CN104241371A - Nanowire transistor - Google Patents
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- 239000002070 nanowire Substances 0.000 title claims abstract description 41
- 229910000577 Silicon-germanium Inorganic materials 0.000 claims abstract description 42
- 239000000758 substrate Substances 0.000 claims abstract description 24
- 229910021420 polycrystalline silicon Inorganic materials 0.000 claims abstract description 11
- 229920005591 polysilicon Polymers 0.000 claims abstract description 11
- 239000000463 material Substances 0.000 claims abstract description 10
- 239000000126 substance Substances 0.000 claims description 21
- 239000013078 crystal Substances 0.000 claims description 17
- 101100207343 Antirrhinum majus 1e20 gene Proteins 0.000 claims description 4
- 230000003071 parasitic effect Effects 0.000 abstract description 8
- 239000004065 semiconductor Substances 0.000 abstract description 6
- 230000005669 field effect Effects 0.000 abstract description 5
- 230000000694 effects Effects 0.000 description 9
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 6
- 229910052710 silicon Inorganic materials 0.000 description 6
- 239000010703 silicon Substances 0.000 description 6
- 238000004519 manufacturing process Methods 0.000 description 5
- 239000002019 doping agent Substances 0.000 description 4
- 239000012535 impurity Substances 0.000 description 4
- 230000009467 reduction Effects 0.000 description 4
- 239000000969 carrier Substances 0.000 description 3
- 238000009792 diffusion process Methods 0.000 description 3
- 238000000206 photolithography Methods 0.000 description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 229910052732 germanium Inorganic materials 0.000 description 2
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 2
- 150000002500 ions Chemical class 0.000 description 2
- 230000000873 masking effect Effects 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- LEVVHYCKPQWKOP-UHFFFAOYSA-N [Si].[Ge] Chemical compound [Si].[Ge] LEVVHYCKPQWKOP-UHFFFAOYSA-N 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000002708 enhancing effect Effects 0.000 description 1
- 238000002955 isolation Methods 0.000 description 1
- 238000002360 preparation method Methods 0.000 description 1
- 238000012827 research and development Methods 0.000 description 1
- 235000012239 silicon dioxide Nutrition 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
- 238000005549 size reduction Methods 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
- 238000000844 transformation Methods 0.000 description 1
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/60—Insulated-gate field-effect transistors [IGFET]
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/10—Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
- H10D62/117—Shapes of semiconductor bodies
- H10D62/118—Nanostructure semiconductor bodies
- H10D62/119—Nanowire, nanosheet or nanotube semiconductor bodies
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- H—ELECTRICITY
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- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/10—Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
- H10D62/13—Semiconductor regions connected to electrodes carrying current to be rectified, amplified or switched, e.g. source or drain regions
- H10D62/149—Source or drain regions of field-effect devices
- H10D62/151—Source or drain regions of field-effect devices of IGFETs
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/10—Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
- H10D62/17—Semiconductor regions connected to electrodes not carrying current to be rectified, amplified or switched, e.g. channel regions
- H10D62/213—Channel regions of field-effect devices
- H10D62/221—Channel regions of field-effect devices of FETs
- H10D62/235—Channel regions of field-effect devices of FETs of IGFETs
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- Insulated Gate Type Field-Effect Transistor (AREA)
Abstract
一种纳米线晶体管,涉及半导体场效应晶体管技术领域,其中,晶体管为圆柱形,所述晶体管具有一SiGe材质的圆柱形衬底,该圆柱形衬底位于中心轴方向上外露的两端分别作为纳米线晶体管的源区和漏区,所述源极和漏极之间形成有沟道区;一圆筒状的栅氧化层将源区和漏区之间的衬底表面进行包覆,且该栅氧化层的外侧被一多晶硅栅所包覆;其中,所述源区、漏区的Ge含量和所述沟道区的Ge含量不同。采用压应变SiGe作为纳米线晶体管的材料,这样就提高了纳米线晶体管的空穴迁移率以及降低寄生电阻。
A nanowire transistor, which relates to the technical field of semiconductor field effect transistors, wherein the transistor is cylindrical, and the transistor has a cylindrical substrate made of SiGe material, and the two ends of the cylindrical substrate located in the direction of the central axis are respectively used as A source region and a drain region of the nanowire transistor, a channel region is formed between the source and the drain; a cylindrical gate oxide layer covers the substrate surface between the source region and the drain region, and The outer side of the gate oxide layer is covered by a polysilicon gate; wherein, the Ge content of the source region and the drain region is different from the Ge content of the channel region. Using compressive strain SiGe as the material of the nanowire transistor improves the hole mobility of the nanowire transistor and reduces the parasitic resistance.
