CN105097911A - HEMT device with junction type semiconductor layer - Google Patents
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- 239000004065 semiconductor Substances 0.000 title claims abstract description 53
- 230000004888 barrier function Effects 0.000 claims abstract description 44
- 229910052751 metal Inorganic materials 0.000 claims abstract description 24
- 239000002184 metal Substances 0.000 claims abstract description 24
- 238000002955 isolation Methods 0.000 claims abstract description 16
- 239000004047 hole gas Substances 0.000 claims abstract description 9
- 230000000903 blocking effect Effects 0.000 claims abstract description 8
- 239000000463 material Substances 0.000 claims description 16
- 238000002161 passivation Methods 0.000 claims description 16
- 229910002601 GaN Inorganic materials 0.000 claims description 14
- 229910002704 AlGaN Inorganic materials 0.000 claims description 9
- 239000000758 substrate Substances 0.000 claims description 9
- 229910010271 silicon carbide Inorganic materials 0.000 claims description 5
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 claims description 4
- 229910052593 corundum Inorganic materials 0.000 claims description 4
- 238000005468 ion implantation Methods 0.000 claims description 4
- 230000005533 two-dimensional electron gas Effects 0.000 claims description 4
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- 229910052594 sapphire Inorganic materials 0.000 claims description 3
- 239000010980 sapphire Substances 0.000 claims description 3
- 229910052710 silicon Inorganic materials 0.000 claims description 3
- 239000010703 silicon Substances 0.000 claims description 3
- 229910017083 AlN Inorganic materials 0.000 claims 3
- 229910003465 moissanite Inorganic materials 0.000 claims 2
- 230000005684 electric field Effects 0.000 abstract description 18
- 230000015556 catabolic process Effects 0.000 abstract description 12
- 230000000694 effects Effects 0.000 abstract description 5
- 230000000779 depleting effect Effects 0.000 abstract description 2
- 239000010410 layer Substances 0.000 description 91
- JMASRVWKEDWRBT-UHFFFAOYSA-N Gallium nitride Chemical compound [Ga]#N JMASRVWKEDWRBT-UHFFFAOYSA-N 0.000 description 14
- PMHQVHHXPFUNSP-UHFFFAOYSA-M copper(1+);methylsulfanylmethane;bromide Chemical compound Br[Cu].CSC PMHQVHHXPFUNSP-UHFFFAOYSA-M 0.000 description 8
- 238000005530 etching Methods 0.000 description 8
- 238000010586 diagram Methods 0.000 description 4
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 description 4
- 239000000243 solution Substances 0.000 description 4
- 239000003989 dielectric material Substances 0.000 description 3
- 230000002028 premature Effects 0.000 description 3
- 229910004205 SiNX Inorganic materials 0.000 description 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 2
- 229910052737 gold Inorganic materials 0.000 description 2
- 229910001092 metal group alloy Inorganic materials 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- PIGFYZPCRLYGLF-UHFFFAOYSA-N Aluminum nitride Chemical compound [Al]#N PIGFYZPCRLYGLF-UHFFFAOYSA-N 0.000 description 1
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- 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]
- H10D30/473—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having confinement of carriers by multiple heterojunctions, e.g. quantum well HEMT
- H10D30/4732—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having confinement of carriers by multiple heterojunctions, e.g. quantum well HEMT using Group III-V semiconductor material
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Abstract
本发明属于半导体技术领域,具体的说涉及一种具有结型半导体层的HEMT器件。本发明的器件,主要为通过在栅漏之间的势垒层上表面生长一层结型半导体层,结型半导体层与势垒层形成二维空穴气(2DHG)。栅极金属与结型半导体层形成整流结构避免栅上加正压时造成栅极-2DHG-2DEG的泄漏电流,同时漏电极与结型半导体之间采用隔离层阻断2DHG;另一方面,栅漏之间的2DHG与2DEG形成极化超结,阻断状态时辅助耗尽漂移区,有效的改善了器件栅靠漏端的电场集中效应,同时,在P型掺杂区和N型掺杂区的接触部分,会引入一个新的电场尖峰,使得器件表面电场分布更加均匀,从而提高器件的关态击穿电压。本发明尤其适用于HEMT器件。
The invention belongs to the technical field of semiconductors, and in particular relates to a HEMT device with a junction semiconductor layer. The device of the present invention mainly grows a junction semiconductor layer on the upper surface of the barrier layer between the gate and drain, and the junction semiconductor layer and the barrier layer form two-dimensional hole gas (2DHG). The gate metal and the junction semiconductor layer form a rectification structure to avoid the gate-2DHG-2DEG leakage current when a positive voltage is applied to the gate. At the same time, an isolation layer is used between the drain electrode and the junction semiconductor to block 2DHG; on the other hand, the gate The 2DHG and 2DEG between the drains form a polarized superjunction, which assists in depleting the drift region in the blocking state, effectively improving the electric field concentration effect at the drain end of the device gate. At the same time, in the P-type doped region and the N-type doped region The contact part of the device will introduce a new electric field spike, which will make the electric field distribution on the surface of the device more uniform, thereby increasing the off-state breakdown voltage of the device. The invention is particularly applicable to HEMT devices.
