CN106876457A - A kind of enhanced MIS structure AlGaN/GaN HFETs of groove grid - Google Patents
A kind of enhanced MIS structure AlGaN/GaN HFETs of groove grid Download PDFInfo
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- 229910002704 AlGaN Inorganic materials 0.000 title claims abstract description 54
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- 229910052751 metal Inorganic materials 0.000 claims description 3
- 239000002184 metal Substances 0.000 claims description 3
- 229910010271 silicon carbide Inorganic materials 0.000 claims description 3
- 229910052581 Si3N4 Inorganic materials 0.000 claims description 2
- 238000000151 deposition Methods 0.000 claims description 2
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- 239000010980 sapphire Substances 0.000 claims description 2
- 229910052710 silicon Inorganic materials 0.000 claims description 2
- 239000010703 silicon Substances 0.000 claims description 2
- HQVNEWCFYHHQES-UHFFFAOYSA-N silicon nitride Chemical compound N12[Si]34N5[Si]62N3[Si]51N64 HQVNEWCFYHHQES-UHFFFAOYSA-N 0.000 claims description 2
- 238000005036 potential barrier Methods 0.000 claims 6
- 239000004411 aluminium Substances 0.000 claims 1
- 229910052782 aluminium Inorganic materials 0.000 claims 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims 1
- 238000005229 chemical vapour deposition Methods 0.000 claims 1
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- 229910003465 moissanite Inorganic materials 0.000 description 1
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- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 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]
- H10D30/40—FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels
- H10D30/47—FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels having 2D charge carrier gas channels, e.g. nanoribbon FETs or high electron mobility transistors [HEMT]
- H10D30/471—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT]
- H10D30/475—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having wider bandgap layer formed on top of lower bandgap active layer, e.g. undoped barrier HEMTs such as i-AlGaN/GaN HEMTs
- H10D30/4755—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having wider bandgap layer formed on top of lower bandgap active layer, e.g. undoped barrier HEMTs such as i-AlGaN/GaN HEMTs having wide bandgap charge-carrier supplying layers, e.g. modulation doped HEMTs such as n-AlGaAs/GaAs HEMTs
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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
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- H10D62/102—Constructional design considerations for preventing surface leakage or controlling electric field concentration
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Abstract
本发明公开了一种具有部分本征GaN帽层的新型槽栅增强型MIS结构AlGaN/GaN异质结场效应晶体管。这种新型晶体管结构是在晶体管栅极边缘引入本征GaN帽层,该本征GaN帽层会降低该区域导电沟道的二维电子气浓度,实现电场调制效应。通过产生新的电场峰,降低了栅边缘的高电场,使晶体管表面的电场分布更加均匀,与传统槽栅增强型MIS结构相比,新型结构的击穿电压和可靠性也就有了明显的提高与改善。
The invention discloses a novel trench gate enhanced MIS structure AlGaN/GaN heterojunction field effect transistor with part of the intrinsic GaN cap layer. This new type of transistor structure introduces an intrinsic GaN cap layer at the edge of the gate of the transistor. The intrinsic GaN cap layer will reduce the two-dimensional electron gas concentration of the conductive channel in this region and realize the electric field modulation effect. By generating a new electric field peak, the high electric field at the edge of the gate is reduced, and the electric field distribution on the surface of the transistor is more uniform. Compared with the traditional trench-gate enhanced MIS structure, the breakdown voltage and reliability of the new structure are significantly improved. Improve and improve.
Description
技术领域technical field
本发明涉及半导体器件技术领域,特别是涉及一种槽栅增强型MIS结构AlGaN/GaN异质结场效应晶体管。The invention relates to the technical field of semiconductor devices, in particular to a trench gate enhanced MIS structure AlGaN/GaN heterojunction field effect transistor.