Description
技术领域technical field
本发明涉及半导体场效应晶体管技术领域,尤其涉及一种纳米线晶体管。The invention relates to the technical field of semiconductor field effect transistors, in particular to a nanowire transistor.
背景技术Background technique
在摩尔定律的指导下,集成电路半导体器件的尺寸越来越小,但是不能无限缩小,在缩小到一定程度将达到它的物理极限,严重的短沟道效应和栅极泄漏电流将会出现。这对摩尔定律的有效性将是一个挑战。但是人们积极寻找着替代用缩短器件尺寸来提高性能的方法,人们把技术上探索的焦点放到了使用高K材料和探索新型器件结构上,特别是后者,新型的器件结构将是未来半导体器件研究和发展的方向和趋势。硅纳米线晶体管是一种新型器件结构,它是集成电路发展路线图22纳米结束节点下最优希望的竞争者之一。目前国内外初步报道的硅纳米线结构晶体管拥有有益的亚阈值特性、载流子迁移率以及关态特性,能够很好的抑制短沟道效应。较之传统的体硅平面器件,一维准弹道输运的纳米线MOSFET表现出很强的缩小尺寸优势,纳米线晶体管对实现半导体路线图的既定目标将表现出极大的潜力。因为扩大栅包围沟道的面积,从而提高了控制沟道反型电子的能力,减小了MOS器件的短沟道效应,同时避免了缩小器件尺寸中所需要做的栅氧化层厚度的减小,从而也减小了栅极的泄漏电流。Under the guidance of Moore's Law, the size of integrated circuit semiconductor devices is getting smaller and smaller, but it cannot be reduced infinitely. It will reach its physical limit when it is reduced to a certain extent, and serious short-channel effects and gate leakage currents will appear. This will be a challenge to the validity of Moore's Law. However, people are actively looking for alternative ways to shorten the device size to improve performance. People put the focus of technical exploration on the use of high-K materials and the exploration of new device structures, especially the latter. The new device structure will be the future of semiconductor devices. Research and development directions and trends. The silicon nanowire transistor is a novel device structure that is one of the best hopeful contenders at the 22nm end node of the integrated circuit development roadmap. At present, the silicon nanowire structure transistors initially reported at home and abroad have beneficial subthreshold characteristics, carrier mobility and off-state characteristics, which can well suppress the short channel effect. Compared with the traditional bulk silicon planar devices, the one-dimensional quasi-ballistic transport nanowire MOSFET shows a strong size reduction advantage, and the nanowire transistor will show great potential for realizing the established goal of the semiconductor roadmap. Because the area of the gate surrounding the channel is enlarged, the ability to control the inversion electrons of the channel is improved, the short channel effect of the MOS device is reduced, and the reduction of the thickness of the gate oxide layer required to reduce the size of the device is avoided. , thereby reducing the gate leakage current.
当MOSFET特征尺寸进入纳米尺度后,载流子迁移率的降低成为限制器件性能的主要因素之一。When the characteristic size of MOSFET enters the nanometer scale, the reduction of carrier mobility becomes one of the main factors limiting the performance of the device.
通过在沟道方向施加应力,或者采用不同的衬底晶向,可以在不改变器件集合尺寸的情况下,显著地增强MOSFET的性能。By applying stress in the direction of the channel, or by employing different substrate orientations, the performance of MOSFETs can be significantly enhanced without changing the size of the device assembly.
对于短沟围栅型纳米线晶体管而言,根据文献“A UnifiedCarrier-Transport Model for the Nonsocial Surrounding-GateMOSFET Comprising Quantum–Mechanical Effects”的报道,其电子迁移率是120cm2/V·s,仍然远低于一般长沟平面MOSFET的1300cm2/V·s的电子迁移率。同样的条件下,电子的迁移率接近空穴迁移率的3倍,故短沟围栅型纳米线晶体管和一般长沟平面MOSFET的空穴迁移率分别为40cm2/V·s和433cm2/V·s,前者只是后者的1/10。故此类围栅型纳米线晶体管亟待解决迁移率过小的问题。For the short trench surround gate type nanowire transistor, according to the report in the literature "A UnifiedCarrier-Transport Model for the Nonsocial Surrounding-GateMOSFET Comprising Quantum–Mechanical Effects", its electron mobility is 120cm 2 /V·s, which is still far lower Compared with the 1300cm2/V·s electron mobility of the general long trench planar MOSFET. Under the same conditions, the mobility of electrons is close to three times the mobility of holes, so the hole mobility of short-groove surrounding gate nanowire transistors and general long-groove planar MOSFETs are 40cm 2 /V·s and 433cm 2 / V·s, the former is only 1/10 of the latter. Therefore, the problem of too small mobility needs to be solved urgently for this kind of gate-enclosed nanowire transistor.