Description
技术领域technical field
本发明属于半导体技术领域,具体的说涉及一种具有结型半导体层的HEMT(HighElectronMobilityTransistor,高电子迁移率晶体管)器件。The invention belongs to the technical field of semiconductors, and in particular relates to a HEMT (High Electron Mobility Transistor, High Electron Mobility Transistor) device with a junction semiconductor layer.
背景技术Background technique
宽禁带半导体氮化镓(GaN)具有高临界击穿电场(~3.3×106V/cm)、高电子迁移率(~2000cm2/V·s)等特性,且基于GaN材料的异质结高电子迁移率晶体管(HEMT)还具有高浓度(~1013cm-2)的二维电子气(2DEG)沟道,使得GaNHEMT器件具有反向阻断电压高、正向导通电阻低、工作频率高等特性,在大电流、低功耗、高压开关器件应用领域具有巨大的应用前景。The wide bandgap semiconductor gallium nitride (GaN) has the characteristics of high critical breakdown electric field (~3.3×106V/cm), high electron mobility (~2000cm2/V s), and the heterojunction based on GaN material has high electronic The mobility transistor (HEMT) also has a high-concentration (~1013cm-2) two-dimensional electron gas (2DEG) channel, which makes GaNHEMT devices have high reverse blocking voltage, low forward conduction resistance, and high operating frequency. The application field of high current, low power consumption and high voltage switching devices has great application prospects.
功率开关器件的关键是实现高击穿电压、低导通电阻和高可靠性。HEMT器件的击穿主要是由于栅肖特基结的泄漏电流和通过缓冲层的泄漏电流引起的。要提高器件耐压,纵向上需要增加缓冲层的厚度和质量,这主要由工艺技术水平决定;横向上需要漂移区长度增加,这不仅使器件(或电路)的芯片面积增加、成本增大,更为严重的是,器件的导通电阻增大,进而导致功耗急剧增加,且器件开关速度也随之降低。The key to power switching devices is to achieve high breakdown voltage, low on-resistance and high reliability. The breakdown of HEMT devices is mainly caused by the leakage current of the gate Schottky junction and the leakage current through the buffer layer. To improve the withstand voltage of the device, the thickness and quality of the buffer layer need to be increased in the vertical direction, which is mainly determined by the technological level; the length of the drift region needs to be increased in the lateral direction, which not only increases the chip area and cost of the device (or circuit), but also increases the cost. More seriously, the on-resistance of the device increases, which in turn leads to a sharp increase in power consumption, and the switching speed of the device is also reduced.