背景技术Background technique
由于以Si和GaAs为代表的第一代和第二代半导体材料的局限性,第三代宽禁带半导体材料因为其优异的性能得到了飞速发展。GaN材料作为第三代半导体材料的核心之一,相比Si,GaAs和SiC特殊之处在于其所具有的极化效应。利用这种特殊性,人们研制了AlGaN/GaN高电子迁移率晶体管,AlGaN/GaN HEMTs是以AlGaN/GaN异质结材料为基础而制造的GaN基微电子器件。AlGaN/GaN异质结通过自发极化和压电极化效应在异质结界面处形成高密度二维电子气(two dimensional electron gas,2DEG),这种二维电子气具有很高的迁移率,从而使AlGaN/GaN HEMTs具有很低的导通电阻。与传统的场效应晶体管(FET)器件相比,AlGaN/GaN HEMTs具有高跨导、高饱和电流以及高截止频率等优良特性。而且,实验证明,GaN基HEMTs在1000K的高温下仍然保持着良好的直流特性,从而为高温环境应用提供了可靠的保证。Due to the limitations of the first-generation and second-generation semiconductor materials represented by Si and GaAs, the third-generation wide-bandgap semiconductor materials have been developed rapidly because of their excellent performance. As one of the cores of the third-generation semiconductor materials, GaN material is special in its polarization effect compared with Si, GaAs and SiC. Taking advantage of this particularity, people have developed AlGaN/GaN high electron mobility transistors, and AlGaN/GaN HEMTs are GaN-based microelectronic devices based on AlGaN/GaN heterojunction materials. AlGaN/GaN heterojunction forms a high-density two-dimensional electron gas (2DEG) at the heterojunction interface through spontaneous polarization and piezoelectric polarization effects, and this two-dimensional electron gas has high mobility. , so that AlGaN/GaN HEMTs have very low on-resistance. Compared with traditional field-effect transistor (FET) devices, AlGaN/GaN HEMTs have excellent characteristics such as high transconductance, high saturation current, and high cut-off frequency. Moreover, experiments have proved that GaN-based HEMTs still maintain good DC characteristics at a high temperature of 1000K, thus providing a reliable guarantee for high-temperature environment applications.
由于AlGaN/GaN异质结得天独厚的优势,AlGaN/GaN异质结材料的生长和AlGaN/GaN HEMTs器件的研制始终占据着GaN电子器件研究的主要地位。然而十几年来针对GaN基电子器件研究的大部分工作集中在耗尽型AlGaN/GaN HEMTs器件上,这是由于AlGaN/GaN异质结中强极化电荷的存在,使得制造GaN基的增强型器件变得十分困难,因此高性能增强型AlGaN/GaN HEMTs的研究具有非常重要的意义。Due to the unique advantages of AlGaN/GaN heterojunction, the growth of AlGaN/GaN heterojunction materials and the development of AlGaN/GaN HEMTs devices have always occupied the main position in the research of GaN electronic devices. However, most of the research on GaN-based electronic devices in the past decade has focused on depletion-mode AlGaN/GaN HEMTs devices. This is due to the existence of strong polarized charges in the AlGaN/GaN heterojunction, making GaN-based enhancement mode Devices become very difficult, so the study of high-performance enhancement mode AlGaN/GaN HEMTs is of great significance.
对于GaN基增强型器件,工艺上较为容易实现的是槽栅MIS结构。Tohru Oka等人利用槽栅技术制得了阈值电压高达5.2V的增强型器件。该器件结构自下而上包括:Si衬底,800nm厚的Al0.05Ga0.95N缓冲层,40nm厚的GaN沟道层,1nm的AlN插入层,34nm厚的Al0.25Ga0.75N势垒层,1nm的GaN帽层。该技术通过将栅下的势垒层刻蚀一定深度,使得栅下势垒层变薄甚至消失,从而使栅下2DEG浓度降低甚至为零,而源漏区的载流子浓度保持较大值不变,同时在栅电极与AlGaN势垒层之间淀积厚度为20nm的SiN绝缘层,形成MIS结构。这样既可实现器件的增强型特性,又可保证一定的电流密度。具体参见文献:For GaN-based enhancement-mode devices, the trench-gate MIS structure is easier to realize in terms of technology. Tohru Oka et al. have fabricated an enhancement-mode device with a threshold voltage as high as 5.2V using trench gate technology. The device structure includes from bottom to top: Si substrate, 800nm thick Al 0.05 Ga 0.95 N buffer layer, 40nm thick GaN channel layer, 1nm AlN insertion layer, 34nm thick Al 0.25 Ga 0.75 N barrier layer, 1nm GaN cap layer. This technology makes the barrier layer under the gate thinner or even disappears by etching the barrier layer under the gate to a certain depth, so that the 2DEG concentration under the gate is reduced or even zero, while the carrier concentration in the source and drain regions remains relatively large. At the same time, a SiN insulating layer with a thickness of 20nm is deposited between the gate electrode and the AlGaN barrier layer to form a MIS structure. In this way, the enhanced characteristics of the device can be realized, and a certain current density can be guaranteed. For details, see the literature:
Tohru Oka,Tomohiro Nozawa,“AlGaN/GaN Recessed MIS-Gate HFET WithHigh-Threshold-Voltage Normally-Off Operation for Power ElectronicsApplications”,Electron Device Letters,Vol.29,No.7,July 2008.Tohru Oka, Tomohiro Nozawa, "AlGaN/GaN Recessed MIS-Gate HFET With High-Threshold-Voltage Normally-Off Operation for Power Electronics Applications", Electron Device Letters, Vol.29, No.7, July 2008.