中国专利(CN102082096A)介绍了一种Ge或SiGe纳米场效应晶体管的制备方法,首先在沉底上的隔离层上形成多晶硅栅;然后形成高K材料的栅介质层,再在栅介质层上淀积SiGe薄膜,对SiGe薄膜进行源漏掺杂后光刻定义出源漏区图形,并各向异性干法刻蚀SiGe薄膜,在多晶硅栅两侧形成SiGe侧墙,同时在栅长方向上SiGe侧墙的两头分别形成源区和漏区,最后对SiGe侧墙进行氧化,去掉表面形成的氧化层,得到Ge纳米线或高Ge含量的SiGe纳米线。Chinese patent (CN102082096A) has introduced a kind of preparation method of Ge or SiGe nanometer field effect transistor, first forms polysilicon gate on the isolation layer on sinking the bottom; The SiGe film is deposited, the source and drain of the SiGe film are doped, and the source and drain region pattern is defined by photolithography, and the SiGe film is anisotropically dry etched to form SiGe sidewalls on both sides of the polysilicon gate. A source region and a drain region are formed at both ends of the sidewall, and finally the SiGe sidewall is oxidized to remove the oxide layer formed on the surface to obtain Ge nanowires or SiGe nanowires with high Ge content.
中国专利(CN102822971A)记载了一种基于纳米级沟道的场效应晶体管中嵌入硅锗源极和漏极应力源的技术,在一方面中,一种制造FET的方法包括以下步骤,提供掺杂的衬底,在所述掺杂的衬底上具有电介质,在所述电介质上设置至少一个硅纳米线。掩蔽所述纳米线的一个或多个部分二使所述纳米线的其他部分暴露,在所述纳米线的暴露的部分上生长外延锗,使所述外延锗与所述纳米线中的Si相互扩散而形成嵌入在所述纳米线中的SiGe区域,所述SiGe区域在所述纳米线中引入压缩应变,所述掺杂的衬底用作所述FET的栅极,所述纳米线的掩蔽部分用作所述FET的沟道,且嵌入的SiGe区域用作所述FET的源极和漏极区域。Chinese patent (CN102822971A) describes a technique for embedding silicon germanium source and drain stressors in field effect transistors based on nanoscale channels. In one aspect, a method of manufacturing FETs includes the following steps, providing doping A substrate having a dielectric on the doped substrate, on which at least one silicon nanowire is disposed. masking one or more parts of the nanowires and exposing other parts of the nanowires, growing epitaxial germanium on the exposed parts of the nanowires, making the epitaxial germanium and Si in the nanowires interact Diffusion to form SiGe regions embedded in the nanowires, the SiGe regions introduce compressive strain in the nanowires, the doped substrate serves as the gate of the FET, the masking of the nanowires A portion serves as the channel of the FET, and the embedded SiGe region serves as the source and drain regions of the FET.
上述两个专利均未记载有关异质结SiGe与<100>晶向作为沟道的晶向结合形成的纳米线晶体管,提高无结晶体管的载流子迁移率和驱动电流的技术特征。The above two patents do not record the technical characteristics of the nanowire transistor formed by combining the heterojunction SiGe with the <100> crystal orientation as the crystal orientation of the channel, and improving the carrier mobility and driving current of the junctionless transistor.
发明内容Contents of the invention
鉴于上述问题,本发明提供一种纳米线晶体管。In view of the above problems, the present invention provides a nanowire transistor.