为了充分利用GaN材料的高临界击穿电场等优异特性,提高器件耐压,业内研究者进行了许多研究。其中场板技术是一种用来改善器件耐压的常用终端技术,文献(J.Li,et.al.“HighbreakdownvoltageGaNHFETwithfieldplate”IEEEElectronLett.,vol.37,no.3,pp.196–197,February.2001.)采用了与栅短接的场板,如图1所示,场板的引入可以降低主结的曲率效应和电场尖峰,从而提高耐压。然而场板的引入会使器件寄生电容增大,影响器件的高频和开关特性文献。(AkiraNakajima,et.al.“GaN-BasedSuperHeterojunctionFieldEffectTransistorsUsingthePolarizationJunctionConcept”IEEEElectronDeviceLetters,vol.32,no.4,pp.542-544,2011)采用极化超结的思想,在漂移区部分的AlGaN势垒层上方生长一层顶层GaN,并在其界面形成二维空穴气(2DHG),2DHG与其下方的2DEG形成天然的“超结”,在阻断耐压时,辅助耗尽漂移区,优化器件横向电场,从而达到提高耐压的目的,如图2所示。但是顶层GaN与栅电极形成了空穴的欧姆接触,在正向导通时,栅压较大时会产生栅极泄漏电流,限制了栅压摆幅。In order to make full use of the excellent characteristics of GaN materials such as high critical breakdown electric field and improve device withstand voltage, researchers in the industry have conducted many studies. Among them, the field plate technology is a common terminal technology used to improve the withstand voltage of the device. The literature (J.Li, et.al. "Highbreakdownvoltage GaNHFET with fieldplate" IEEE Electron Lett., vol.37, no.3, pp.196-197, February. 2001.) A field plate shorted to the gate is used, as shown in Figure 1, the introduction of the field plate can reduce the curvature effect of the main junction and the electric field spike, thereby improving the withstand voltage. However, the introduction of the field plate will increase the parasitic capacitance of the device, which will affect the high frequency and switching characteristics of the device. (AkiraNakajima, et.al. "GaN-BasedSuperHeterojunctionFieldEffectTransistorsUsingthePolarizationJunctionConcept" IEEE ElectronDeviceLetters, vol.32, no.4, pp.542-544, 2011) Using the idea of polarized superjunction, a GaN on the top layer of the layer, and two-dimensional hole gas (2DHG) is formed at its interface. The 2DHG and the 2DEG below form a natural "superjunction". To achieve the purpose of improving the withstand voltage, as shown in Figure 2. However, the top-layer GaN forms an ohmic contact with the gate electrode, and when the gate is conducting forward, a gate leakage current will be generated when the gate voltage is high, which limits the gate voltage swing.
对于AlGaN/GaNHEMT器件而言,增强型(常关型)HEMT器件比耗尽型(常开型)HEMT器件具有更多的优势,其实现技术也是研究者们极其关注的问题。文献(W.Saito,et.al.,“Recessed-gatestructureapproachtowardnormallyoffhigh-voltageAlGaN/GaNHEMTforpowerelectronicsapplications,”IEEETrans.ElectronDevices,vol.53,no.2,pp.356-362,2006)报道了采用槽栅结构实现了一种准增强型高压AlGaN/GaNHEMT,如图3所示,凹栅刻蚀能够有效地耗尽栅极下方2DEG浓度,极大地提高阈值电压,但是凹栅刻蚀需要精确地控制刻蚀深度和降低等离子体处理引起的刻蚀损伤。For AlGaN/GaN HEMT devices, enhancement mode (normally off) HEMT devices have more advantages than depletion mode (normally on) HEMT devices, and its implementation technology is also a matter of great concern to researchers. Literature (W.Saito, et.al., "Recessed-gatestructure approachtoward normally off high-voltageAlGaN/GaNHEMTforpowerelectronicsapplications," IEEETrans.ElectronDevices, vol.53, no.2, pp.356-362, 2006) reported the use of a trench gate structure to achieve a Quasi-enhanced high-voltage AlGaN/GaN HEMT, as shown in Figure 3, the recessed gate etching can effectively deplete the 2DEG concentration under the gate and greatly increase the threshold voltage, but the recessed gate etching needs to precisely control the etching depth and reduce the Etch damage caused by plasma treatment.
发明内容Contents of the invention
本发明所要解决的,就是针对上述问题,提出一种具有结型半导体层的HEMT器件。What the present invention aims to solve is to propose a HEMT device with a junction semiconductor layer in view of the above problems.
