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CN113113469B - A high withstand voltage double gate lateral HEMT device and its preparation method - Google Patents

A high withstand voltage double gate lateral HEMT device and its preparation method Download PDF

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CN113113469B
CN113113469B CN202110259511.5A CN202110259511A CN113113469B CN 113113469 B CN113113469 B CN 113113469B CN 202110259511 A CN202110259511 A CN 202110259511A CN 113113469 B CN113113469 B CN 113113469B
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尹以安
李佳霖
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South China Normal University
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Abstract

本发明涉及一种高耐压双栅极横向HEMT器件,包括位于衬底上的缓冲层以及依次层叠于缓冲层上的GaN沟道层、AlN插入层和AlGaN势垒层组成的叠层,还包括p型埋层、位于p型埋层上的栅极和位于势垒层上的源/漏极和Γ型栅;沿厚度方向上,p型埋层自缓冲层靠近沟道层的表面朝向缓冲层中远离沟道层的一侧延伸一定深度;源极和漏极位于势垒层表面;源极和漏极之间设置一栅槽,Γ型栅位于栅槽中并朝向漏极一侧延伸;沿长度方向上,p型埋层自栅极下方延伸至栅槽下方。通过p型埋层的引入、双栅结合AlGaN/AlN/GaN异质结的结构设置,本发明获得了低导通电阻、高饱和电流、高击穿电压和低泄漏电流HEMT器件。

The invention relates to a high withstand voltage double-gate lateral HEMT device, which comprises a buffer layer on a substrate and a stack composed of a GaN channel layer, an AlN insertion layer and an AlGaN barrier layer sequentially stacked on the buffer layer. Including the p-type buried layer, the gate on the p-type buried layer, the source/drain and the Γ-type gate on the barrier layer; along the thickness direction, the p-type buried layer faces from the surface of the buffer layer close to the channel layer The side of the buffer layer away from the channel layer extends to a certain depth; the source and the drain are located on the surface of the barrier layer; a gate groove is arranged between the source and the drain, and the Γ-type gate is located in the gate groove and faces the drain side Extending: along the length direction, the p-type buried layer extends from below the gate to below the gate groove. Through the introduction of the p-type buried layer and the structure setting of double gates combined with AlGaN/AlN/GaN heterojunction, the invention obtains HEMT devices with low on-resistance, high saturation current, high breakdown voltage and low leakage current.

Description

一种高耐压双栅极横向HEMT器件及其制备方法A high withstand voltage double gate lateral HEMT device and its preparation method

技术领域technical field

本发明涉及HEMT器件技术领域,尤其涉及一种高耐压双栅极横向HEMT器件及其制备方法。The invention relates to the technical field of HEMT devices, in particular to a high withstand voltage double-gate lateral HEMT device and a preparation method thereof.

背景技术Background technique

AlGaN/GaN HEMT器件,在高功率、高工作温度、强抗辐照能力等性能方面的潜能已然超越了Si基功率器件,其不仅具有GaN材料的优势,而且AlGaN/GaN异质结界面处产生极化电场,能够形成高迁移率和高载流子面密度的二维电子气(2DEG),在电力电子领域受到了极大的关注。AlGaN/GaN HEMT devices have surpassed Si-based power devices in terms of high power, high operating temperature, and strong radiation resistance. They not only have the advantages of GaN materials, but also AlGaN/GaN heterojunctions. Polarized electric fields, capable of forming a two-dimensional electron gas (2DEG) with high mobility and high carrier areal density, have received great attention in the field of power electronics.

虽然AlGaN/GaN HEMT器件在理论上具有很高的耐压特性,但实际器件的击穿电压只有几百伏,离GaN材料的理论耐压极限还有很大差距,限制着GaN基HEMT器件的大规模应用。其耐压低的主要原因有:(1)栅极电场的集中效应。当器件处在关断状态下时,电场线集中在栅极边缘,在栅极靠漏一侧出现电场峰值,使器件提前击穿;(2)缓冲层的泄漏电流。在关断状态下,从源极注入的电子经过缓冲层到达漏极形成电流通道,造成器件的提前击穿。因此,提高HEMT器件的耐压能力对改善其性能具有非常重要的意义。Although AlGaN/GaN HEMT devices have high withstand voltage characteristics in theory, the breakdown voltage of actual devices is only a few hundred volts, which is still far from the theoretical withstand voltage limit of GaN materials, which limits the development of GaN-based HEMT devices. large-scale application. The main reasons for its low withstand voltage are: (1) The concentration effect of the gate electric field. When the device is in the off state, the electric field lines are concentrated on the gate edge, and the electric field peak appears on the drain side of the gate, causing the device to break down in advance; (2) The leakage current of the buffer layer. In the off state, electrons injected from the source pass through the buffer layer to the drain to form a current channel, causing premature breakdown of the device. Therefore, it is of great significance to improve the withstand voltage capability of HEMT devices to improve their performance.