一种纳米线晶体管,其中,所述晶体管具有一SiGe材质的圆柱形衬底,该圆柱形衬底位于中心轴方向上外露的两端分别作为纳米线晶体管的源区和漏区,所述源极和漏极之间形成有沟道区;A nanowire transistor, wherein the transistor has a cylindrical substrate of SiGe material, and the two ends of the cylindrical substrate located in the direction of the central axis are respectively used as a source region and a drain region of the nanowire transistor, and the source A channel region is formed between the electrode and the drain;
一圆筒状的栅氧化层将源区和漏区之间的衬底表面进行包覆,且该栅氧化层的外侧被一多晶硅栅所包覆;A cylindrical gate oxide layer covers the substrate surface between the source region and the drain region, and the outer side of the gate oxide layer is covered by a polysilicon gate;
其中,所述源区、漏区的Ge含量和所述沟道区的Ge含量不同。Wherein, the Ge content of the source region and the drain region is different from the Ge content of the channel region.
上述的晶体管,其中,所述沟道区沿所述源区指向漏区的方向上的晶向为<100>。In the above-mentioned transistor, wherein, the crystal orientation of the channel region along the direction from the source region to the drain region is <100>.
上述的晶体管,其中,所述源区和漏区中Ge的化学摩尔比均小于所述沟道区中Ge的化学摩尔比。In the above transistor, the chemical molar ratio of Ge in the source region and the drain region is smaller than the chemical molar ratio of Ge in the channel region.
上述的晶体管,其中,所述源区和漏区中Ge的化学摩尔比相同。In the above transistor, the chemical molar ratio of Ge in the source region and the drain region is the same.
上述的晶体管,其中,选用BF2对所述衬底的两端进行掺杂形成源区和漏区,掺杂浓度为1e20/cm3。In the above transistor, BF 2 is selected to dope both ends of the substrate to form a source region and a drain region, and the doping concentration is 1e20/cm 3 .
上述的晶体管,其中,所述源区和漏区中Ge的化学摩尔比为1%-100%。The above transistor, wherein the chemical molar ratio of Ge in the source region and the drain region is 1%-100%.
上述的晶体管,其中,所述沟道区中Ge的化学摩尔比为1%-100%。The above transistor, wherein the chemical molar ratio of Ge in the channel region is 1%-100%.
上述的晶体管,其中,所述源极和漏极为P型,且所述沟道区为N型。In the above transistor, the source and drain are P-type, and the channel region is N-type.
上述的晶体管,其中,所述多晶硅栅为圆筒状。In the above-mentioned transistor, the polysilicon gate is cylindrical.
综上所述,本发明公开的纳米线晶体管,通过采用Ge含量不同的SiGe作为源漏区和沟道区的材料,从而增大了载流子的迁移率(由于SiGe的晶格常数比Si大),且由于源漏区和沟道区的Ge含量不同,从而使得沟道区的禁带宽度以及晶格常数均与源漏区不同,造成空穴速度增加,并导致有横向的压应力以进一步增强了空穴迁移率,且本发明使用<100>作为晶体管沟道晶向,从而进一步提高了纳米线晶体管的空穴迁移率,降低了纳米线晶体管寄生电阻。In summary, the nanowire transistor disclosed by the present invention increases the mobility of carriers by using SiGe with different Ge contents as the source and drain regions and the channel region (because the lattice constant of SiGe is higher than that of Si Large), and because the Ge content of the source and drain regions and the channel region are different, the band gap and lattice constant of the channel region are different from those of the source and drain regions, resulting in an increase in hole velocity and resulting in lateral compressive stress The hole mobility is further enhanced, and the present invention uses <100> as the crystal orientation of the transistor channel, thereby further improving the hole mobility of the nanowire transistor and reducing the parasitic resistance of the nanowire transistor.
附图说明Description of drawings
参考所附附图,以更加充分的描述本发明的实施例。然而,所附附图仅用于说明和阐述,并不构成对本发明范围的限制。Embodiments of the present invention are more fully described with reference to the accompanying drawings. However, the accompanying drawings are for illustration and illustration only, and do not limit the scope of the present invention.
图1是本发明晶体管的结构示意图;Fig. 1 is the structural representation of transistor of the present invention;
图2是本发明晶体管源漏端和沟道结构示意图;Fig. 2 is a schematic diagram of the source, drain and channel structure of the transistor of the present invention;
图3是本发明沟道和源漏端的电子能带示意图。Fig. 3 is a schematic diagram of the electronic energy bands of the channel and source and drain terminals of the present invention.
具体实施方式Detailed ways
下面结合附图和具体的实施例对本发明作进一步的说明,但是不作为本发明的限定。The present invention will be further described below in conjunction with the accompanying drawings and specific embodiments, but not as a limitation of the present invention.