为实现上述目的,本发明采用如下技术方案:To achieve the above object, the present invention adopts the following technical solutions:
一种具有结型半导体层的HEMT器件,包括衬底1、设置在衬底1上表面的缓冲层2和设置在缓冲层2上表面的势垒层3,所述缓冲层2和势垒层3的接触面形成具有二维电子气沟道的第一异质结;所述势垒层3上表面的两端分别具有源电极4和漏电极5,势垒层3上表面中部具有栅极结构;所述源电极4与栅极结构之间的势垒层3上表面具有介质钝化层10,所述漏电极5与栅极结构之间的势垒层3上表面具有结型半导体层8;所述结型半导体层8与势垒层3的接触面形成具有二维空穴气的第二异质结;其特征在于,所述结型半导体层8由P型掺杂区81和N型掺杂区82构成,所述P型掺杂区81与栅极结构连接,所述N型掺杂区82与漏电极5之间具有能阻断二维空穴气的隔断层11;所述栅极结构由绝缘栅介质7和金属栅电极6构成,所述绝缘栅介质7分别与介质钝化层10、势垒层3和P型掺杂区81连接,其横截面形状为U型结构,所述金属栅电极6位于绝缘栅介质7中,所述金属栅电极6沿器件横向方向延伸并覆盖在绝缘栅介质7的上表面;所述金属栅电极6还延伸至P型掺杂区81上表面并与结型半导体层8之间形成整流结构9。A HEMT device with a junction semiconductor layer, comprising a substrate 1, a buffer layer 2 arranged on the upper surface of the substrate 1 and a barrier layer 3 arranged on the upper surface of the buffer layer 2, the buffer layer 2 and the barrier layer The contact surface of 3 forms a first heterojunction with a two-dimensional electron gas channel; the two ends of the upper surface of the barrier layer 3 respectively have a source electrode 4 and a drain electrode 5, and the middle part of the upper surface of the barrier layer 3 has a gate structure; the upper surface of the barrier layer 3 between the source electrode 4 and the gate structure has a dielectric passivation layer 10, and the upper surface of the barrier layer 3 between the drain electrode 5 and the gate structure has a junction semiconductor layer 8; the contact surface of the junction semiconductor layer 8 and the barrier layer 3 forms a second heterojunction with two-dimensional hole gas; it is characterized in that the junction semiconductor layer 8 is composed of a P-type doped region 81 and An N-type doped region 82 is formed, the P-type doped region 81 is connected to the gate structure, and an isolation layer 11 capable of blocking two-dimensional hole gas is provided between the N-type doped region 82 and the drain electrode 5; The gate structure is composed of an insulating gate dielectric 7 and a metal gate electrode 6. The insulating gate dielectric 7 is respectively connected to the dielectric passivation layer 10, the barrier layer 3 and the P-type doped region 81, and its cross-sectional shape is U type structure, the metal gate electrode 6 is located in the insulating gate dielectric 7, the metal gate electrode 6 extends along the lateral direction of the device and covers the upper surface of the insulating gate dielectric 7; the metal gate electrode 6 also extends to the P-type doped A rectifying structure 9 is formed between the upper surface of the impurity region 81 and the junction semiconductor layer 8 .
本发明总的技术方案,通过在栅漏之间的势垒层上表面生长一层结型半导体层,结型半导体层与势垒层形成二维空穴气(2DHG)。栅极金属与结型半导体层形成整流结构避免栅上加正压时造成栅极-2DHG-2DEG的泄漏电流,同时漏电极与结型半导体之间采用隔离层阻断2DHG;另一方面,栅漏之间的2DHG与2DEG形成极化超结,阻断状态时辅助耗尽漂移区,有效的改善了器件栅靠漏端的电场集中效应,同时,在P型掺杂区和N型掺杂区的接触部分,会引入一个新的电场尖峰,使得器件表面电场分布更加均匀,从而提高器件的关态击穿电压。In the general technical solution of the present invention, a junction semiconductor layer is grown on the upper surface of the barrier layer between the gate and drain, and the junction semiconductor layer and the barrier layer form a two-dimensional hole gas (2DHG). The gate metal and the junction semiconductor layer form a rectification structure to avoid the gate-2DHG-2DEG leakage current when a positive voltage is applied to the gate. At the same time, an isolation layer is used between the drain electrode and the junction semiconductor to block 2DHG; on the other hand, the gate The 2DHG and 2DEG between the drains form a polarized superjunction, which assists in the depletion of the drift region in the blocking state, effectively improving the electric field concentration effect at the drain end of the device gate. At the same time, in the P-type doped region and the N-type doped region The contact part of the device will introduce a new electric field spike, which will make the electric field distribution on the surface of the device more uniform, thereby increasing the off-state breakdown voltage of the device.
进一步的,所述金属栅电极6与漏电极5之间的结型半导体层8的上表面具有第二介质钝化层13,所述漏电极5沿第二介质钝化层13上表面向金属栅电极6的方向延伸,形成漏场板电极12。Further, the upper surface of the junction semiconductor layer 8 between the metal gate electrode 6 and the drain electrode 5 has a second dielectric passivation layer 13, and the drain electrode 5 faces the metal along the upper surface of the second dielectric passivation layer 13. The direction of the gate electrode 6 is extended to form a drain field plate electrode 12 .