然而,在槽栅增强型MIS结构AlGaN/GaN HEMTs的栅边缘往往存在着高峰电场,其会给器件带来以下不利影响:1、会引起电子–空穴对离化,当达到GaN材料的临界击穿电场这一雪崩条件时,器件在栅电极边缘击穿。2、即使没有达到GaN材料的临界击穿电场,高电场效应仍然会使栅电极电子场致发射遂穿进入表面钝化层,这些隧穿的电子会中和AlGaN层的表面极化正电荷,而这些表面极化正电荷,直接关系到异质结界面处2DEG的浓度大小,部分表面正电荷被中和会降低高密度的2DEG浓度,从而使AlGaN/GaN HEMTs输出电流明显减小,这就是电流崩塌效应。3、使电子–空穴对的离化几率增加,电离后的空穴在纵向电场作用下进入沟道中和2DEG,也会使2DEG浓度减小,进一步减小输出电流;而且电离后的电子进入AlGaN极化层会给器件阈值电压带来不利影响,使得器件可靠性降低。However, there is often a peak electric field at the gate edge of AlGaN/GaN HEMTs with trench gate enhanced MIS structure, which will bring the following adverse effects on the device: 1. It will cause electron-hole pair ionization. When the critical In the avalanche condition of the breakdown electric field, the device breaks down at the edge of the gate electrode. 2. Even if the critical breakdown electric field of the GaN material is not reached, the high electric field effect will still cause the field emission of the gate electrode electrons to tunnel into the surface passivation layer, and these tunneling electrons will neutralize the surface polarized positive charges of the AlGaN layer, These surface polarized positive charges are directly related to the concentration of 2DEG at the heterojunction interface. The neutralization of part of the surface positive charges will reduce the concentration of high-density 2DEG, thereby significantly reducing the output current of AlGaN/GaN HEMTs, which is current collapse effect. 3. The ionization probability of electron-hole pairs is increased, and the ionized holes enter the channel and 2DEG under the action of the longitudinal electric field, which will also reduce the concentration of 2DEG and further reduce the output current; and the ionized electrons enter The AlGaN polarization layer will adversely affect the threshold voltage of the device, reducing the reliability of the device.
因此,设计一种新型槽栅增强型MIS结构AlGaN/GaN HEMTs器件,通过引入新的电场峰,从而降低器件栅边缘高峰电场是一种优化其性能、提高其击穿电压与可靠性的重要手段。Therefore, designing a new trench gate enhanced MIS structure AlGaN/GaN HEMTs device, by introducing a new electric field peak, thereby reducing the peak electric field at the edge of the device gate is an important means to optimize its performance and improve its breakdown voltage and reliability. .
发明内容Contents of the invention
为了解决现有技术中由于在槽栅增强型MIS结构AlGaN/GaN异质结场效应晶体管的栅边缘存在高峰电场而引起的器件雪崩击穿、电流崩塌效应,阈值电压和输出电流减小,可靠性降低等一系列问题,本发明提供一种新型槽栅增强型MIS结构AlGaN/GaN异质结场效应晶体管。In order to solve the device avalanche breakdown and current collapse effect caused by the peak electric field at the gate edge of the AlGaN/GaN heterojunction field effect transistor with a trench-gate enhanced MIS structure in the prior art, the threshold voltage and output current are reduced, and the reliability To solve a series of problems such as reduced performance, the present invention provides a novel trench gate enhanced MIS structure AlGaN/GaN heterojunction field effect transistor.