本发明提供一种纳米线晶体管,可应用于半导体场效应晶体管技术领域,当使用该晶体管,因为采用SiGe为材料的纳米线晶体管,提高了纳米线晶体管的载流子迁移率和驱动电流。The invention provides a nanowire transistor, which can be applied to the technical field of semiconductor field effect transistors. When the transistor is used, the carrier mobility and driving current of the nanowire transistor are improved because SiGe is used as the material of the nanowire transistor.
本发明的核心思想是采用SiGe作为纳米晶体管的材料,Ge的加入能够提高无结晶体管的电子和空穴的迁移率,且器件的源漏端与沟道中的Ge含量有差别,这种源漏异质结的结构能够提高空穴的发射速度和迁移率,同时,使用能够提高空穴迁移率的<100>晶向作为沟道的晶向,与异质结SiGe增强空穴迁移率的效果共同作用,解决纳米线晶体管迁移率过小的问题。The core idea of the present invention is to adopt SiGe as the material of the nano-transistor, the addition of Ge can improve the mobility of electrons and holes of the junction-free transistor, and the source-drain end of the device is different from the Ge content in the channel. The structure of the heterojunction can increase the emission speed and mobility of the holes. At the same time, the <100> crystal orientation that can improve the hole mobility is used as the crystal orientation of the channel, and the effect of enhancing the hole mobility with the heterojunction SiGe Work together to solve the problem of too small mobility of nanowire transistors.
13nm直径异质SiGe纳米线PMOSFET与平面同质SiGe沟道器件(宽度1μm)的电学特性的比较,前者是后者的4.5倍,同时13nm直径异质SiGe纳米线PMOSFET与平面同质SiGe沟道器件(宽度1μm)的gm和Vg关系的比较,在饱和区和线性区都显示出前者比后者增加4.5倍;应力Si0.8Ge0.2的p-MOSFET如果采用<100>晶向作为沟道晶向,比<110>沟道晶向的应力Si0.8Ge0.2的p-MOSFET有着25%的空穴迁移率提高及20%的寄生电阻的降低。而后者已经比Sip-MOSFET有着更优越的迁移率和阈值电压滚落(Threshold Voltage Roll-Off)效应特性。Comparison of the electrical characteristics of 13nm diameter heterogeneous SiGe nanowire PMOSFET and planar homogeneous SiGe channel device (width 1μm), the former is 4.5 times that of the latter, while 13nm diameter heterogeneous SiGe nanowire PMOSFET and planar homogeneous SiGe channel The comparison of the relationship between gm and Vg of the device (width 1μm) shows that the former is 4.5 times larger than the latter in both the saturation region and the linear region; if the p-MOSFET with stress Si0.8Ge0.2 adopts the <100> crystal orientation as the channel Crystal orientation, p-MOSFET with stress Si0.8Ge0.2 compared with <110> channel crystal orientation has 25% higher hole mobility and 20% lower parasitic resistance. The latter has superior mobility and threshold voltage roll-off (Threshold Voltage Roll-Off) effect characteristics than Sip-MOSFET.
故可以预见,如果SiGe异质结的无结晶体管采用<100>作为沟道晶向,则可以显著提高空穴迁移率以及降低寄生电阻。Therefore, it can be predicted that if the SiGe heterojunction junctionless transistor adopts <100> as the crystal orientation of the channel, the hole mobility can be significantly improved and the parasitic resistance can be reduced.