上述方案的目的在于,通过漏场板12的引入,可以有效的降低漏端的电场尖峰,避免了漏电发生提前击穿。The purpose of the above solution is to effectively reduce the electric field peak at the drain end through the introduction of the leakage field plate 12 and avoid premature breakdown of the leakage current.
进一步的,所述栅极结构为平面绝缘栅结构,所述绝缘栅介质7的下表面与势垒层3的上表面连接。Further, the gate structure is a planar insulating gate structure, and the lower surface of the insulating gate dielectric 7 is connected to the upper surface of the barrier layer 3 .
进一步的,所述栅极结构为凹槽绝缘栅结构,所述绝缘栅介质7的底部位于势垒层3中。Further, the gate structure is a recessed insulated gate structure, and the bottom of the insulated gate dielectric 7 is located in the barrier layer 3 .
进一步的,所述栅极结构为凹槽绝缘栅结构,所述绝缘栅介质7的下表面与缓冲层2的上表面连接。Further, the gate structure is a recessed insulated gate structure, and the lower surface of the insulating gate dielectric 7 is connected to the upper surface of the buffer layer 2 .
进一步的,其特征在于,所述整流结构9为金属栅电极6与P型掺杂区81接触形成肖特基势垒接触。Further, it is characterized in that, the rectifying structure 9 is that the metal gate electrode 6 contacts the P-type doped region 81 to form a Schottky barrier contact.
进一步的,所P型掺杂区81与栅极结构连接处的上表面掺杂有N型半导体形成PN结整流,所述整流结构9为金属栅电极6与PN结整流形成欧姆接触。Further, the upper surface of the connection between the P-type doped region 81 and the gate structure is doped with an N-type semiconductor to form a PN junction rectification, and the rectification structure 9 is an ohmic contact between the metal gate electrode 6 and the PN junction rectification.
进一步的,所述隔断层11为物理隔断层或离子注入隔断层。Further, the isolation layer 11 is a physical isolation layer or an ion implantation isolation layer.
上述方案中,物理隔断层为指将结型半导体层8与漏电极5之间的部分刻蚀掉,使结型半导体层8与漏电极5之间隔离;离职注入隔断层是指在结型半导体层8与漏电极5之间注入N型半导体形成重掺杂的N型隔离层。In the above scheme, the physical isolation layer refers to etching away the part between the junction semiconductor layer 8 and the drain electrode 5, so as to isolate the junction semiconductor layer 8 from the drain electrode 5; An N-type semiconductor is implanted between the semiconductor layer 8 and the drain electrode 5 to form a heavily doped N-type isolation layer.
进一步的,所述绝缘栅介质7采用的材料为Al2O3或其他单层或多层绝缘介质材料;所述结型半导体层8采用的材料为Si、SiC、GaN、AlN、AlGaN、InGaN、InAlN中的一种或几种的组合;所述缓冲层2及势垒层3采用材料为GaN、AlN、AlGaN、InGaN、InAlN中的一种或几种的组合;所述衬底1采用的材料为蓝宝石、硅、SiC、AlN或GaN中的一种或几种的组合。Further, the material used for the insulating gate dielectric 7 is Al2O3 or other single-layer or multi-layer insulating dielectric materials; the material used for the junction semiconductor layer 8 is Si, SiC, GaN, AlN, AlGaN, InGaN, InAlN One or a combination of several; the buffer layer 2 and the barrier layer 3 are made of one or a combination of GaN, AlN, AlGaN, InGaN, InAlN; the material used for the substrate 1 is One or a combination of sapphire, silicon, SiC, AlN or GaN.
本发明的有益效果为,有效的改善了器件栅靠漏端的电场集中效应,同时在P型掺杂区和N型掺杂区的接触部分,引入一个新的电场尖峰,使得器件表面电场分布更加均匀,从而提高器件的关态击穿电压。The beneficial effect of the present invention is that the electric field concentration effect at the drain end of the device gate is effectively improved, and at the same time, a new electric field peak is introduced at the contact part between the P-type doped region and the N-type doped region, so that the electric field distribution on the surface of the device is more accurate. uniform, thereby increasing the off-state breakdown voltage of the device.