发明内容Contents of the invention

本发明的首要目的在于提供一种高耐压双栅极横向HEMT器件及其制备方法,以克服现有技术中的不足,获得低导通电阻、高饱和电流、高击穿电压和低泄漏电流的HEMT器件。The primary purpose of the present invention is to provide a high withstand voltage double-gate lateral HEMT device and its preparation method, to overcome the deficiencies in the prior art, to obtain low on-resistance, high saturation current, high breakdown voltage and low leakage current HEMT devices.

本发明提供的高耐压双栅极横向HEMT器件,既可由P型栅极与MIS槽栅共同控制,同时也可由P型栅极与MIS栅独立控制。通过在部分GaN沟道层中离子注入形成p型埋层,形成了独立的P-GaN栅极结构,参与调控沟道层的二维电子气。其作用机理如下:p型埋层与GaN沟道层构成PN结,形成空间电荷区,消耗一部分2DEG,提高了器件的阈值电压。p型GaN栅极位于AlGaN势垒层、AlN插入层和GaN沟道层构成的AlGaN/AlN/GaN异质结叠层一侧,在器件工作状态下,P-GaN栅极接正电压,GaN沟道层的源极接负电压,此时PN结正向导通,空间电荷区减小,降低了源漏的导通电阻,提高了正向输出电流。当器件处于关断状态,P-GaN栅极接负电压,GaN沟道层的漏极接正电压,PN结处于反向偏压,同时与GaN缓冲层也形成PN结反向偏压,不仅减少了栅极泄漏电流,也减少了缓冲层的泄漏电流,大大提高了器件的耐压特性。而MIS槽栅则是通过刻蚀部分AlGaN势垒层形成,降低了栅极下方势垒层的厚度,使阈值电压正移,提高栅控能力。同时,在MIS槽栅朝向漏极一侧引入Γ型栅场板,能够优化栅极电场分布,减低栅极电场集中效应,提高器件的耐压特性。The high withstand voltage double-gate lateral HEMT device provided by the present invention can be controlled jointly by the P-type gate and the MIS slot gate, and can also be independently controlled by the P-type gate and the MIS gate. A p-type buried layer is formed by ion implantation in part of the GaN channel layer, forming an independent P-GaN gate structure, which participates in regulating the two-dimensional electron gas of the channel layer. The mechanism of action is as follows: the p-type buried layer and the GaN channel layer form a PN junction, forming a space charge region, consuming part of the 2DEG, and increasing the threshold voltage of the device. The p-type GaN gate is located on the side of the AlGaN/AlN/GaN heterojunction stack composed of the AlGaN barrier layer, the AlN insertion layer and the GaN channel layer. In the working state of the device, the P-GaN gate is connected to a positive voltage, and the GaN The source of the channel layer is connected to a negative voltage. At this time, the PN junction is forward-conducting, the space charge area is reduced, the on-resistance of the source and drain is reduced, and the forward output current is increased. When the device is in the off state, the P-GaN gate is connected to a negative voltage, the drain of the GaN channel layer is connected to a positive voltage, the PN junction is in reverse bias, and the GaN buffer layer also forms a PN junction reverse bias, not only The gate leakage current is reduced, and the leakage current of the buffer layer is also reduced, which greatly improves the withstand voltage characteristics of the device. The MIS groove gate is formed by etching part of the AlGaN barrier layer, which reduces the thickness of the barrier layer under the gate, shifts the threshold voltage positively, and improves the gate control capability. At the same time, the Γ-shaped gate field plate is introduced on the side of the MIS groove gate facing the drain, which can optimize the distribution of the gate electric field, reduce the concentration effect of the gate electric field, and improve the withstand voltage characteristics of the device.

