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CN103943502B - Fin formula field effect transistor and forming method thereof - Google Patents

Fin formula field effect transistor and forming method thereof Download PDF

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CN103943502B
CN103943502B CN201310024103.7A CN201310024103A CN103943502B CN 103943502 B CN103943502 B CN 103943502B CN 201310024103 A CN201310024103 A CN 201310024103A CN 103943502 B CN103943502 B CN 103943502B
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effect transistor
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CN103943502A (en
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三重野文健
殷华湘
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Semiconductor Manufacturing International Shanghai Corp
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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]
    • H10D30/024Manufacture or treatment of FETs having insulated gates [IGFET] of fin field-effect transistors [FinFET]
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/60Insulated-gate field-effect transistors [IGFET]
    • H10D30/62Fin field-effect transistors [FinFET]
    • 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
    • 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
    • H10D62/17Semiconductor regions connected to electrodes not carrying current to be rectified, amplified or switched, e.g. channel regions
    • H10D62/213Channel regions of field-effect devices
    • H10D62/221Channel regions of field-effect devices of FETs
    • H10D62/235Channel regions of field-effect devices of FETs of IGFETs
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D64/00Electrodes of devices having potential barriers
    • H10D64/20Electrodes characterised by their shapes, relative sizes or dispositions 
    • H10D64/27Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
    • H10D64/311Gate electrodes for field-effect devices
    • H10D64/411Gate electrodes for field-effect devices for FETs
    • H10D64/511Gate electrodes for field-effect devices for FETs for IGFETs

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  • Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)

Abstract

一种鳍式场效应晶体管及其形成方法,其中所述鳍式场效应晶体管的形成方法包括:提供半导体衬底,所述半导体衬底具有第一区域和第二区域,所述第一区域和第二区域内具有凸起的鳍部、位于所述鳍部上的栅极结构;在所述第一区域的栅极结构两侧形成第一侧墙,所述第一侧墙覆盖的部分鳍部构成第一负遮盖区;在所述第二区域的栅极结构两侧形成第二侧墙,所述第二侧墙的宽度小于所述第一侧墙的宽度,所述第二侧墙覆盖的部分鳍部构成第二负遮盖区;对所述第一区域和第二区域的栅极结构两侧的鳍部进行离子注入,形成源区和漏区。本发明的鳍式场效应晶体管的形成方法可以形成具有不同阈值电压的鳍式场效应晶体管,且工艺简单。

A fin field effect transistor and its forming method, wherein the forming method of the fin field effect transistor includes: providing a semiconductor substrate, the semiconductor substrate has a first region and a second region, the first region and There are raised fins in the second region and a gate structure on the fins; first sidewalls are formed on both sides of the gate structure in the first region, and part of the fins covered by the first sidewalls The portion constitutes a first negative covering region; second sidewalls are formed on both sides of the gate structure in the second region, the width of the second sidewalls is smaller than the width of the first sidewalls, and the second sidewalls The covered part of the fin constitutes a second negative covering region; ion implantation is performed on the fins on both sides of the gate structure in the first region and the second region to form a source region and a drain region. The fin field effect transistor forming method of the present invention can form fin field effect transistors with different threshold voltages, and the process is simple.

Description

鳍式场效应晶体管及其形成方法Fin field effect transistor and method of forming the same

技术领域technical field

本发明涉及半导体技术领域,尤其涉及一种鳍式场效应晶体管及其形成方法。The invention relates to the technical field of semiconductors, in particular to a fin field effect transistor and a forming method thereof.

背景技术Background technique

随着集成电路工艺技术的进步,使得芯片的集成度越来越高,规模也越来越大,但芯片的功耗也随之增大。单个芯片上通常包括了核心逻辑晶体管区域和输入/输出(I/O)晶体管区域,核心逻辑晶体管的阈值电压较低以降低系统功耗,而输入/输出晶体管的阈值电压较高以保证较高的驱动能力和击穿电压。因此,如何在单个芯片上获得不同阈值电压的晶体管成为了研究的重点。With the advancement of integrated circuit technology, the integration level of the chip is getting higher and higher, and the scale is getting larger and larger, but the power consumption of the chip is also increasing. A single chip usually includes a core logic transistor area and an input/output (I/O) transistor area. The threshold voltage of the core logic transistor is low to reduce system power consumption, and the threshold voltage of the input/output transistor is high to ensure high drive capability and breakdown voltage. Therefore, how to obtain transistors with different threshold voltages on a single chip has become the focus of research.

请参考图1,为现有技术的MOS晶体管的结构示意图,包括:半导体衬底100;位于所述半导体衬底100上的栅介质层102;位于所述栅介质层102上的功函数层103;位于所述功函数层103上的栅电极层104;位于所述介质层102、所述功函数层103和所述栅电极层104两侧的侧墙105;位于所述栅电极层104两侧的半导体衬底100内的源区和漏区106。现有技术的MOS晶体管中,通过选择适当的功函数层103的材料,如TiN、TaAl或TiC等,改变MOS晶体管栅电极和栅介质层之间的功函数差,来调节MOS晶体管的阈值电压,在同一芯片上获得不同阈值电压的晶体管,使输入/输出晶体管的阈值电压较高,核心逻辑晶体管的阈值电压较低。由于所述功函数层103通常为多层结构,且应用于NMOS晶体管和PMOS晶体管的功函数层材料不同,形成工艺复杂。尤其在鳍式场效应晶体管中,功函数层形成在凸出于半导体衬底的鳍部之上,进一步增加了工艺难度,成本高。Please refer to FIG. 1, which is a schematic structural diagram of a MOS transistor in the prior art, including: a semiconductor substrate 100; a gate dielectric layer 102 located on the semiconductor substrate 100; a work function layer 103 located on the gate dielectric layer 102 ; the gate electrode layer 104 located on the work function layer 103; the sidewalls 105 located on both sides of the dielectric layer 102, the work function layer 103 and the gate electrode layer 104; The source region and the drain region 106 in the semiconductor substrate 100 on the side. In the MOS transistors of the prior art, the threshold voltage of the MOS transistor is adjusted by changing the work function difference between the gate electrode of the MOS transistor and the gate dielectric layer by selecting an appropriate material for the work function layer 103, such as TiN, TaAl or TiC. , to obtain transistors with different threshold voltages on the same chip, so that the threshold voltage of the input/output transistor is higher, and the threshold voltage of the core logic transistor is lower. Since the work function layer 103 is usually a multi-layer structure, and the materials of the work function layer applied to NMOS transistors and PMOS transistors are different, the formation process is complicated. Especially in the fin field effect transistor, the work function layer is formed on the fin protruding from the semiconductor substrate, which further increases the difficulty of the process and the cost is high.

因此,现有技术的多阈值电压的鳍式场效应晶体管的形成方法,工艺复杂,成本高。Therefore, the prior art method for forming fin field effect transistors with multiple threshold voltages is complicated in process and high in cost.