附图说明Description of drawings
图1是具有场板的HEMT器件结构;Figure 1 is a HEMT device structure with a field plate;
图2是具有与栅电极电气相连的极化超结HEMT器件结构;Fig. 2 is a polarized superjunction HEMT device structure electrically connected to the gate electrode;
图3是具有凹槽绝缘栅结构的HEMT器件结构;3 is a HEMT device structure with a grooved insulating gate structure;
图4是实施例1的HEMT器件结构;Fig. 4 is the HEMT device structure of embodiment 1;
图5是实施例2的HEMT器件结构;Fig. 5 is the HEMT device structure of embodiment 2;
图6是实施例3的HEMT器件结构;Fig. 6 is the HEMT device structure of embodiment 3;
图7是实施例4的HEMT器件结构;Fig. 7 is the HEMT device structure of embodiment 4;
图8是实施例5的HEMT器件结构;Fig. 8 is the HEMT device structure of embodiment 5;
图9是实施例6的HEMT器件结构;Fig. 9 is the HEMT device structure of embodiment 6;
图10是本发明提出的结型超异质结HEMT器件结构与传统MOS-HEMT结构的反向耐压比较图;Fig. 10 is a comparison diagram of the reverse withstand voltage between the junction superheterojunction HEMT device structure proposed by the present invention and the traditional MOS-HEMT structure;
图11是本发明提出的结型超异质结HEMT器件结构与传统MOS-HEMT结构的反向耐压时电场分布比较图。Fig. 11 is a comparison diagram of the electric field distribution between the junction superheterojunction HEMT device structure proposed by the present invention and the traditional MOS-HEMT structure during reverse withstand voltage.
具体实施方式Detailed ways
下面结合附图和实施例,详细描述本发明的技术方案:Below in conjunction with accompanying drawing and embodiment, describe technical solution of the present invention in detail:
实施例1Example 1
如图4所示,本例包括衬底1、设置在衬底1上表面的缓冲层2和设置在缓冲层2上表面的势垒层3,所述缓冲层2和势垒层3的接触面形成具有二维电子气沟道(2DEG)的第一异质结;所述势垒层3上表面的两端分别具有源电极4和漏电极5,势垒层3上表面中部具有栅极结构;所述源电极4与栅极结构之间的势垒层3上表面具有介质钝化层10,所述漏电极5与栅极结构之间的势垒层3上表面具有结型半导体层8;所述结型半导体层8与势垒层3的接触面形成具有二维空穴气(2DHG)的第二异质结;其特征在于,所述结型半导体层8由P型掺杂区81和N型掺杂区82构成,所述P型掺杂区81与栅极结构连接,所述N型掺杂区82与漏电极5之间具有能阻断二维空穴气的隔断层11;所述栅极结构由绝缘栅介质7和金属栅电极6构成,所述绝缘栅介质7分别与介质钝化层10、势垒层3和P型掺杂区81连接,其横截面形状为U型结构,所述金属栅电极6位于绝缘栅介质7中,所述金属栅电极6沿器件横向方向延伸并覆盖在绝缘栅介质7的上表面;所述金属栅电极6还延伸至P型掺杂区81上表面并与结型半导体层8之间形成整流结构9;所述整流结构9为金属栅电极6与P型掺杂区81接触形成肖特基势垒接触,其中隔断层11为采用离子注入方式阻断2DHG。As shown in FIG. 4 , this example includes a substrate 1, a buffer layer 2 disposed on the upper surface of the substrate 1, and a barrier layer 3 disposed on the upper surface of the buffer layer 2. The contact between the buffer layer 2 and the barrier layer 3 A first heterojunction with a two-dimensional electron gas channel (2DEG) is formed on the surface; the two ends of the upper surface of the barrier layer 3 have a source electrode 4 and a drain electrode 5 respectively, and the middle part of the upper surface of the barrier layer 3 has a gate structure; the upper surface of the barrier layer 3 between the source electrode 4 and the gate structure has a dielectric passivation layer 10, and the upper surface of the barrier layer 3 between the drain electrode 5 and the gate structure has a junction semiconductor layer 8; the contact surface between the junction semiconductor layer 8 and the barrier layer 3 forms a second heterojunction with two-dimensional hole gas (2DHG); it is characterized in that the junction semiconductor layer 8 is doped by P type region 81 and N-type doped region 82, the P-type doped region 81 is connected to the gate structure, the N-type doped region 82 and the drain electrode 5 have a partition capable of blocking two-dimensional hole gas layer 11; the gate structure is composed of an insulating gate dielectric 7 and a metal gate electrode 6, and the insulating gate dielectric 7 is respectively connected with the dielectric passivation layer 10, the barrier layer 3 and the P-type doped region 81, and its cross section The shape is a U-shaped structure, the metal gate electrode 6 is located in the insulating gate dielectric 7, the metal gate electrode 6 extends along the lateral direction of the device and covers the upper surface of the insulating gate dielectric 7; the metal gate electrode 6 also extends to A rectification structure 9 is formed between the upper surface of the P-type doped region 81 and the junction semiconductor layer 8; the rectification structure 9 is formed by contacting the metal gate electrode 6 with the P-type doped region 81 to form a Schottky barrier contact. Layer 11 is to block 2DHG by ion implantation.