实施例1:Example 1:
如图1所示为该晶体管的结构,该晶体管具有一SiGe材质的圆柱形衬底,一圆筒状的氧化层2包覆在该衬底外侧,并将衬底两端暴露形成源区4和漏区3,在源区4和漏区3之间形成该晶体管的沟道区5,一圆筒状多晶硅栅1包覆于栅氧化层2外侧,对源区4和漏区3进行了BF2施主离子的掺杂,掺杂浓度为1e20/cm3。工艺制造时在晶圆上挑选<100>晶向作为沟道区的方向,并沿轴心线由源区4指向漏区3(图中所示箭头方向),关于纳米线晶体管的制造工艺,只要在光刻的时候选择好沟道晶向为<100>即可。本发明的器件能带结构如图3所示,该晶体管源区4和漏区3中Ge的化学摩尔比相同,且源区4和漏区3中Ge的化学摩尔比小于沟道区5中Ge的化学摩尔比,其中,源区4和漏区3的SiGe中的Ge的含量是30%,中间沟道区5的SiGe中Ge的含量是70%,这样的源区4、漏区3与沟道区5的异质结的结构带来了中间沟道区5价带的上移,价带的上移能使空穴的发射速度和迁移率得到提升。如图1和图2所示,从图中可以看到该晶体管的结构是圆柱形,左右两端是SiGe且Ge含量为30%的P型掺杂源漏区,中间部分是SiGe且Ge含量为70%的N型掺杂的硅。The structure of the transistor is shown in Figure 1, the transistor has a cylindrical substrate of SiGe material, a cylindrical oxide layer 2 is coated on the outside of the substrate, and both ends of the substrate are exposed to form a source region 4 and the drain region 3, the channel region 5 of the transistor is formed between the source region 4 and the drain region 3, a cylindrical polysilicon gate 1 is covered on the outside of the gate oxide layer 2, and the source region 4 and the drain region 3 are formed Doping of BF 2 donor ions, the doping concentration is 1e20/cm 3 . During the manufacturing process, select the <100> crystal orientation on the wafer as the direction of the channel region, and point from the source region 4 to the drain region 3 along the axis (the direction of the arrow shown in the figure). Regarding the manufacturing process of the nanowire transistor, As long as the crystal orientation of the channel is selected to be <100> during photolithography. The energy band structure of the device of the present invention is shown in Figure 3, the chemical molar ratio of Ge in the source region 4 and the drain region 3 of the transistor is the same, and the chemical molar ratio of Ge in the source region 4 and the drain region 3 is smaller than that in the channel region 5 The chemical molar ratio of Ge, wherein, the content of Ge in the SiGe of source region 4 and drain region 3 is 30%, the content of Ge in the SiGe of intermediate channel region 5 is 70%, such source region 4, drain region 3 The structure of the heterojunction with the channel region 5 brings about an upward shift of the valence band of the intermediate channel region 5 , and the upward shift of the valence band can improve the hole emission velocity and mobility. As shown in Figure 1 and Figure 2, it can be seen from the figure that the structure of the transistor is cylindrical, the left and right ends are P-type doped source and drain regions with SiGe and Ge content of 30%, and the middle part is SiGe and Ge content 70% N-type doped silicon.
如图1所示,圆筒状的围栅结构可以增强栅控能力,有效抑制短沟效应,为晶体管尺寸缩小作出贡献。SiGe作为构成源漏和沟道的材料,由于其晶格常数比Si大,故可以提高载流子的迁移率。同时,<100>晶向的沟道能够抑制漏端P型掺杂杂质的扩散,增加了漏端掺杂杂质的浓度,减小了寄生电阻。As shown in Figure 1, the cylindrical surrounding gate structure can enhance the gate control capability, effectively suppress the short-channel effect, and contribute to the reduction of the transistor size. SiGe, as a material for source, drain and channel, can increase the mobility of carriers because its lattice constant is larger than that of Si. At the same time, the <100> oriented channel can suppress the diffusion of P-type dopant impurities at the drain end, increase the concentration of dopant impurities at the drain end, and reduce parasitic resistance.
实施例2:Example 2:
如图1所示为该晶体管的结构,该晶体管具有一SiGe材质的圆柱形衬底,一圆筒状上氧化层2包覆在该衬底外侧,并将衬底两端暴露形成源区4和漏区3,在源区4和漏区3之间形成该晶体管的沟道区5,一圆筒状多晶硅栅1包覆于栅氧化层2外侧,对源区4和漏区3进行了BF2离子的掺杂,掺杂浓度为1e20/cm3。工艺制造时在晶圆上挑选<100>晶向作为沟道区的方向,并沿轴心线由源区4指向漏区3,(图中所示箭头方向),关于纳米线晶体管的制造工艺,只要在光刻的时候选择好沟道晶向为<100>即可。本发明的器件能带结构如图3所示,该晶体管源区4和漏区3中Ge的化学摩尔比相同,且源区4和漏区3中Ge的化学摩尔比小于沟道区5中Ge的化学摩尔比,其中,源区4和漏区3的SiGe中的Ge的含量是20%,中间沟道区5SiGe中Ge的含量是80%,这样的源区4、漏区3与沟道区5的异质结的结构带来了中间沟道区价带的上移,价带的上移能使空穴的发射速度和迁移率得到提升。如图1和图2所示,从图中可以看到该晶体管的结构是圆柱形,左右两端是SiGe且Ge含量为20%的P型掺杂源漏区,中间部分是SiGe且Ge含量为80%的N型掺杂的硅。