解决方案如下:The solution is as follows:
一种槽栅增强型MIS结构AlGaN/GaN异质结场效应晶体管,包括:A trench gate enhanced MIS structure AlGaN/GaN heterojunction field effect transistor, comprising:
半绝缘衬底;semi-insulating substrate;
位于所述半绝缘衬底上异质外延生长的AlN成核层;A heteroepitaxially grown AlN nucleation layer located on the semi-insulating substrate;
位于所述AlN成核层上外延生长的GaN缓冲层;a GaN buffer layer epitaxially grown on the AlN nucleation layer;
位于所述GaN缓冲层上外延生长的AlGaN势垒层;an AlGaN barrier layer epitaxially grown on the GaN buffer layer;
分列于所述AlGaN层上的源极、栅凹槽以及漏极;a source electrode, a gate groove, and a drain electrode arranged on the AlGaN layer;
位于所述源极与漏极之间的栅凹槽;a gate groove between the source and the drain;
位于所述栅凹槽上的绝缘介质层;an insulating dielectric layer on the gate groove;
位于所述绝缘介质层上的栅极(即栅极通过绝缘介质层与所述AlGaN势垒层相连);A gate located on the insulating dielectric layer (that is, the gate is connected to the AlGaN barrier layer through an insulating dielectric layer);
其特殊之处在于:Its special features are:
在AlGaN势垒层上还外延生长有与栅极边缘邻接的本征GaN帽层,所述本征GaN帽层部分覆盖或者完全覆盖栅极和漏极之间的区域。An intrinsic GaN cap layer adjacent to the edge of the gate is epitaxially grown on the AlGaN barrier layer, and the intrinsic GaN cap layer partially or completely covers the region between the gate and the drain.
基于上述解决方案,本发明还进一步作如下优化限定和改进:Based on the above solution, the present invention further makes the following optimization limitations and improvements:
上述本征GaN帽层是通过在AlGaN势垒层表面外延生长本征GaN层,然后刻蚀形成的。The above-mentioned intrinsic GaN cap layer is formed by epitaxially growing an intrinsic GaN layer on the surface of the AlGaN barrier layer, and then etching.
本征GaN帽层位于栅极和漏极之间,可以部分覆盖,也可以完全覆盖。这是因为本征GaN帽层对沟道2DEG浓度调制作用的效果与其长度有关,可以灵活选择刻蚀区域。The intrinsic GaN cap layer is located between the gate and drain and can be partially covered or completely covered. This is because the effect of the intrinsic GaN cap layer on channel 2DEG concentration modulation is related to its length, and the etching area can be flexibly selected.
上述本征GaN帽层长度以不超过栅漏间距的百分之二十为佳。Preferably, the above-mentioned intrinsic GaN cap layer length should not exceed 20% of the gate-to-drain distance.
上述栅凹槽是通过对本征GaN帽层和AlGaN势垒层局部刻蚀形成的。The gate groove is formed by partially etching the intrinsic GaN cap layer and the AlGaN barrier layer.
上述绝缘介质层是通过等离子增强化学气相淀积介质层形成的,材料为氮化硅或氧化铝。The above insulating dielectric layer is formed by plasma enhanced chemical vapor deposition dielectric layer, and the material is silicon nitride or aluminum oxide.
上述栅极是通过在绝缘介质层上淀积金属形成的。The gate is formed by depositing metal on the insulating dielectric layer.
上述源极和所述漏极均通过欧姆接触与所述AlGaN势垒层相连。Both the source and the drain are connected to the AlGaN barrier layer through ohmic contacts.
上述外延生长的GaN缓冲层具有n型电阻特性或半绝缘特性。The epitaxially grown GaN buffer layer has n-type resistance characteristics or semi-insulation characteristics.
上述半绝缘衬底为能够与所述AlN成核层异质外延的半绝缘材料,优选硅或碳化硅;或者,半绝缘衬底替换为蓝宝石。The aforementioned semi-insulating substrate is a semi-insulating material capable of heteroepitaxy with the AlN nucleation layer, preferably silicon or silicon carbide; or, the semi-insulating substrate is replaced by sapphire.