其次在GaN沟道层和AlGaN势垒层之间插入AlN层形成更深而窄的量子阱,提高了沟道电子密度,同时抑制2DEG渗入到AlGaN势垒层中,提高了沟道电子迁移率且抑制了电流崩塌。Secondly, an AlN layer is inserted between the GaN channel layer and the AlGaN barrier layer to form a deeper and narrower quantum well, which increases the channel electron density, and at the same time inhibits 2DEG from penetrating into the AlGaN barrier layer, improving the channel electron mobility and The current collapse is suppressed.

另外,本发明的横向HEMT器件的制备方法简单,可行性高,制备的器件稳定性良好。基于上述目的,本发明至少提供如下技术方案:In addition, the preparation method of the lateral HEMT device of the present invention is simple, the feasibility is high, and the prepared device has good stability. Based on the above object, the present invention at least provides the following technical solutions:

一种高耐压双栅极横向HEMT器件,包括:衬底、位于衬底上的缓冲层以及依次层叠于缓冲层上的GaN沟道层、AlN插入层和AlGaN势垒层组成的叠层,还包括p型埋层、位于p型埋层上的p型栅极和位于势垒层上的源极、漏极和Γ型栅;其中,沿厚度方向上,p型埋层自所述缓冲层靠近沟道层的表面朝向缓冲层中远离所述沟道层的一侧延伸一定深度;源极和漏极位于势垒层表面;源极和漏极之间还设置一栅槽,该栅槽延伸至势垒层中一定深度,一高介电介质层设置于该栅槽内壁,Γ型栅位于该栅槽中并沿栅槽指向漏极的方向延伸;沿长度方向上,p型埋层自栅极下方延伸至栅槽下方。A high withstand voltage double-gate lateral HEMT device, comprising: a substrate, a buffer layer on the substrate, and a stack composed of a GaN channel layer, an AlN insertion layer, and an AlGaN barrier layer sequentially stacked on the buffer layer, It also includes a p-type buried layer, a p-type gate positioned on the p-type buried layer, and a source electrode, a drain electrode, and a Γ-type gate positioned on the barrier layer; wherein, along the thickness direction, the p-type buried layer is separated from the buffer The surface of the layer close to the channel layer extends to a certain depth toward the side of the buffer layer away from the channel layer; the source and the drain are located on the surface of the barrier layer; a gate groove is also arranged between the source and the drain, and the gate The groove extends to a certain depth in the barrier layer, a high dielectric layer is arranged on the inner wall of the gate groove, the Γ-type gate is located in the gate groove and extends along the direction from the gate groove to the drain; along the length direction, the p-type buried The layer extends from under the gate to under the trench.

进一步地,所述p型埋层的掺杂浓度大于等于108cm-3,厚度为70~150nm,长度为3~5μm。Further, the doping concentration of the p-type buried layer is greater than or equal to 10 8 cm -3 , the thickness is 70-150 nm, and the length is 3-5 μm.

进一步地,AlGaN势垒层、高介电介质层和Γ型栅构成MISΓ型槽栅结构。Further, the AlGaN barrier layer, the high dielectric layer and the Γ-type gate form a MISΓ-type groove gate structure.

进一步地,所述缓冲层优选GaN缓冲层,所述p型埋层选用F+离子源注入缓冲层中形成。Further, the buffer layer is preferably a GaN buffer layer, and the p-type buried layer is formed by implanting an F + ion source into the buffer layer.

进一步地,所述栅极与所述叠层之间设置有第一钝化层,所述Γ型栅与源极之间以及所述Γ型栅与漏极之间设置有第二钝化层。Further, a first passivation layer is provided between the gate and the laminate, a second passivation layer is provided between the Γ-shaped gate and the source and between the Γ-shaped gate and the drain .

进一步地,所述GaN沟道层的厚度为8~15nm;所述势垒层选用Al组分为1%~3%,厚度为15~30nm的AlGaN势垒层;所述AlN插入层的厚度为1~2nm。Further, the thickness of the GaN channel layer is 8-15nm; the barrier layer is an AlGaN barrier layer with an Al composition of 1%-3% and a thickness of 15-30nm; the thickness of the AlN insertion layer is It is 1~2nm.

进一步地,所述高介电介质层选用HfO2、Al2O3或TiO2,其厚度为4~6nm。Further, the high dielectric layer is selected from HfO 2 , Al 2 O 3 or TiO 2 , and its thickness is 4-6 nm.