其他有关多阈值电压晶体管的形成方法还可以参考公开号为US2011/0248351A1的美国专利申请。For other methods of forming multi-threshold voltage transistors, reference may also be made to US Patent Application Publication No. US2011/0248351A1.

发明内容Contents of the invention

本发明解决的问题是现有技术形成多阈值电压晶体管的工艺复杂,成本高。The problem solved by the invention is that the process of forming multi-threshold voltage transistors in the prior art is complicated and the cost is high.

为解决上述问题,本发明提出了一种鳍式场效应晶体管的形成方法,包括:提供半导体衬底,所述半导体衬底具有第一区域和第二区域,所述第一区域和第二区域内具有凸起的鳍部、位于所述鳍部上的栅极结构,所述栅极结构覆盖部分所述鳍部的顶部和侧壁;在所述第一区域的栅极结构两侧形成第一侧墙,所述第一侧墙覆盖的部分鳍部构成第一负遮盖区;在所述第二区域的栅极结构两侧形成第二侧墙,所述第二侧墙的宽度小于所述第一侧墙的宽度,所述第二侧墙覆盖的部分鳍部构成第二负遮盖区;对所述第一区域和第二区域的栅极结构两侧的鳍部进行离子注入,形成源区和漏区。In order to solve the above problems, the present invention proposes a method for forming a fin field effect transistor, comprising: providing a semiconductor substrate, the semiconductor substrate has a first region and a second region, and the first region and the second region There are protruding fins and a gate structure on the fins, the gate structure covers part of the top and sidewalls of the fins; a second gate structure is formed on both sides of the gate structure in the first region. A side wall, the part of the fin covered by the first side wall constitutes a first negative cover area; a second side wall is formed on both sides of the gate structure in the second region, and the width of the second side wall is smaller than the The width of the first sidewall, the part of the fins covered by the second sidewall constitutes the second negative cover region; ion implantation is performed on the fins on both sides of the gate structure in the first region and the second region to form source and drain regions.

可选的,所述第二负遮盖区的宽度小于所述第一负遮盖区的宽度。Optionally, the width of the second negative masking area is smaller than the width of the first negative masking area.

可选的,所述第一负遮盖区的宽度范围为300埃~500埃。Optionally, the width of the first negative masking region ranges from 300 angstroms to 500 angstroms.

可选的,所述第二负遮盖区的宽度范围为10埃~50埃。Optionally, the width of the second negative masking region ranges from 10 angstroms to 50 angstroms.

可选的,所述第一区域形成的鳍式场效应晶体管作为输入/输出晶体管。Optionally, the fin field effect transistor formed in the first region serves as an input/output transistor.

可选的,所述第一负遮盖区的掺杂浓度与所述输入/输出晶体管沟道区域的掺杂浓度相同。Optionally, the doping concentration of the first negative covering region is the same as that of the channel region of the input/output transistor.

可选的,还包括对所述输入/输出晶体管的漏区端的第一负遮盖区进行离子注入,形成反型掺杂区。Optionally, the method further includes performing ion implantation on the first negative covering region at the drain region end of the input/output transistor to form an inversion doped region.

可选的,所述反型掺杂区的掺杂类型与所述输入/输出晶体管的源区和漏区掺杂类型相反。Optionally, the doping type of the inverse doping region is opposite to that of the source region and the drain region of the input/output transistor.

可选的,所述反型掺杂区的宽度范围为1埃~300埃。Optionally, the width of the inversion doped region ranges from 1 angstrom to 300 angstrom.

可选的,所述第二区域形成的鳍式场效应晶体管作为核心逻辑晶体管。Optionally, the fin field effect transistor formed in the second region serves as a core logic transistor.

可选的,所述第二负遮盖区的掺杂浓度与所述核心逻辑晶体管沟道区域的掺杂浓度相同。Optionally, the doping concentration of the second negative covering region is the same as that of the channel region of the core logic transistor.

可选的,所述第一侧墙和第二侧墙的材料为高介电常数材料。Optionally, the first sidewall and the second sidewall are made of high dielectric constant material.

可选的,所述高介电常数材料为HfO2、Al2O3、ZrO2、HfSiO、HfSiON、HfTaO和HfZrO中的一种或几种。Optionally, the high dielectric constant material is one or more of HfO 2 , Al 2 O 3 , ZrO 2 , HfSiO, HfSiON, HfTaO and HfZrO.

可选的,还包括对所述第一区域和第二区域的栅极结构两侧的鳍部进行预非晶化离子注入。Optionally, the method further includes performing pre-amorphization ion implantation on the fins on both sides of the gate structure in the first region and the second region.

可选的,所述预非晶化离子注入的注入离子为Si、C、Ge、Xe或者Ar。Optionally, the implanted ions of the pre-amorphization ion implantation are Si, C, Ge, Xe or Ar.

对应的,本发明还提出了一种鳍式场效应晶体管,包括:半导体衬底,所述半导体衬底具有第一区域和第二区域,所述第一区域和第二区域内具有凸起的鳍部;位于所述鳍部上的栅极结构,所述栅极结构覆盖部分所述鳍部的顶部和侧壁;位于所述第一区域的栅极结构两侧的第一侧墙,所述第一侧墙覆盖的部分鳍部构成第一负遮盖区;位于所述第二区域的栅极结构两侧的第二侧墙,所述第二侧墙的宽度大于所述第一侧墙的宽度,所述第二侧墙覆盖的部分鳍部构成第二负遮盖区;位于所述第一区域和第二区域的栅极结构两侧的鳍部内的源区和漏区。Correspondingly, the present invention also proposes a fin field effect transistor, comprising: a semiconductor substrate, the semiconductor substrate has a first region and a second region, and the first region and the second region have raised a fin; a gate structure located on the fin, the gate structure covering part of the top and sidewalls of the fin; first sidewalls located on both sides of the gate structure in the first region, the Part of the fin covered by the first sidewall constitutes a first negative cover area; second sidewalls located on both sides of the gate structure in the second region, the width of the second sidewall is greater than that of the first sidewall The part of the fin covered by the second spacer constitutes the second negative cover area; the source region and the drain region in the fin located on both sides of the gate structure in the first region and the second region.

可选的,所述第二负遮盖区的宽度小于所述第一负遮盖区的宽度。Optionally, the width of the second negative masking area is smaller than the width of the first negative masking area.

可选的,所述第一区域为输入/输出晶体管区域,所述第二区域为核心逻辑晶体管区域。Optionally, the first area is an input/output transistor area, and the second area is a core logic transistor area.

可选的,还包括位于所述输入/输出晶体管的漏区端的第一负遮盖区内的反型掺杂区,所述反型掺杂区的掺杂类型与所述输入/输出晶体管的源区和漏区掺杂类型相反,所述反型掺杂区的宽度范围为1埃~300埃。Optionally, it also includes an inversion doped region located in the first negative covering region at the drain region end of the input/output transistor, the doping type of the inversion doped region is the same as that of the source of the input/output transistor The doping types of the region and the drain region are opposite, and the width of the inversion doping region ranges from 1 angstrom to 300 angstroms.