本发明的上述技术方案的有益效果如下:The beneficial effects of above-mentioned technical scheme of the present invention are as follows:
在晶体管栅极边缘引入本征GaN帽层,该本征GaN帽层会降低该区域导电沟道2DEG的浓度,实现电场调制效应。通过产生新的电场峰,降低了栅边缘的高电场,使晶体管表面的电场分布更加均匀。随着本征GaN帽层长度的增加,电场调制效应增强,使得新电场峰值提高,栅边缘高峰电场下降量增加;而且由于表面电场分布更加均匀,使得器件在达到GaN材料临界击穿电场时所需要施加的漏端电压更大,击穿电压提高,器件可靠性相比于传统槽栅增强型结构,也有了明显的改善。An intrinsic GaN cap layer is introduced at the edge of the gate of the transistor, and the intrinsic GaN cap layer will reduce the concentration of the conductive channel 2DEG in this region to realize the electric field modulation effect. By generating new electric field peaks, the high electric field at the gate edge is reduced, making the electric field distribution on the surface of the transistor more uniform. With the increase of the intrinsic GaN cap layer length, the electric field modulation effect is enhanced, which makes the peak value of the new electric field increase, and the drop of the peak electric field at the gate edge increases; and because the surface electric field distribution is more uniform, the device reaches the critical breakdown electric field of the GaN material. The drain terminal voltage that needs to be applied is larger, the breakdown voltage is increased, and the reliability of the device is also significantly improved compared with the traditional trench-gate enhanced structure.
同时,该结构在工艺上制作简单,不会对AlGaN势垒层造成额外的不利影响,保证了器件在工艺制造过程中的稳定性与可靠性。At the same time, the structure is easy to manufacture in terms of process, does not cause additional adverse effects on the AlGaN barrier layer, and ensures the stability and reliability of the device during the process of manufacturing.
附图说明Description of drawings
图1为本发明具有部分本征GaN帽层的新型槽栅增强型MIS结构AlGaN/GaN异质结场效应晶体管的示意图。FIG. 1 is a schematic diagram of a novel trench gate enhanced MIS structure AlGaN/GaN heterojunction field effect transistor with a part of intrinsic GaN cap layer according to the present invention.
图2为传统槽栅增强型MIS结构AlGaN/GaN异质结场效应晶体管结构与本发明具有部分本征GaN帽层的槽栅增强型MIS结构AlGaN/GaN异质结场效应晶体管结构击穿时沟道电场分布与电压值对比图。Figure 2 shows the breakdown of the AlGaN/GaN heterojunction field effect transistor structure of the traditional trench gate enhanced MIS structure and the trench gate enhanced MIS structure AlGaN/GaN heterojunction field effect transistor structure of the present invention with part of the intrinsic GaN cap layer Comparison diagram of channel electric field distribution and voltage value.
具体实施方式detailed description
为使本发明要解决的技术问题、技术方案和优点更加清楚,下面结合附图及具体实施例进行详细描述。In order to make the technical problems, technical solutions and advantages to be solved by the present invention clearer, a detailed description will be given below in conjunction with the accompanying drawings and specific embodiments.
该实施例是一种具有部分本征GaN帽层的新型槽栅增强型MIS结构AlGaN/GaN异质结场效应晶体管。其结构如图1所示,主要包括:半绝缘衬底0;位于半绝缘衬底上异质外延生长的AlN成核层1;位于AlN成核层上外延生长的GaN缓冲层2;位于GaN缓冲层上外延生长的AlGaN势垒层3;位于所述AlGaN势垒层上的栅凹槽4、漏极5以及源极6;位于栅凹槽上的绝缘介质层7;位于绝缘介质层上的栅极8;位于所述AlGaN势垒层上,与栅极边缘邻接的本征GaN帽层9。This embodiment is a novel trench gate enhanced MIS structure AlGaN/GaN heterojunction field effect transistor with part of the intrinsic GaN cap layer. Its structure is shown in Figure 1, mainly including: a semi-insulating substrate 0; a heteroepitaxially grown AlN nucleation layer 1 on the semi-insulating substrate; a GaN buffer layer 2 epitaxially grown on the AlN nucleation layer; AlGaN barrier layer 3 epitaxially grown on the buffer layer; gate groove 4, drain 5 and source 6 located on the AlGaN barrier layer; insulating dielectric layer 7 located on the gate groove; located on the insulating dielectric layer The gate 8; the intrinsic GaN cap layer 9 located on the AlGaN barrier layer and adjacent to the edge of the gate.
槽栅MIS结构是常用的实现增强型的方法。通过将栅下的势垒层刻蚀一定深度,使得栅下势垒层变薄甚至消失,从而使栅下2DEG浓度降低甚至为零,进而实现增强型特性。器件的阈值电压取决于刻蚀深度。The trench gate MIS structure is a commonly used method to realize the enhancement mode. By etching the barrier layer under the gate to a certain depth, the barrier layer under the gate becomes thinner or even disappears, so that the concentration of 2DEG under the gate is reduced or even zero, thereby realizing enhanced characteristics. The threshold voltage of the device depends on the etch depth.