进一步地,所述钝化层包括SiNx、SiO2、HfO2或Al2O3Further, the passivation layer includes SiN x , SiO 2 , HfO 2 or Al 2 O 3 .

进一步地,所述栅槽靠近所述源极。Further, the gate groove is close to the source.

本发明还提供一种高耐压双栅极横向HEMT器件的制备方法,包括以下步骤:The present invention also provides a method for preparing a high withstand voltage double-gate lateral HEMT device, comprising the following steps:

在衬底上外延生长缓冲层;growing the buffer layer epitaxially on the substrate;

在所述缓冲层的特定区域离子注入形成p型埋层;ion implantation in a specific region of the buffer layer to form a p-type buried layer;

在所述p型埋层以及缓冲层的表面依次外延生长GaN沟道层、AlN插入层和AlGaN势垒层形成叠层;Epitaxially growing a GaN channel layer, an AlN insertion layer, and an AlGaN barrier layer on the surface of the p-type buried layer and the buffer layer in sequence to form a stack;

刻蚀该叠层的预定区域暴露部分p型埋层区域;Etching a predetermined region of the stack to expose a part of the p-type buried layer region;

在p型埋层和AlGaN势垒层表面沉积钝化层;Depositing a passivation layer on the surface of the p-type buried layer and the AlGaN barrier layer;

刻蚀p型埋层表面的钝化层和势垒层表面的钝化层,形成栅极和源/漏极开孔;Etching the passivation layer on the surface of the p-type buried layer and the passivation layer on the surface of the barrier layer to form gate and source/drain openings;

沉积金属层形成欧姆接触的源/漏极和栅极;Deposit metal layers to form source/drain and gate of ohmic contacts;

刻蚀源极和漏极之间的钝化层至势垒层中一定深度形成栅槽;Etching the passivation layer between the source and the drain to a certain depth in the barrier layer to form a gate groove;

在栅槽内壁生长一定厚度的高介电介质层;A high dielectric layer with a certain thickness is grown on the inner wall of the gate groove;

沉积金属层形成肖特基接触的Γ型栅。A metal layer is deposited to form the Γ-gate of the Schottky contact.

附图说明Description of drawings

图1是本发明实施例高耐压双栅极横向HEMT器件的结构示意图。FIG. 1 is a schematic structural diagram of a high withstand voltage double-gate lateral HEMT device according to an embodiment of the present invention.

图2是本发明实施例高耐压双栅极横向HEMT器件的工作状态示意图。FIG. 2 is a schematic diagram of the working state of the high withstand voltage double-gate lateral HEMT device according to the embodiment of the present invention.

图3是本发明实施例高耐压双栅极横向HEMT器件的击穿状态的示意图。FIG. 3 is a schematic diagram of a breakdown state of a high withstand voltage double-gate lateral HEMT device according to an embodiment of the present invention.

图4是本发明实施例高耐压双栅极横向HEMT器件的制备工艺流程图。FIG. 4 is a flow chart of the manufacturing process of a high withstand voltage double-gate lateral HEMT device according to an embodiment of the present invention.

图5是本发明实施例高耐压双栅极横向HEMT器件的直流特性图。FIG. 5 is a DC characteristic diagram of a high withstand voltage double-gate lateral HEMT device according to an embodiment of the present invention.

图6是本发明实施例高耐压双栅极横向HEMT器件的击穿电压图。FIG. 6 is a breakdown voltage diagram of a high withstand voltage double-gate lateral HEMT device according to an embodiment of the present invention.

具体实施方式Detailed ways

接下来将结合本发明的附图对本发明实施例中的技术方案进行清楚、完整地描述,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,可以做出结构或逻辑的变化而不脱离本发明的范围。本发明的范围由所附权利要求限定。Next, the technical solutions in the embodiments of the present invention will be clearly and completely described in conjunction with the accompanying drawings of the present invention, and the described embodiments are only some of the embodiments of the present invention, not all of them. Based on the embodiments in the present invention, structural or logical changes may be made without departing from the scope of the present invention. The scope of the invention is defined by the appended claims.

本说明书中使用例如“之下”、“下方”、“下”、“之上”、“上方”、“上”等空间相对性术语,以解释一个元件相对于第二元件的定位。除了与图中所示那些不同的取向以外,这些术语意在涵盖器件的不同取向。Spatially relative terms such as "under", "beneath", "under", "above", "above", "upper", etc. are used in this specification to explain the positioning of one element relative to a second element. These terms are intended to encompass different orientations of the device in addition to orientations other than those depicted in the figures.