可选的,所述第一侧墙和第二侧墙的材料为高介电常数材料。Optionally, the first sidewall and the second sidewall are made of high dielectric constant material.

与现有技术相比,本发明具有以下优点:Compared with the prior art, the present invention has the following advantages:

本发明实施例的鳍式场效应晶体管的形成方法中,在第一区域的栅极结构两侧形成第一侧墙,在第二区域的栅极结构两侧形成第二侧墙,由于所述第一侧墙和第二侧墙的宽度不同,位于所述第一侧墙下的第一负遮盖区和位于第二侧墙下的第二负遮盖区的宽度不同。在具有负遮盖区的鳍式场效应晶体管中,不同的负遮盖区的宽度导致后续形成的鳍式场效应晶体管的有效沟道宽度不同,改变了沟道区域电场分布,影响鳍式场效应晶体管的阈值电压。本发明实施例正是利用负遮盖区宽度对鳍式场效应晶体管阈值电压的影响,在鳍式场效应晶体管的形成过程中,通过控制在第一区域和第二区域形成的侧墙的宽度,来控制第一负遮盖区和第二负遮盖区的宽度,获得具有不同阈值电压的鳍式场效应晶体管,工艺简单,成本低。In the method for forming a fin field effect transistor according to an embodiment of the present invention, first sidewalls are formed on both sides of the gate structure in the first region, and second sidewalls are formed on both sides of the gate structure in the second region. The widths of the first side wall and the second side wall are different, and the widths of the first negative covering area under the first side wall and the second negative covering area under the second side wall are different. In a FinFET with a negative cover region, different widths of the negative cover region lead to different effective channel widths of the subsequently formed FinFET, which changes the electric field distribution in the channel region and affects the FinFET. threshold voltage. The embodiment of the present invention utilizes the influence of the width of the negative covering region on the threshold voltage of the FinFET, and controls the width of the sidewalls formed in the first region and the second region during the formation of the FinFET. The widths of the first negative cover region and the second negative cover region are controlled to obtain fin field effect transistors with different threshold voltages, and the process is simple and the cost is low.

进一步的,本发明实施例的鳍式场效应晶体管的形成方法中,所述第一区域形成的鳍式场效应晶体管作为输入/输出晶体管,由于输入/输出晶体管通常需要较高的阈值电压和击穿电压,因此,对所述输入/输出晶体管的漏区端的第一负遮盖区进行离子注入,形成反型掺杂区。所述反型掺杂区的掺杂类型与所述输入/输出晶体管的源区和漏区掺杂类型相反,在所述反型掺杂区和漏区之间形成势垒,进一步提高了所述输入/输出晶体管的击穿电压和阈值电压。Further, in the method for forming a fin field effect transistor in the embodiment of the present invention, the fin field effect transistor formed in the first region is used as an input/output transistor, since the input/output transistor usually requires a higher threshold voltage and Therefore, ion implantation is performed on the first negative covering region at the drain region end of the input/output transistor to form an inversion doped region. The doping type of the inversion doping region is opposite to the doping type of the source region and the drain region of the input/output transistor, and a potential barrier is formed between the inversion doping region and the drain region, further improving the breakdown and threshold voltages of the input/output transistors described above.

对应的,本发明实施例的鳍式场效应晶体管采用上述的方法所形成,因此位于第一区域的鳍式场效应晶体管和位于第二区域的鳍式场效应晶体管具有不同的阈值电压。Correspondingly, the FinFETs in the embodiment of the present invention are formed by the above method, so the FinFETs located in the first region and the FinFETs located in the second region have different threshold voltages.

附图说明Description of drawings

图1是现有技术的MOS晶体管的结构示意图;FIG. 1 is a schematic structural diagram of a MOS transistor in the prior art;

图2至图6是本发明实施例的鳍式场效应晶体管形成过程的结构示意图。FIG. 2 to FIG. 6 are structural schematic diagrams of the forming process of the fin field effect transistor according to the embodiment of the present invention.

具体实施方式detailed description

由背景技术可知,现有技术形成具有多阈值电压的鳍式场效应晶体管的工艺复杂,成本高。It can be seen from the background art that in the prior art, the process of forming the fin field effect transistor with multiple threshold voltages is complicated and the cost is high.

本发明的发明人研究了具有负遮盖区(Underlap)的鳍式场效应晶体管的形成方法,发现由于负遮盖区没有进行轻掺杂漏区注入(LDD)和晕环注入(Halo Implantation),所述负遮盖区可以增大鳍式场效应晶体管的有效沟道区域宽度,缓解短沟道效应。而且不同负遮盖区的宽度对鳍式场效应晶体管的沟道区域电场分布影响不同、对阈值电压影响不同,因此可以通过控制形成的负遮盖区的宽度来获得具有不同阈值电压的鳍式场效应晶体管。The inventors of the present invention have studied the formation method of a fin field effect transistor with a negative cover region (Underlap), and found that because the negative cover region is not subjected to lightly doped drain implantation (LDD) and halo implantation (Halo Implantation), the The above-mentioned negative covering region can increase the width of the effective channel region of the fin field effect transistor and alleviate the short channel effect. Moreover, the widths of different negative cover regions have different influences on the electric field distribution in the channel region of the fin field effect transistor, and have different effects on the threshold voltage. Therefore, fin field effects with different threshold voltages can be obtained by controlling the width of the formed negative cover region. transistor.

基于以上研究,本发明的发明人提出了一种鳍式场效应晶体管的形成方法,在半导体衬底第一区域和第二区域的栅极结构两侧形成具有不同宽度的第一侧墙和第二侧墙,由于位于所述第一侧墙下的第一负遮盖区和位于所述第二侧墙下的第二负遮盖区的宽度不同,所述第一区域形成的鳍式场效应晶体管和第二区域形成的鳍式场效应晶体管的阈值电压不同。降低了形成具有不同阈值电压的鳍式场效应晶体管的工艺难度,制造成本低。Based on the above studies, the inventors of the present invention proposed a method for forming a fin field effect transistor, forming first sidewalls and second sidewalls with different widths on both sides of the gate structure in the first region and the second region of the semiconductor substrate. Two sidewalls, because the width of the first negative cover area under the first side wall is different from that of the second negative cover area under the second side wall, the fin field effect transistor formed in the first area The threshold voltage of the fin field effect transistor formed in the second region is different from that of the fin field effect transistor. The process difficulty of forming fin field effect transistors with different threshold voltages is reduced, and the manufacturing cost is low.

下面结合附图详细地描述具体实施例,上述的目的和本发明的优点将更加清楚。The specific embodiments will be described in detail below in conjunction with the accompanying drawings, and the above-mentioned purpose and advantages of the present invention will be more clear.