引入本征GaN帽层,使得GaN/AlGaN界面处感应出负极化电荷,这层负电荷降低了沟道2DEG浓度,产生新的电场峰,使得栅极边缘高电场降低,表面电场分布趋于均匀。随着本征GaN帽层长度的增加,电场调制效应增强,使得新电场峰值提高,栅边缘高峰电场下降量增加;而且由于表面电场分布更加均匀,使得器件在达到GaN材料临界击穿电场时所需要施加的漏端电压更大,击穿电压提高,器件可靠性相比于传统槽栅增强型MIS结构,也有了明显的改善。The introduction of an intrinsic GaN cap layer induces negative polarization charges at the GaN/AlGaN interface. This layer of negative charges reduces the channel 2DEG concentration and generates a new electric field peak, which reduces the high electric field at the edge of the gate and makes the surface electric field distribution tend to be uniform. . With the increase of the intrinsic GaN cap layer length, the electric field modulation effect is enhanced, which makes the peak value of the new electric field increase, and the drop of the peak electric field at the gate edge increases; and because the surface electric field distribution is more uniform, the device reaches the critical breakdown electric field of the GaN material. The drain terminal voltage that needs to be applied is larger, the breakdown voltage is improved, and the reliability of the device is also significantly improved compared with the traditional trench-gate enhanced MIS structure.
如图2所示,由于传统结构在栅极边缘存在高峰电场,其击穿电压只有46V,而新型结构能够有效降低栅极边缘高峰电场,并在本征GaN帽层靠近漏极一侧产生新的电场峰,击穿电压提高至78V,其中栅极靠近漏极边缘位置为X=3.0μm,本征GaN帽层长度为2.0μm,厚度为100nm。As shown in Figure 2, the breakdown voltage of the traditional structure is only 46V due to the peak electric field at the edge of the gate, while the new structure can effectively reduce the peak electric field at the edge of the gate and generate a new GaN cap near the drain. The electric field peak of , the breakdown voltage increases to 78V, where X=3.0μm is the position of the gate near the edge of the drain, the length of the intrinsic GaN cap layer is 2.0μm, and the thickness is 100nm.
其具体实现方法以感应耦合等离子体刻蚀(ICP)为例:在完成本征GaN帽层AlGaN/GaN异质结场效应晶体管的刻蚀与金属电极淀积工艺后,利用ICP在靠近栅极边缘刻蚀出本征GaN帽层。刻蚀区域可以灵活选择。The specific implementation method takes inductively coupled plasma etching (ICP) as an example: after completing the etching and metal electrode deposition process of the intrinsic GaN cap layer AlGaN/GaN heterojunction field effect transistor, use ICP to close the gate The intrinsic GaN cap layer is etched out at the edge. The etching area can be flexibly selected.
这里,本征GaN帽层的厚度,只与该帽层所对应的沟道具体要求有关,在需要减少沟道载流子浓度的地方,就应存在本征GaN帽层,帽层的厚度越大,载流子浓度减小的幅度越大,具体沟道载流子浓度的大小,主要是根据需要着重遏制的不利影响来确定,比如:Here, the thickness of the intrinsic GaN cap layer is only related to the specific requirements of the channel corresponding to the cap layer. Where the channel carrier concentration needs to be reduced, there should be an intrinsic GaN cap layer. The thicker the cap layer is, The larger the carrier concentration is, the greater the reduction of the carrier concentration is. The specific channel carrier concentration is mainly determined according to the adverse effects that need to be curbed, such as:
若需要一个LDD的浓度分布以提高击穿电压遏制热载流子注入效应,则可以在由栅到漏依次刻蚀不同深度,产生阶梯型本征GaN帽层。If a concentration distribution of LDD is required to increase the breakdown voltage to curb the hot carrier injection effect, different depths can be sequentially etched from the gate to the drain to produce a stepped intrinsic GaN cap layer.
若需要充分改善器件的击穿特性,则可以在栅漏间完全覆盖本征GaN帽层。If it is necessary to fully improve the breakdown characteristics of the device, the intrinsic GaN cap layer can be completely covered between the gate and the drain.