The structure of the transistor is shown in Figure 1, the transistor has a cylindrical substrate made of SiGe, a cylindrical upper oxide layer 2 is coated on the outside of the substrate, and both ends of the substrate are exposed to form a source region 4 and the drain region 3, the channel region 5 of the transistor is formed between the source region 4 and the drain region 3, a cylindrical polysilicon gate 1 is covered on the outside of the gate oxide layer 2, and the source region 4 and the drain region 3 are formed Doping of BF 2 ions, the doping concentration is 1e20/cm 3 . During the manufacturing process, select the <100> crystal orientation on the wafer as the direction of the channel region, and point from the source region 4 to the drain region 3 along the axis line (the direction of the arrow shown in the figure), regarding the manufacturing process of nanowire transistors , as long as the crystal orientation of the channel is selected to be <100> during photolithography. The energy band structure of the device of the present invention is shown in Figure 3, the chemical molar ratio of Ge in the source region 4 and the drain region 3 of the transistor is the same, and the chemical molar ratio of Ge in the source region 4 and the drain region 3 is smaller than that in the channel region 5 The chemical molar ratio of Ge, wherein, the content of Ge in the SiGe of source region 4 and drain region 3 is 20%, the content of Ge in the intermediate channel region 5 SiGe is 80%, such source region 4, drain region 3 and ditch The structure of the heterojunction in the channel region 5 brings about an upward shift of the valence band in the middle channel region, and the upward shift of the valence band can improve the hole emission velocity and mobility. As shown in Figure 1 and Figure 2, it can be seen from the figure that the structure of the transistor is cylindrical, and the left and right ends are P-type doped source and drain regions with SiGe and Ge content of 20%, and the middle part is SiGe and Ge content 80% N-type doped silicon.
如图1所示,圆筒状的围栅结构可以增强栅控能力,有效抑制短沟效应,为晶体管尺寸缩小作出贡献。SiGe作为构成源漏和沟道的材料,由于其晶格常数比Si大,故可以提高载流子的迁移率。同时,<100>方向的沟道能够抑制漏端P型掺杂杂质的扩散,增加了漏端掺杂杂质的浓度,减小了寄生电阻。As shown in Figure 1, the cylindrical surrounding gate structure can enhance the gate control capability, effectively suppress the short-channel effect, and contribute to the reduction of the transistor size. SiGe, as a material for source, drain and channel, can increase the mobility of carriers because its lattice constant is larger than that of Si. At the same time, the channel in the <100> direction can suppress the diffusion of P-type dopant impurities at the drain end, increase the concentration of dopant impurities at the drain end, and reduce parasitic resistance.
作为衬底的SiGe在不同区域,其Ge的含量也是有所不同的,源区和漏区中的Ge含量化学摩尔比在1%-100%,且源区和漏区中Ge的化学摩尔比是相同的,沟道区的Ge含量化学摩尔比在1%-100%,其中源区和漏区中Ge的化学摩尔比是小于沟道区中的Ge的化学摩尔比,这样的结构设计使得左右两边与中间沟道部分的异质结的结构带来中间沟道部分价带的上移,价带上移使空穴的发射速度和迁移率得到提升。SiGe as the substrate has different Ge content in different regions. The chemical molar ratio of the Ge content in the source region and the drain region is 1%-100%, and the chemical molar ratio of Ge in the source region and the drain region is are the same, the Ge content chemical molar ratio of the channel region is 1%-100%, wherein the chemical molar ratio of Ge in the source region and the drain region is less than the chemical molar ratio of Ge in the channel region, such a structural design makes The structure of the heterojunction between the left and right sides and the middle channel part brings up the valence band of the middle channel part, and the upward shift of the valence band improves the emission speed and mobility of holes.
为了得到更好效果的无结晶体管,该晶体管的多晶硅栅长为300-400nm(例如300nm、340nm、350nm和400nm);厚度为70-80nm(例如73nm、75nm、78nm和80nm);由此可见SiGe衬底中沟道区的长度与多晶硅栅的长度是相同的,作为栅氧化层的二氧化硅层厚度为5-10nm(例如5nm、7nm、8nm和10nm);该晶体管的源区、漏区和沟道区的直径为10-15nm(例如10nm、12nm、13nm和15nm)。In order to obtain a junction-free transistor with better effect, the polysilicon gate length of the transistor is 300-400nm (such as 300nm, 340nm, 350nm and 400nm); the thickness is 70-80nm (such as 73nm, 75nm, 78nm and 80nm); it can be seen that The length of the channel region in the SiGe substrate is the same as the length of the polysilicon gate, and the thickness of the silicon dioxide layer as the gate oxide layer is 5-10nm (such as 5nm, 7nm, 8nm and 10nm); the source region, drain of the transistor The regions and channel regions are 10-15 nm in diameter (eg 10 nm, 12 nm, 13 nm and 15 nm).