图2至图6是本发明实施例的鳍式场效应晶体管形成过程的结构示意图。FIG. 2 to FIG. 6 are structural schematic diagrams of the forming process of the fin field effect transistor according to the embodiment of the present invention.

请参考图2,提供半导体衬底200,所述半导体衬底200具有第一区域Ι和第二区域Ⅱ,所述第一区域Ι和第二区域Ⅱ内具有突出的鳍部202、位于所述鳍部202上的栅极结构203,所述栅极结构203覆盖部分所述鳍部202的顶部和侧壁。Please refer to FIG. 2 , a semiconductor substrate 200 is provided, the semiconductor substrate 200 has a first region I and a second region II, the first region I and the second region II have protruding fins 202 located in the The gate structure 203 on the fin 202 , the gate structure 203 covers part of the top and sidewall of the fin 202 .

所述半导体衬底200可以是硅或者绝缘体上硅(SOI),所述半导体衬底200也可以是锗、锗硅、砷化镓或者绝缘体上锗。所述半导体衬底200具有第一区域Ι和第二区域Ⅱ,所述第一区域Ι和第二区域Ⅱ分别用于形成具有不同阈值电压的鳍式场效应晶体管。所述半导体衬底200表面具有凸起的鳍部202,所述鳍部202与所述半导体衬底200的连接方式可以是一体的,例如所述鳍部202是通过对所述半导体衬底200刻蚀后形成的凸起结构。所述栅极结构203位于所述鳍部202上,所述栅极结构203覆盖部分所述鳍部202的顶部和侧壁。本实施例中,所述栅极结构203包括栅介质层和栅电极层(未示出),所述栅介质层的材料为氧化硅,所述栅电极层的材料为多晶硅。The semiconductor substrate 200 may be silicon or silicon-on-insulator (SOI), and the semiconductor substrate 200 may also be germanium, silicon germanium, gallium arsenide, or germanium-on-insulator. The semiconductor substrate 200 has a first region I and a second region II, and the first region I and the second region II are respectively used to form fin field effect transistors with different threshold voltages. The surface of the semiconductor substrate 200 has a raised fin 202, and the connection between the fin 202 and the semiconductor substrate 200 can be integrated, for example, the fin 202 is connected to the semiconductor substrate 200 The raised structure formed after etching. The gate structure 203 is located on the fin 202 , and the gate structure 203 covers part of the top and sidewall of the fin 202 . In this embodiment, the gate structure 203 includes a gate dielectric layer and a gate electrode layer (not shown), the material of the gate dielectric layer is silicon oxide, and the material of the gate electrode layer is polysilicon.

在另一实施例中,所述栅极结构为伪栅极,所述伪栅极的材料为多晶硅。所述伪栅极在高介电常数栅介质层和金属栅极(HKMG)的后栅形成工艺中,用于减小后续形成的高介电常数栅介质层和金属栅电极的热预算。后续工艺中去除所述伪栅极后,在所述伪栅极的位置依次形成高介电常数栅介质层和金属栅极。In another embodiment, the gate structure is a dummy gate, and the material of the dummy gate is polysilicon. The dummy gate is used to reduce the thermal budget of the subsequently formed high dielectric constant gate dielectric layer and metal gate electrode in the gate-last formation process of the high dielectric constant gate dielectric layer and the metal gate (HKMG). After the dummy gate is removed in a subsequent process, a high dielectric constant gate dielectric layer and a metal gate are sequentially formed at the position of the dummy gate.

本实施例中,还包括位于所述半导体衬底200表面,且覆盖部分所述鳍部202侧壁的浅沟槽隔离结构201(STI)。所述浅沟槽隔离结构201用于将所述半导体衬底200内的不同鳍部隔离,所述浅沟槽隔离结构201的材料为氧化硅,所述浅沟槽隔离结构的形成方法可以参考现有工艺,在此不再赘述。In this embodiment, a shallow trench isolation structure 201 (STI) located on the surface of the semiconductor substrate 200 and covering part of the sidewall of the fin 202 is also included. The shallow trench isolation structure 201 is used to isolate different fins in the semiconductor substrate 200, the material of the shallow trench isolation structure 201 is silicon oxide, and the formation method of the shallow trench isolation structure can refer to The existing technology will not be repeated here.

请参考图3,图3为在图2的基础上形成鳍式场效应晶体管的过程中,沿AA1方向的剖面结构示意图,在所述第一区域Ι的栅极结构203两侧形成第一侧墙204,所述第一侧墙204覆盖的部分鳍部202构成第一负遮盖区(未标示)。Please refer to FIG. 3. FIG. 3 is a schematic cross-sectional structure diagram along the AA1 direction during the process of forming a fin field effect transistor on the basis of FIG. The wall 204 , and the part of the fin 202 covered by the first side wall 204 constitutes a first negative covering area (not shown).

具体的,首先形成第一光刻胶层(未图示),所述第一光刻胶层覆盖所述第二区域Ⅱ,所述第一光刻胶层在后续工艺中用于保护所述第二区域Ⅱ的鳍部202和栅极结构203;其次,采用物理气相沉积、化学气相沉积或者原子层沉积工艺在所述第一区域Ι的鳍部202上形成第一侧墙材料层(未图示),所述第一侧墙材料层覆盖所述第一区域Ι的栅极结构203,所述第一侧墙材料层具有较高的介电常数,例如所述第一侧墙材料层为HfO2、Al2O3、ZrO2、HfSiO、HfSiON、HfTaO和HfZrO中的一种或几种;接着采用干法刻蚀工艺回刻蚀所述第一侧墙材料层,由于干法刻蚀具有较好的方向性,回刻蚀所述以第一侧墙材料层后,仅位于所述第一区域Ι的栅极结构203两侧的第一侧墙材料层保留形成第一侧墙204,位于所述第一区域Ι的栅极结构203顶部和其余区域的第一侧墙材料层被去除;去除所述第一光刻胶层。Specifically, a first photoresist layer (not shown) is first formed, the first photoresist layer covers the second region II, and the first photoresist layer is used to protect the The fin portion 202 and the gate structure 203 in the second region II; secondly, a first spacer material layer (not shown) is formed on the fin portion 202 in the first region I by using physical vapor deposition, chemical vapor deposition or atomic layer deposition process As shown in the figure), the first sidewall material layer covers the gate structure 203 in the first region I, and the first sidewall material layer has a relatively high dielectric constant, for example, the first sidewall material layer It is one or more of HfO 2 , Al 2 O 3 , ZrO 2 , HfSiO, HfSiON, HfTaO and HfZrO; then the first sidewall material layer is etched back by a dry etching process, because the dry etching The etching has better directionality. After etching back the first sidewall material layer, only the first sidewall material layer located on both sides of the gate structure 203 in the first region I remains to form the first sidewall 204, removing the first sidewall material layer located on the top of the gate structure 203 in the first region I and the rest of the region; removing the first photoresist layer.