本例的工作原理为:首先,整流结构与结型半导体层的P型区域形成肖特基势垒,避免栅上加正压时造成栅极-2DHG-2DEG的泄漏电流,同时隔离结构采用离子注入方式阻断2DHG;其次结型半导体层/势垒层/缓冲层形成极化超结结构,阻断状态时,2DHG辅助耗尽漂移区,有效的改善了器件栅靠漏端的电场集中效应,使器件表面电场分布更加均匀,获得极大的耐压提升。The working principle of this example is as follows: First, the rectification structure and the P-type region of the junction semiconductor layer form a Schottky barrier to avoid the leakage current of the gate-2DHG-2DEG when a positive voltage is applied to the gate. At the same time, the isolation structure adopts ion The injection method blocks 2DHG; secondly, the junction semiconductor layer/barrier layer/buffer layer forms a polarized superjunction structure. In the blocking state, 2DHG assists in depleting the drift region, which effectively improves the electric field concentration effect at the drain end of the device gate. The electric field distribution on the surface of the device is made more uniform, and the withstand voltage is greatly improved.
实施例2Example 2
如图5所示,本例与实施例1不同的地方在于,本例器件整流结构9为PN结整流,其他结构与实施例1相同。整流结构与结型半导体层的P型区域形成PN结,避免栅上加正压时造成栅极-2DHG-2DEG的泄漏电流,导致器件提前击穿。As shown in FIG. 5 , the difference between this example and Example 1 is that the rectification structure 9 of the device in this example is PN junction rectification, and other structures are the same as those of Example 1. The rectifier structure and the P-type region of the junction semiconductor layer form a PN junction, which prevents the leakage current of the gate-2DHG-2DEG from being caused by a positive voltage on the gate, resulting in premature breakdown of the device.
实施例3Example 3
如图6所示,本例与实施例1不同的地方在于,隔断层11采用刻槽方式阻断2DHG,用于避免因栅加正压时造成栅极-2DHG-2DEG的泄漏电流而导致器件提前击穿。As shown in Figure 6, the difference between this example and Example 1 is that the isolation layer 11 uses grooves to block the 2DHG, which is used to avoid the leakage current of the gate-2DHG-2DEG caused by the positive voltage on the gate. Early breakdown.
实施例4Example 4
如图7所示,本例与实施例1不同的地方在于,本例器件在结型结型半导体层8上方形成介质钝化层10,栅漏之间的介质钝化层10靠漏一侧上方形成漏场板12,与漏电极5电气相连。采用介质钝化层可以改善器件的表面态,抑制电流崩塌。所述介质钝化层材料可以采用与栅介质相同的材料且同时形成,或者采用SiNx、Al2O3、AlN等常用介质材料。与此同时,漏场板12的引入,可以有效的降低漏端的电场尖峰,避免了漏电发生提前击穿。As shown in Figure 7, the difference between this example and Example 1 is that the device of this example forms a dielectric passivation layer 10 above the junction semiconductor layer 8, and the dielectric passivation layer 10 between the gate and drain is on the drain side. A drain field plate 12 is formed above, and is electrically connected to the drain electrode 5 . The use of a dielectric passivation layer can improve the surface state of the device and suppress the current collapse. The material of the dielectric passivation layer can be the same material as the gate dielectric and formed at the same time, or common dielectric materials such as SiNx, Al2O3, AlN, etc. can be used. At the same time, the introduction of the leakage field plate 12 can effectively reduce the electric field peak at the drain end, and avoid premature breakdown of the leakage.