另外,使用诸如“第一”、“第二”等术语描述各个元件、区域、区段等,并非意在进行限制。使用“厚度方向上”理解为表示垂直于半导体材料或载体的表面范围延伸的方向或范围。本说明书中“长度方向上”特定理解为源极指向漏极或漏极指向源极的方向。使用的“具有”、“含有”、“包含”、“包括”等是开放式术语,表示存在所陈述的元件或特征,但不排除额外的元件或特征。除非上下文明确做出不同表述。In addition, the use of terms such as "first", "second", etc. to describe various elements, regions, sections, etc., is not intended to be limiting. The use "in the thickness direction" is understood to mean a direction or an extent extending perpendicularly to the surface extent of the semiconductor material or carrier. In this specification, "in the length direction" is specifically understood as a direction in which the source points to the drain or the drain points to the source. The use of "having", "containing", "comprising", "comprising" and the like are open-ended terms meaning the presence of stated elements or features but not excluding additional elements or features. unless the context clearly states otherwise.

下面来对本发明做进一步详细的说明。图1示出了根据优选实施例的横向HEMT器件的结构示意图。在该实施例中,横向HEMT包括衬底1和布置于衬底1上的缓冲层3。衬底1可以包括Si、蓝宝或SiC。缓冲层3优选GaN缓冲层,GaN缓冲层的厚度为2~5μm,优选地,GaN缓冲层的厚度为3.5μm。在该优选实施例中,衬底1与缓冲层3之间还包含一AlN成核层2。The present invention will be described in further detail below. Fig. 1 shows a schematic structural diagram of a lateral HEMT device according to a preferred embodiment. In this embodiment, the lateral HEMT includes a substrate 1 and a buffer layer 3 arranged on the substrate 1 . The substrate 1 may comprise Si, sapphire or SiC. The buffer layer 3 is preferably a GaN buffer layer, the thickness of the GaN buffer layer is 2-5 μm, preferably, the thickness of the GaN buffer layer is 3.5 μm. In this preferred embodiment, an AlN nucleation layer 2 is also included between the substrate 1 and the buffer layer 3 .

在图1所示的实施例中,沟道层5、插入层6和势垒层7构成的叠层布置于缓冲层3的部分表面。沟道层5优选GaN沟道层,GaN沟道层的厚度为8~15nm。在优选实施例中,插入层6优选AlN插入层,其厚度为1~2nm,优选地,AlN插入层的厚度为1nm。势垒层7优选AlGaN势垒层,其中Al组分为1%-3%,厚度为15-30nm。该优选实施例中,在GaN沟道层和AlGaN势垒层之间插入AlN层,不仅能形成更深而窄的量子阱,提高了沟道电子密度;还能抑制2DEG渗入到AlGaN势垒层中,提高了沟道电子迁移率且抑制了电流崩塌,从而提高了器件的击穿电压。In the embodiment shown in FIG. 1 , a stack of channel layer 5 , insertion layer 6 and barrier layer 7 is arranged on part of the surface of buffer layer 3 . The channel layer 5 is preferably a GaN channel layer, and the thickness of the GaN channel layer is 8-15 nm. In a preferred embodiment, the insertion layer 6 is preferably an AlN insertion layer with a thickness of 1-2 nm, preferably, the thickness of the AlN insertion layer is 1 nm. The barrier layer 7 is preferably an AlGaN barrier layer, wherein the Al composition is 1%-3%, and the thickness is 15-30nm. In this preferred embodiment, an AlN layer is inserted between the GaN channel layer and the AlGaN barrier layer, which not only forms a deeper and narrower quantum well, improves the channel electron density, but also inhibits 2DEG from penetrating into the AlGaN barrier layer , improving the channel electron mobility and suppressing the current collapse, thereby increasing the breakdown voltage of the device.