形成所述第一侧墙204后,所述第一侧墙204覆盖的部分鳍部202构成第一负遮盖区。由于第一负遮盖区在后续工艺中不会进行轻掺杂漏区注入和晕环注入,所述第一负遮盖区的掺杂浓度与后续形成的第一区域Ι的鳍式场效应晶体管的沟道区域的掺杂浓度和掺杂类型相同,可以增大第一区域Ι的鳍式场效应晶体管的有效沟道宽度,缓解短沟道效应。且由于所述第一侧墙204具有较高的介电常数,可以提高第一负遮盖区的电容值,使得后续形成于第一区域Ι的鳍式场效应晶体管的驱动电流不会因为第一负遮盖区的掺杂浓度较低而导致驱动电流降低。After the first sidewall 204 is formed, the part of the fin 202 covered by the first sidewall 204 constitutes a first negative covering area. Since lightly doped drain region implantation and halo implantation will not be performed in the first negative cover region in the subsequent process, the doping concentration of the first negative cover region is the same as that of the fin field effect transistor in the first region I formed subsequently. The doping concentration and doping type of the channel region are the same, which can increase the effective channel width of the FinFET in the first region I and alleviate the short channel effect. And because the first spacer 204 has a higher dielectric constant, the capacitance value of the first negative cover region can be increased, so that the driving current of the fin field effect transistor subsequently formed in the first region I will not be affected by the first The lower doping concentration of the negative cover region results in lower driving current.

本实施例中,所述第一区域Ι形成的鳍式场效应晶体管作为输入/输出晶体管,所述输入/输出晶体管通常需要具有较高的阈值电压。所述第一负遮盖区的宽度范围为300埃~500埃,所述第一负遮盖区的宽度范围可以通过调节所述第一侧墙204的宽度来控制。在具有负遮盖区的鳍式场效应晶体管中,不同的负遮盖区的宽度会导致鳍式场效应晶体管的有效沟道宽度不同,沟道区域电场分布不同,鳍式场效应晶体管的阈值电压也不同,且鳍式场效应晶体管的阈值电压会随着负遮盖区的宽度增加而增大。本实施例中,所述第一负遮盖区的宽度较大,所形成的输入/输出晶体管的阈值电压也较高。In this embodiment, the fin field effect transistors formed in the first region I are used as input/output transistors, and the input/output transistors generally need to have a relatively high threshold voltage. The width range of the first negative masking region is 300 Ř500 Å, and the width range of the first negative masking region can be controlled by adjusting the width of the first sidewall 204 . In a FinFET with a negative cover region, different widths of the negative cover region will result in different effective channel widths of the FinFET, different electric field distributions in the channel region, and different threshold voltages of the FinFET. different, and the threshold voltage of the FinFET will increase with the increase of the width of the negative cover region. In this embodiment, the width of the first negative covering region is larger, and the threshold voltage of the formed input/output transistor is also higher.

请参考图4,在所述第二区域Ⅱ的栅极结构203两侧形成第二侧墙205,所述第二侧墙205的宽度小于所述第一侧墙204的宽度,所述第二侧墙205覆盖的部分鳍部202构成第二负遮盖区(未标示)。Referring to FIG. 4 , second sidewalls 205 are formed on both sides of the gate structure 203 in the second region II, and the width of the second sidewalls 205 is smaller than the width of the first sidewalls 204 . Part of the fin portion 202 covered by the side wall 205 constitutes a second negative covering area (not shown).

具体的,首先形成第二光刻胶层(未图示),所述第二光刻胶层覆盖所述第一区域Ι,所述第二光刻胶层在后续工艺用于保护第一区域Ι的鳍部202、栅极结构203和第一侧墙204;其次,采用物理气相沉积、化学气相沉积或者原子层沉积工艺在所述第二区域Ⅱ的鳍部202上形成第二侧墙材料层(未示出),所述第二侧墙材料层覆盖所述第二区域Ⅱ的栅极结构203,所述第二侧墙材料层具有较高的介电常数,所述第二侧墙材料层为HfO2、Al2O3、ZrO2、HfSiO、HfSiON、HfTaO和HfZrO中的一种或几种,所述第二侧墙材料层可以与第一侧墙204的材料相同或者不同;采用干法刻蚀工艺回刻蚀所述第二侧墙材料层,形成位于所述第二区域Ⅱ的栅极结构203两侧第二侧墙205;去除所述第二光刻胶层。Specifically, first form a second photoresist layer (not shown), the second photoresist layer covers the first region I, and the second photoresist layer is used to protect the first region in subsequent processes The fin portion 202, gate structure 203 and first sidewall 204 of I; secondly, a second sidewall material is formed on the fin portion 202 of the second region II by using physical vapor deposition, chemical vapor deposition or atomic layer deposition process layer (not shown), the second sidewall material layer covers the gate structure 203 in the second region II, the second sidewall material layer has a relatively high dielectric constant, and the second sidewall material layer The material layer is one or more of HfO 2 , Al 2 O 3 , ZrO 2 , HfSiO, HfSiON, HfTaO and HfZrO, and the second sidewall material layer can be the same as or different from the material of the first sidewall 204; Etching back the second sidewall material layer by using a dry etching process to form second sidewalls 205 on both sides of the gate structure 203 in the second region II; removing the second photoresist layer.

形成所述第二侧墙205后,所述第二侧墙205覆盖的部分鳍部202构成第二负遮盖区,所述第二负遮盖区的掺杂浓度与形成于第二区域Ⅱ的鳍式场效应晶体管的沟道区域的掺杂浓度相同。本实施例中,所述第二区域Ⅱ形成的鳍式场效应晶体管作为核心逻辑晶体管,所述核心逻辑晶体管的阈值电压较低,以降低核心逻辑晶体管的功耗。请继续参考图4,在形成位于所述第二区域Ⅱ的核心逻辑晶体管的过程中,所述第二侧墙205的宽度小于所述第一侧墙204的宽度,所述第二侧墙205的宽度和所述第一侧墙204宽度是指所述第二侧墙205和所述第一侧墙204底部与所述鳍部202的接触面的宽度,本实施例中,所述第二负遮盖区的宽度范围为10埃~50埃。因此位于所述第二侧墙205下的第二负遮盖区的宽度小于位于所述第一侧墙204下的第一负遮盖区的宽度,由于鳍式场效应晶体管的阈值电压随着负遮盖区宽度的减小而减小,所述核心逻辑晶体管的阈值电压也小于所述输入/输出晶体管。After the second sidewall 205 is formed, the part of the fin 202 covered by the second sidewall 205 constitutes a second negative covering region, and the doping concentration of the second negative covering region is the same as that of the fins formed in the second region II. The doping concentration of the channel region of the field effect transistor is the same. In this embodiment, the fin field effect transistor formed in the second region II is used as a core logic transistor, and the threshold voltage of the core logic transistor is relatively low, so as to reduce power consumption of the core logic transistor. Please continue to refer to FIG. 4, in the process of forming the core logic transistor located in the second region II, the width of the second sidewall 205 is smaller than the width of the first sidewall 204, and the second sidewall 205 The width and the width of the first side wall 204 refer to the width of the contact surface between the bottom of the second side wall 205 and the first side wall 204 and the fin 202. In this embodiment, the second The width of the negative masking area ranges from 10 angstroms to 50 angstroms. Therefore, the width of the second negative shielding region located under the second sidewall 205 is smaller than the width of the first negative shielding region located under the first sidewall 204, since the threshold voltage of the FinFET increases with the negative shielding The threshold voltage of the core logic transistor is also smaller than that of the input/output transistor.