实施例5Example 5
如图8所示,本例与实施例1不同的地方在于,本例器件栅极结构为凹槽绝缘栅结构。凹槽绝缘栅结构将栅下势垒层全部刻蚀,实现增强型器件。凹栅刻蚀能够有效地耗尽栅极下方2DEG浓度,极大地提高阈值电压,但是栅下势垒层全部刻蚀会对缓冲层界面造成损伤,影响器件的电学性能。As shown in FIG. 8 , the difference between this example and Example 1 is that the gate structure of the device in this example is a grooved insulated gate structure. The recessed insulating gate structure etches all the barrier layer under the gate to realize an enhanced device. Recessed gate etching can effectively deplete the 2DEG concentration under the gate and greatly increase the threshold voltage, but all etching of the barrier layer under the gate will cause damage to the interface of the buffer layer and affect the electrical performance of the device.
实施例6Example 6
如图9所示,本例与实施例5不同的地方在于,凹槽绝缘栅结构将栅下势垒层部分刻蚀,实现增强型器件,与实施例5相比,栅下势垒层部分刻蚀可在一定程度上避免因刻蚀所造成的界面损伤。As shown in Figure 9, the difference between this example and Example 5 is that the recessed insulated gate structure partially etches the lower barrier layer to realize an enhanced device. Compared with Example 5, the lower barrier layer part Etching can avoid the interface damage caused by etching to a certain extent.
本发明的HEMT器件,可以采用蓝宝石,硅,碳化硅(SiC),氮化铝(AlN)或氮化镓(GaN)中的一种或几种的组合作为衬底层1的材料;可以采用GaN、AlN、AlGaN中的一种或几种的组合作为缓冲层2的材料;可以采用GaN、AlN、AlGaN、InGaN、InAlN中的一种或几种的组合作为势垒层3的材料;可以采用Si、SiC、GaN、AlN、AlGaN、InGaN、InAlN中的一种或几种的组合作为结型结型半导体层8的材料;对于钝化层10,业界常用的材料为SiNx,也可采用Al2O3,AlN等介质材料,绝缘栅介质7可采用与钝化层相同的材料;源电极4、漏电极5一般采用金属合金,常用的有Ti/Al/Ni/Au或Mo/Al/Mo/Au等;栅电极6一般采用功函数较大的金属合金,例如Ni/Au或Ti/Au等。The HEMT device of the present invention can adopt one or more combination in sapphire, silicon, silicon carbide (SiC), aluminum nitride (AlN) or gallium nitride (GaN) as the material of substrate layer 1; Can adopt GaN One or more of AlN, AlGaN is used as the material of the buffer layer 2; one or more of GaN, AlN, AlGaN, InGaN, and InAlN can be used as the material of the barrier layer 3; One or a combination of Si, SiC, GaN, AlN, AlGaN, InGaN, InAlN is used as the material of the junction semiconductor layer 8; for the passivation layer 10, the material commonly used in the industry is SiNx, and Al2O3 can also be used , AlN and other dielectric materials, the insulating gate dielectric 7 can use the same material as the passivation layer; the source electrode 4 and the drain electrode 5 generally use metal alloys, commonly used are Ti/Al/Ni/Au or Mo/Al/Mo/Au etc.; the gate electrode 6 generally adopts a metal alloy with a relatively large work function, such as Ni/Au or Ti/Au.
图10、图11分别是本发明提出的结型超异质结HEMT器件结构与传统MOS-HEMT结构的反向耐压比较图、反向耐压时电场分布比较图。采用SentaurusTCAD软件进行仿真,两种结构在器件横向尺寸均为10.5μm,栅长均为1.5μm,栅漏距离均为5μm的条件下,本发明所提出的结构的击穿电压从传统MOS-HEMT的548V提高到880V,击穿电压提高60%。Fig. 10 and Fig. 11 are respectively the comparison diagrams of the reverse withstand voltage and the comparison diagram of the electric field distribution during the reverse withstand voltage between the junction superheterojunction HEMT device structure proposed by the present invention and the traditional MOS-HEMT structure. Using SentaurusTCAD software for simulation, the two structures have a device lateral dimension of 10.5 μm, a gate length of 1.5 μm, and a gate-to-drain distance of 5 μm. The 548V is increased to 880V, and the breakdown voltage is increased by 60%.
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| CN119521725B (en) * | 2024-11-08 | 2026-01-02 | 电子科技大学 | A novel heterojunction field plate gallium oxide MOSFET device |
| CN120730770A (en) * | 2025-08-14 | 2025-09-30 | 山东大学 | A P-N junction field plate GaN power device with source field plate connection |
| CN120730770B (en) * | 2025-08-14 | 2025-11-11 | 山东大学 | A P-N junction junction field-plate GaN power device with source field plate connection |
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