SiGe异质结结构应用到纳米线晶体管中,可以提高该晶体管空穴迁移率和驱动电流,SiGe衬底中沟道采用<100>晶向作为沟道晶向,则可以显著提高空穴迁移率以及降低寄生电阻,将两者的结合起来,能够大大的提高P型无结晶体管的空穴迁移率和驱动电流,并且减小了寄生电阻。The SiGe heterojunction structure applied to the nanowire transistor can improve the hole mobility and driving current of the transistor, and the <100> crystal orientation of the channel in the SiGe substrate can be used as the channel crystal orientation, which can significantly improve the hole mobility. As well as reducing the parasitic resistance, the combination of the two can greatly improve the hole mobility and driving current of the P-type junctionless transistor, and reduce the parasitic resistance.
通过说明和附图,给出了具体实施方式的特定结构的典型实施例,基于本发明精神,还可作其他的转换。尽管上述发明提出了现有的较佳实施例,然而,这些内容并不作为局限。Through the description and drawings, typical examples of specific structures of specific implementations are given, and other transformations can also be made based on the spirit of the present invention. While the above invention presents preferred embodiments, such disclosure is not intended to be limiting.
对于本领域的技术人员而言,阅读上述说明后,各种变化和修正无疑将显而易见。因此,所附的权利要求书应看作是涵盖本发明的真实意图和范围的全部变化和修正。在权利要求书范围内任何和所有等价的范围与内容,都应认为仍属本发明的意图和范围内。Various changes and modifications will no doubt become apparent to those skilled in the art upon reading the foregoing description. Therefore, the appended claims should be considered to cover all changes and modifications within the true intent and scope of the invention. Any and all equivalent scope and content within the scope of the claims should still be deemed to be within the intent and scope of the present invention.
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Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20050062033A1 (en) * | 2003-08-08 | 2005-03-24 | Canon Kabushiki Kaisha | Structure and method for production of the same |
CN101986423A (en) * | 2009-07-28 | 2011-03-16 | 台湾积体电路制造股份有限公司 | Method for forming silicon-germanium stressors with high germanium concentration and integrated circuit transistor structure |
CN102034863A (en) * | 2009-09-28 | 2011-04-27 | 中芯国际集成电路制造(上海)有限公司 | Semiconductor device, transistor having gate of around cylindrical channel and manufacturing method |
CN102148250A (en) * | 2011-01-07 | 2011-08-10 | 清华大学 | High-speed low-noise semiconductor device structure and method for forming same |
US20130075817A1 (en) * | 2011-09-23 | 2013-03-28 | International Business Machines Corporation | Junctionless transistor |
-
2014
- 2014-07-31 CN CN201410375234.4A patent/CN104241371A/en active Pending
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20050062033A1 (en) * | 2003-08-08 | 2005-03-24 | Canon Kabushiki Kaisha | Structure and method for production of the same |
CN101986423A (en) * | 2009-07-28 | 2011-03-16 | 台湾积体电路制造股份有限公司 | Method for forming silicon-germanium stressors with high germanium concentration and integrated circuit transistor structure |
CN102034863A (en) * | 2009-09-28 | 2011-04-27 | 中芯国际集成电路制造(上海)有限公司 | Semiconductor device, transistor having gate of around cylindrical channel and manufacturing method |
CN102148250A (en) * | 2011-01-07 | 2011-08-10 | 清华大学 | High-speed low-noise semiconductor device structure and method for forming same |
US20130075817A1 (en) * | 2011-09-23 | 2013-03-28 | International Business Machines Corporation | Junctionless transistor |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN111162074A (en) * | 2018-11-07 | 2020-05-15 | 中芯国际集成电路制造(上海)有限公司 | Semiconductor structure and forming method thereof |
CN111162074B (en) * | 2018-11-07 | 2022-07-26 | 中芯国际集成电路制造(上海)有限公司 | Semiconductor structure and method of forming the same |
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