请参考图5,本实施例中,所述第一区域Ι形成的鳍式场效应晶体管作为输入/输出晶体管,为了进一步提高所述输入/输出晶体管的阈值电压和击穿电压,还对所述输入/输出晶体管的待形成漏区端的第一负遮盖区进行离子注入,形成反型掺杂区206。需要说明的是,图5中为了简洁明了,仅示出了位于第一区域Ι的输入/输出晶体管的剖面结构示意图。Please refer to FIG. 5. In this embodiment, the fin field effect transistor formed in the first region I is used as an input/output transistor. In order to further improve the threshold voltage and breakdown voltage of the input/output transistor, the Ion implantation is performed on the first negative covering region where the drain region end of the input/output transistor is to be formed to form an inversion doped region 206 . It should be noted that, for the sake of simplicity and clarity, FIG. 5 only shows a schematic cross-sectional structure diagram of the input/output transistor located in the first region I.

具体的,形成第三光刻胶层(未图示),所述第三光刻胶层覆盖所述第二区域Ⅱ,所述第三光刻胶层用于在后续的离子注入过程中保护所述第二区域Ⅱ;接着对所述输入/输出晶体管的漏极端的第一负遮盖区进行离子注入,形成反型掺杂区206。需要说明的,所述离子注入工艺的注入方向沿所述输入/输出晶体管的沟道方向,且与所述半导体衬底200表面具有夹角,使得在注入过程中,仅对输入/输出晶体管待形成漏区端的第一负遮盖区进行离子注入,形成反型掺杂区206,而由于所述栅极结构203的遮挡作用,不会对位于输入/输出晶体管待形成源区端的第一负遮盖区进行离子注入。Specifically, a third photoresist layer (not shown) is formed, the third photoresist layer covers the second region II, and the third photoresist layer is used to protect the region during the subsequent ion implantation process. The second region II; then perform ion implantation on the first negative covering region of the drain terminal of the input/output transistor to form an inversion doped region 206 . It should be noted that the implantation direction of the ion implantation process is along the channel direction of the input/output transistor, and has an included angle with the surface of the semiconductor substrate 200, so that only the input/output transistor is treated during the implantation process. Ion implantation is performed on the first negative cover region at the end of the drain region to form an inverse doped region 206, and due to the shielding effect of the gate structure 203, the first negative cover region at the end of the source region of the input/output transistor to be formed will not be affected. region for ion implantation.

所述反型掺杂区206的掺杂类型与所述输入/输出晶体管的源区和漏区的掺杂类型相反。本实施例中,所述输入/输出晶体管为NMOS晶体管,源区和漏区为N型掺杂,所述反型掺杂区206的掺杂类型为P型,例如可以为硼离子、磷离子或者镓离子掺杂。本实施例中,对所述输入/输出晶体管的漏区端的第一负遮盖区进行离子注入的注入离子为BF2,所述反型掺杂区206的宽度范围为1埃~300埃。由于所述反型掺杂区206的掺杂类型与所述输入/输出晶体管的源区和漏区掺杂类型相反,在所述反型掺杂区206和漏区之间形成势垒,进一步提高了所述输入/输出晶体管的击穿电压和阈值电压。The doping type of the inverse doping region 206 is opposite to that of the source region and the drain region of the I/O transistor. In this embodiment, the input/output transistor is an NMOS transistor, the source region and the drain region are N-type doped, and the doping type of the reverse-type doped region 206 is P-type, such as boron ions, phosphorus ions Or gallium ion doping. In this embodiment, BF 2 is used for ion implantation in the first negative covering region at the drain region end of the input/output transistor, and the width of the inversion doped region 206 ranges from 1 angstrom to 300 angstrom. Since the doping type of the inversion doping region 206 is opposite to the doping type of the source region and the drain region of the input/output transistor, a potential barrier is formed between the inversion doping region 206 and the drain region, further The breakdown voltage and threshold voltage of the input/output transistor are improved.

在另一实施例中,所述输入/输出晶体管为PMOS晶体管,源区和漏区为P型掺杂,所述反型掺杂区的掺杂类型为N型,例如可以为磷离子、砷离子或者锑离子掺杂。In another embodiment, the input/output transistor is a PMOS transistor, the source region and the drain region are P-type doped, and the doping type of the reverse-type doped region is N-type, such as phosphorus ions, arsenic ion or antimony ion doping.

请参考图6,对所述第一区域Ι和第二区域Ⅱ的栅极结构203两侧的鳍部202进行离子注入,形成源区207和漏区208。Referring to FIG. 6 , ion implantation is performed on the fins 202 on both sides of the gate structure 203 in the first region I and the second region II to form a source region 207 and a drain region 208 .

本实施例中,所述第一区域Ι和第二区域Ⅱ用于形成NMOS晶体管,对所述第一区域Ι和第二区域Ⅱ的栅极结构203两侧的鳍部202进行N型离子注入,例如可以为磷离子、砷离子或者锑离子注入,形成源区207和漏区208。需要说明的是,所述离子注入的方向垂直于所述NMOS晶体管的沟道方向,且与所述半导体衬底200表面具有夹角,使得在离子注入过程中,仅对所述栅极结构203两侧的鳍部202进行离子注入,而由于所述栅极结构203的遮挡作用,不会对第一区域Ι的第一负遮盖区和第二区域Ⅱ的第二负遮盖区进行离子注入,影响第一负遮盖区和第二负遮盖区的掺杂浓度。In this embodiment, the first region I and the second region II are used to form NMOS transistors, and N-type ion implantation is performed on the fins 202 on both sides of the gate structure 203 in the first region I and the second region II For example, phosphorus ions, arsenic ions or antimony ions can be implanted to form the source region 207 and the drain region 208 . It should be noted that, the direction of the ion implantation is perpendicular to the channel direction of the NMOS transistor, and has an included angle with the surface of the semiconductor substrate 200, so that only the gate structure 203 Ion implantation is performed on the fins 202 on both sides, and due to the shielding effect of the gate structure 203, ion implantation will not be performed on the first negative covering region of the first region I and the second negative covering region of the second region II, Affects the doping concentration of the first negative covering region and the second negative covering region.