若需要降低器件漏极靠近栅极边缘产生的高峰电场,则可以在漏极边缘根据具体要求刻蚀产生本征GaN帽层,等等。If it is necessary to reduce the peak electric field generated by the drain of the device near the edge of the gate, an intrinsic GaN cap layer can be etched on the edge of the drain according to specific requirements, and so on.
为获得“具有调制沟道载流子浓度的本征GaN帽层”,并不限于上述实施例采用的本征GaN帽层ICP刻蚀技术,也可以采用其他方式实现,最终应能达到相同的技术效果。In order to obtain "intrinsic GaN cap layer with modulated channel carrier concentration", it is not limited to the intrinsic GaN cap layer ICP etching technology used in the above-mentioned embodiments, and other methods can also be used to achieve the same result. technical effect.
获得本征GaN帽层的刻蚀技术与方法有很多,反应离子刻蚀(RIE)、电子回旋共振等离子体刻蚀(ECR)等能够刻蚀本征GaN帽层的技术都可以应用于此方案。There are many etching techniques and methods to obtain the intrinsic GaN cap layer, such as reactive ion etching (RIE), electron cyclotron resonance plasma etching (ECR), etc., which can etch the intrinsic GaN cap layer, can be applied to this scheme.
以上所述的是本发明的优选实施方式,对于本技术领域的普通人员来说,基于本发明的原理,还可以进行若干改进和完善,这些改进和完善的产物也应视为本发明的保护范围。What has been described above is a preferred embodiment of the present invention. For those of ordinary skill in the art, based on the principle of the present invention, some improvements and perfections can also be carried out. The products of these improvements and perfections should also be regarded as the protection of the present invention. scope.
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Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN115148797A (en) * | 2021-06-04 | 2022-10-04 | 山东大学 | A kind of open gate AlGaN/GaN heterojunction field effect transistor with auxiliary gate structure and its application |
| CN120500077A (en) * | 2025-07-18 | 2025-08-15 | 深圳平湖实验室 | Semiconductor device, preparation method thereof and chip |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN1554121A (en) * | 2001-07-12 | 2004-12-08 | ���﹫˾ | AlGaN/GaN High Electron Mobility Transistor with Gate Contact Region on Gallium Nitride-Based Cap Region and Method of Fabrication |
| CN103022121A (en) * | 2011-09-27 | 2013-04-03 | 富士通株式会社 | Semiconductor device and method of manufacturing the same |
| CN104377241A (en) * | 2014-09-30 | 2015-02-25 | 苏州捷芯威半导体有限公司 | Power semiconductor device and manufacturing method thereof |
| US20150270379A1 (en) * | 2014-03-19 | 2015-09-24 | Kabushiki Kaisha Toshiba | Semiconductor device |
-
2017
- 2017-01-11 CN CN201710020055.2A patent/CN106876457B/en active Active
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN1554121A (en) * | 2001-07-12 | 2004-12-08 | ���﹫˾ | AlGaN/GaN High Electron Mobility Transistor with Gate Contact Region on Gallium Nitride-Based Cap Region and Method of Fabrication |
| CN103022121A (en) * | 2011-09-27 | 2013-04-03 | 富士通株式会社 | Semiconductor device and method of manufacturing the same |
| US20150270379A1 (en) * | 2014-03-19 | 2015-09-24 | Kabushiki Kaisha Toshiba | Semiconductor device |
| CN104377241A (en) * | 2014-09-30 | 2015-02-25 | 苏州捷芯威半导体有限公司 | Power semiconductor device and manufacturing method thereof |
Non-Patent Citations (1)
| Title |
|---|
| TOHRU OKA 等: "AlGaN/GaN recessed MIS-Gate HFET With High-Threshold-Voltage Normally-Off Operation for power electronics applications", 《ELECTRON DEVICE LETTERS》 * |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN115148797A (en) * | 2021-06-04 | 2022-10-04 | 山东大学 | A kind of open gate AlGaN/GaN heterojunction field effect transistor with auxiliary gate structure and its application |
| CN120500077A (en) * | 2025-07-18 | 2025-08-15 | 深圳平湖实验室 | Semiconductor device, preparation method thereof and chip |
| CN120500077B (en) * | 2025-07-18 | 2025-10-03 | 深圳平湖实验室 | Semiconductor device and manufacturing method thereof, and chip |
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