the
因此,在退火处理过程中,反型注入区205’和源漏注入区204’这两个掺杂类型相反的注入区,相互影响,最终改善了源/漏区204中的电场分布,减小了源/漏结漏电流,提高了源漏击穿电压,进而改善了MOS晶体管的电学特性,且可以保证反型掺杂区205的上下边界以及面向沟道的边界均与源/漏区204的相应边界有距离,继而可以避免反型掺杂区205的加入对沟道带来不利影响。Therefore, during the annealing process, the two implanted regions with opposite doping types, the inversion implanted region 205' and the source-drain implanted region 204', interact with each other, which ultimately improves the electric field distribution in the source/
本实施例的MOS晶体管的制造方法,能够通过高能量离子注入工程,可以在源/漏区中形成用于改善器件电学特性的反型掺杂区,进而制造出高性能的MOS晶体管,且工艺简单,成本低。In the method for manufacturing a MOS transistor in this embodiment, an inversion doped region for improving the electrical characteristics of the device can be formed in the source/drain region through a high-energy ion implantation process, thereby manufacturing a high-performance MOS transistor. Simple and low cost.
上述描述仅是对本发明较佳实施例的描述,并非对本发明范围的任何限定,本发明领域的普通技术人员根据上述揭示内容做的任何变更、修饰,均属于本发明技术方案的范围。The above description is only a description of the preferred embodiments of the present invention, and does not limit the scope of the present invention. Any changes and modifications made by those of ordinary skill in the field of the present invention according to the above disclosure belong to the scope of the technical solutions of the present invention.
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| EP0596468A2 (en) * | 1992-11-04 | 1994-05-11 | Matsushita Electric Industrial Co., Ltd. | MOSFET of LDD type and a method for fabricating the same |
| US6451675B1 (en) * | 2000-09-12 | 2002-09-17 | United Microelectronics Corp. | Semiconductor device having varied dopant density regions |
| CN102544092A (en) * | 2010-12-16 | 2012-07-04 | 无锡华润上华半导体有限公司 | CMOS (complementary metal oxide semiconductor) device and manufacturing method thereof |
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| JPH05110081A (en) * | 1991-10-16 | 1993-04-30 | Seiko Epson Corp | Semiconductor device |
| EP0596468A2 (en) * | 1992-11-04 | 1994-05-11 | Matsushita Electric Industrial Co., Ltd. | MOSFET of LDD type and a method for fabricating the same |
| US6451675B1 (en) * | 2000-09-12 | 2002-09-17 | United Microelectronics Corp. | Semiconductor device having varied dopant density regions |
| CN102544092A (en) * | 2010-12-16 | 2012-07-04 | 无锡华润上华半导体有限公司 | CMOS (complementary metal oxide semiconductor) device and manufacturing method thereof |
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