在另一实施例中,所述第一区域Ι和第二区域Ⅱ用于形成PMOS晶体管,对所述第一区域Ι和第二区域Ⅱ的栅极结构两侧的鳍部进行P型离子注入,例如可以为硼离子、磷离子或者镓离子注入,形成源区和漏区。In another embodiment, the first region I and the second region II are used to form PMOS transistors, and P-type ion implantation is performed on the fins on both sides of the gate structure of the first region I and the second region II For example, boron ions, phosphorus ions or gallium ions can be implanted to form source regions and drain regions.

在另一实施例中,在形成源区和漏区前,还对所述第一区域Ι和第二区域Ⅱ的栅极结构两侧鳍部进行了预非晶化离子注入(PAI:Pre-Amorphization Implantation),所述预非晶化离子注入可以将待形成源区和漏区的鳍部表面的单晶材料转化为非晶材料。在后续进行源区和漏区的离子注入时,由于所述鳍部表面材料为非晶材料,晶格排列不规则,对注入离子的散射增强,使注入离子的分布更集中,拖尾更短,有利于提高所形成的鳍式场效应晶体管的性能。所述预非晶化注入的粒子为Si、C、Ge、Xe或者Ar。In another embodiment, before forming the source region and the drain region, pre-amorphization ion implantation (PAI: Pre- Amorphization Implantation), the pre-amorphization ion implantation can convert the single crystal material on the surface of the fin where the source region and the drain region are to be formed into an amorphous material. During the subsequent ion implantation of the source region and the drain region, since the fin surface material is an amorphous material, the crystal lattice arrangement is irregular, and the scattering of implanted ions is enhanced, so that the distribution of implanted ions is more concentrated and the tail is shorter , which is conducive to improving the performance of the formed fin field effect transistor. The particles implanted in the pre-amorphization are Si, C, Ge, Xe or Ar.

对应的,请继续参考图6,本发明还提出了一种鳍式场效应晶体管,包括:半导体衬底200,所述半导体衬底200表面具有第一区域Ι和第二区域Ⅱ,所述第一区域Ι和第二区域Ⅱ内具有凸起的鳍部202;位于所述鳍部202上的栅极结构203,所述栅极结构203覆盖部分所述鳍部202的顶部和侧壁;位于所述第一区域Ι的栅极结构203两侧的第一侧墙204,所述第一侧墙204覆盖的部分鳍部202构成第一负遮盖区(未示出);位于所述第二区域Ⅱ的栅极结构203两侧的第二侧墙205,所述第二侧墙205的宽度小于所述第一侧墙204的宽度,所述第一侧墙204和第二侧墙205的材料为高介电常数材料;所述第二侧墙205覆盖的部分鳍部202构成第二负遮盖区(未示出);位于所述第一区域Ι和第二区域Ⅱ的栅极结构203两侧的鳍部202内的源区207和漏区208。Correspondingly, please continue to refer to FIG. 6, the present invention also proposes a fin field effect transistor, including: a semiconductor substrate 200, the surface of the semiconductor substrate 200 has a first region I and a second region II, the first There are raised fins 202 in the first region I and the second region II; a gate structure 203 located on the fins 202, the gate structure 203 covers part of the top and sidewalls of the fins 202; The first sidewalls 204 on both sides of the gate structure 203 in the first region I, and the part of the fins 202 covered by the first sidewalls 204 form a first negative covering area (not shown); The second sidewalls 205 on both sides of the gate structure 203 in region II, the width of the second sidewalls 205 is smaller than the width of the first sidewalls 204, and the width of the first sidewalls 204 and the second sidewalls 205 The material is a high dielectric constant material; the part of the fins 202 covered by the second spacer 205 forms a second negative cover area (not shown); the gate structure 203 located in the first region I and the second region II The source region 207 and the drain region 208 in the fin portion 202 on both sides.

本实施例中,所述第一区域Ι为输入/输出晶体管区域,所述第二区域Ⅱ为核心逻辑晶体管区域。所述第二负遮盖区的宽度小于所述第一负遮盖区的宽度。本实施例中,还包括了位于所述输入/输出晶体管的漏区208端的第一负遮盖区内的反型掺杂区206,所述反型掺杂区206的掺杂类型与所述输入/输出晶体管的源区207和漏区208掺杂类型相反,所述反型掺杂区206的宽度范围为1埃~300埃。In this embodiment, the first area I is an input/output transistor area, and the second area II is a core logic transistor area. The width of the second negative masking area is smaller than the width of the first negative masking area. In this embodiment, an inversion doped region 206 located in the first negative cover region at the drain region 208 end of the input/output transistor is also included, and the doping type of the inversion doped region 206 is the same as that of the input The source region 207 and the drain region 208 of the output transistor have opposite doping types, and the width of the inverse doping region 206 ranges from 1 angstrom to 300 angstroms.

本实施例的鳍式场效应晶体管采用上述的鳍式场效应晶体管的形成方法所形成,因此,位于第一区域Ι的鳍式场效应晶体管和位于第二区域Ⅱ的鳍式场效应晶体管具有不同的阈值电压。The fin field effect transistor of this embodiment is formed using the above-mentioned fin field effect transistor forming method, therefore, the fin field effect transistor located in the first region I and the fin field effect transistor located in the second region II have different threshold voltage.

综上所述,与现有技术相比,本发明具有以下优点:In summary, compared with the prior art, the present invention has the following advantages:

本发明实施例的鳍式场效应晶体管的形成方法中,在第一区域的栅极结构两侧形成第一侧墙,在第二区域的栅极结构两侧形成第二侧墙,由于所述第一侧墙和第二侧墙的宽度不同,位于所述第一侧墙下的第一负遮盖区和位于第二侧墙下的第二负遮盖区的宽度不同。在具有负遮盖区的鳍式场效应晶体管中,不同的负遮盖区的宽度导致后续形成的鳍式场效应晶体管的有效沟道宽度不同,改变了沟道区域电场分布,影响鳍式场效应晶体管的阈值电压。本发明实施例正是利用负遮盖区宽度对鳍式场效应晶体管阈值电压的影响,在鳍式场效应晶体管的形成过程中,通过控制在第一区域和第二区域形成的侧墙的宽度,来控制第一负遮盖区和第二负遮盖区的宽度,获得具有不同阈值电压的鳍式场效应晶体管,工艺简单,成本低。In the method for forming a fin field effect transistor according to an embodiment of the present invention, first sidewalls are formed on both sides of the gate structure in the first region, and second sidewalls are formed on both sides of the gate structure in the second region. The widths of the first side wall and the second side wall are different, and the widths of the first negative covering area under the first side wall and the second negative covering area under the second side wall are different. In a FinFET with a negative cover region, different widths of the negative cover region lead to different effective channel widths of the subsequently formed FinFET, which changes the electric field distribution in the channel region and affects the FinFET. threshold voltage. The embodiment of the present invention utilizes the influence of the width of the negative covering region on the threshold voltage of the FinFET, and controls the width of the sidewalls formed in the first region and the second region during the formation of the FinFET. The widths of the first negative cover region and the second negative cover region are controlled to obtain fin field effect transistors with different threshold voltages, and the process is simple and the cost is low.

进一步的,本发明实施例的鳍式场效应晶体管的形成方法中,所述第一区域用于形成输入/输出晶体管,由于输入/输出晶体管通常需要较高的阈值电压和击穿电压,因此,对所述输入/输出晶体管的漏区端的第一负遮盖区进行离子注入,形成反型掺杂区。所述反型掺杂区的掺杂类型与所述输入/输出晶体管的源区和漏区掺杂类型相反,在所述反型掺杂区和漏区之间形成势垒,进一步提高了所述输入/输出晶体管的击穿电压和阈值电压。Further, in the method for forming a fin field effect transistor according to the embodiment of the present invention, the first region is used to form an input/output transistor. Since the input/output transistor usually requires a relatively high threshold voltage and breakdown voltage, therefore, Ion implantation is performed on the first negative covering region at the drain region end of the input/output transistor to form an inversion doped region. The doping type of the inversion doping region is opposite to the doping type of the source region and the drain region of the input/output transistor, and a potential barrier is formed between the inversion doping region and the drain region, further improving the breakdown and threshold voltages of the input/output transistors described above.

本发明虽然已以较佳实施例公开如上,但其并不是用来限定本发明,任何本领域技术人员在不脱离本发明的精神和范围内,都可以利用上述揭示的方法和技术对本发明技术方案做出可能的变动和修改,因此,凡是未脱离本发明技术方案的内容,依据本发明的技术实质对以上实施例所作的任何简单修改、等同变化及修饰,均属于本发明技术方案的保护范围。Although the present invention has been disclosed as above with preferred embodiments, it is not intended to limit the present invention, and any person skilled in the art can utilize the methods and techniques disclosed above to analyze the technical aspects of the present invention without departing from the spirit and scope of the present invention. Therefore, any simple modifications, equivalent changes and modifications made to the above embodiments according to the technical essence of the present invention, which do not depart from the content of the technical solution of the present invention, all belong to the protection of the technical solution of the present invention. scope.

Claims (19)

  1. A kind of 1. forming method of fin formula field effect transistor, it is characterised in that including:
    Semiconductor substrate is provided, the Semiconductor substrate has first area and second area, the first area and the secondth area There is raised fin, the grid structure on the fin, the top of fin described in the grid structure covering part in domain Portion and side wall;
    Form the first side wall in the grid structure both sides of the first area, the part fin of first side wall covering forms the One negative covering area;
    The second side wall is formed in the grid structure both sides of the second area, the width of second side wall is less than first side The width of wall, the part fin of the second side wall covering form the second negative covering area;
    Ion implanting is carried out to the fin of the first area and the grid structure both sides of second area, forms source region and drain region;
    Wherein, the fin formula field effect transistor that the first area is formed as input/output transistors, first side wall Material is high dielectric constant material, the doping concentration of the channel region in the described first negative fin for covering area and first area and is mixed Miscellany type is identical.
  2. 2. the forming method of fin formula field effect transistor as claimed in claim 1, it is characterised in that the second negative covering area Width be less than described first it is negative cover area width.
  3. 3. the forming method of fin formula field effect transistor as claimed in claim 2, it is characterised in that the first negative covering area Width range be 300 angstroms~500 angstroms.
  4. 4. the forming method of fin formula field effect transistor as claimed in claim 2, it is characterised in that the second negative covering area Width range be 10 angstroms~50 angstroms.
  5. 5. the forming method of fin formula field effect transistor as claimed in claim 4, it is characterised in that the first negative covering area Doping concentration it is identical with the doping concentration of the input/output transistors channel region.
  6. 6. the forming method of fin formula field effect transistor as claimed in claim 4, it is characterised in that also include to described defeated Enter/the first negative area that covers at the drain region end of output transistor carries out ion implanting, form transoid doped region.
  7. 7. the forming method of fin formula field effect transistor as claimed in claim 6, it is characterised in that the transoid doped region Doping type is opposite with the source region and drain region doping type of the input/output transistors.
  8. 8. the forming method of fin formula field effect transistor as claimed in claim 7, it is characterised in that the transoid doped region Width range is 1 angstrom~300 angstroms.
  9. 9. the forming method of fin formula field effect transistor as claimed in claim 1, it is characterised in that the second area is formed Fin formula field effect transistor as core logic transistor.
  10. 10. the forming method of fin formula field effect transistor as claimed in claim 9, it is characterised in that the second negative covering The doping concentration in area is identical with the doping concentration of the core logic transistor channel region.
  11. 11. the forming method of fin formula field effect transistor as claimed in claim 1, it is characterised in that second side wall Material is high dielectric constant material.
  12. 12. the forming method of the fin formula field effect transistor as described in claim 1 or 11, it is characterised in that the high dielectric Constant material is HfO2、Al2O3、ZrO2, one or more in HfSiO, HfSiON, HfTaO and HfZrO.
  13. 13. the forming method of fin formula field effect transistor as claimed in claim 1, it is characterised in that also include to described the The fin of one region and the grid structure both sides of second area carries out pre-amorphous ion implanting.
  14. 14. the forming method of fin formula field effect transistor as claimed in claim 13, it is characterised in that it is described it is pre-amorphous from The injection ion of son injection is Si, C, Ge, Xe or Ar.
  15. A kind of 15. fin formula field effect transistor, it is characterised in that including:
    Semiconductor substrate, the Semiconductor substrate have a first area and second area, in the first area and second area Fin with projection;
    Grid structure on the fin, the top of fin and side wall described in the grid structure covering part;
    The first side wall positioned at the grid structure both sides of the first area, the part fin of first side wall covering form the One negative covering area;
    The second side wall positioned at the grid structure both sides of the second area, the width of second side wall are less than first side The width of wall, the part fin of the second side wall covering form the second negative covering area;
    Source region and drain region in the fin of the first area and the grid structure both sides of second area;
    Wherein, the fin formula field effect transistor that the first area is formed as input/output transistors, first side wall Material is high dielectric constant material, the doping concentration of the channel region in the described first negative fin for covering area and first area and is mixed Miscellany type is identical.
  16. 16. fin formula field effect transistor as claimed in claim 15, it is characterised in that the width in the second negative covering area is small In the described first negative width for covering area.
  17. 17. fin formula field effect transistor as claimed in claim 15, it is characterised in that the first area is input/output Transistor area, the second area are core logic transistor region.
  18. 18. fin formula field effect transistor as claimed in claim 17, it is characterised in that also include being located at the input/output The drain region end of transistor first it is negative cover area in transoid doped region, the doping type of the transoid doped region with it is described defeated Enter/source region of output transistor and drain region doping type be on the contrary, the width range of the transoid doped region is 1 angstrom~300 angstroms.
  19. 19. fin formula field effect transistor as claimed in claim 15, it is characterised in that the material of second side wall is Gao Jie Permittivity material.
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