该横向HEMT还包括源极10、漏极9、p型栅极11和Γ型栅14。p型栅极11即p型GaN栅极,被配置为布置于缓冲层3的表面、叠层的一侧,栅极11通过第二钝化层12与叠层隔离。源极10和漏极9布置在势垒层7上,第一钝化层8布置在源极10和漏极9之间,一栅槽沿第一钝化层8的表面延伸至势垒层7中一定深度,栅槽的内壁上设置有一定厚度的高介电介质层13。Γ型栅14设置于该栅槽中,且自该栅槽延伸至栅槽与漏极9之间的第一钝化层8的表面。该Γ型栅14、高介电介质层13和AlGaN势垒层7构成了MISΓ型栅结构。该MISΓ型栅结构在功能上既能起到MIS槽栅结构的作用,又能够沿漏极一侧起到Γ型栅场板结构的作用。首先槽栅可减薄势垒层,减少二维电子气,使阈值电压正移,提高器件控栅能力。其次,选用高介电常数介质作为栅介质层,可提高器件的频率特性,且介质层材料禁带宽度越大,可形成越高的导带不连续性,即减小了栅漏电,也提高器件的击穿特性。进一步地采用场板结构,缓解了栅极电场集中的现象,使电场分布更加均匀,进一步提高了器件的耐压特性。具体地,栅槽靠近源极10。高介电介质层选用HfO2、Al2O3或TiO2,其厚度为4-6nm。第一钝化层和第二钝化层包括SiNx、SiO2、HfO2或Al2O3The lateral HEMT also includes a source 10 , a drain 9 , a p-type gate 11 and a Γ-type gate 14 . The p-type gate 11 , that is, the p-type GaN gate, is configured to be arranged on the surface of the buffer layer 3 and one side of the stack, and the gate 11 is isolated from the stack by the second passivation layer 12 . The source electrode 10 and the drain electrode 9 are arranged on the barrier layer 7, the first passivation layer 8 is arranged between the source electrode 10 and the drain electrode 9, and a gate groove extends along the surface of the first passivation layer 8 to the barrier layer 7, a high dielectric layer 13 with a certain thickness is provided on the inner wall of the grid groove at a certain depth. The Γ-shaped gate 14 is disposed in the gate groove and extends from the gate groove to the surface of the first passivation layer 8 between the gate groove and the drain 9 . The Γ-type gate 14, the high dielectric layer 13 and the AlGaN barrier layer 7 constitute a MISΓ-type gate structure. The MISΓ-type gate structure can function not only as a MIS trench gate structure, but also as a Γ-type gate field plate structure along the drain side. Firstly, the trench gate can thin the barrier layer, reduce the two-dimensional electron gas, shift the threshold voltage positively, and improve the gate control ability of the device. Secondly, choosing a high dielectric constant dielectric as the gate dielectric layer can improve the frequency characteristics of the device, and the larger the forbidden band width of the dielectric layer material, the higher the conduction band discontinuity can be formed, which reduces the gate leakage and improves Breakdown characteristics of the device. Further adopting the field plate structure alleviates the phenomenon of grid electric field concentration, makes the electric field distribution more uniform, and further improves the withstand voltage characteristics of the device. Specifically, the gate trench is close to the source 10 . The high dielectric layer is made of HfO 2 , Al 2 O 3 or TiO 2 , and its thickness is 4-6nm. The first passivation layer and the second passivation layer include SiN x , SiO 2 , HfO 2 or Al 2 O 3 .

该横向HEMT还包括p型埋层4。在一优选方案中,p型埋层4优选F+离子源注入部分缓冲层3中进行掺杂形成。埋层4的厚度为70~150nm,长度为3~5μm,其掺杂浓度大于等于108cm-3。优选地,埋层4的载流子浓度为1×1018cm-3,其长度为3μm,厚度为100nm。The lateral HEMT also includes a p-type buried layer 4 . In a preferred solution, the p-type buried layer 4 is preferably formed by implanting F + ions into a part of the buffer layer 3 for doping. The buried layer 4 has a thickness of 70-150 nm, a length of 3-5 μm, and a doping concentration greater than or equal to 10 8 cm −3 . Preferably, the buried layer 4 has a carrier concentration of 1×10 18 cm −3 , a length of 3 μm, and a thickness of 100 nm.

p型栅极11布置为与p型埋层4接触形成p型栅极。具体地,沿厚度方向上,p型埋层4布置于自缓冲层3与栅极11接触的表面朝向缓冲层中远离沟道层5的一侧延伸一定深度。沿长度方向上,p型埋层4自栅极11的正下方延伸至栅槽的正下方。该实施例中,引入p型埋层形成p型栅,p型GaN与GaN沟道层形成PN结,利用PN结二极管的特性调节沟道层内的电子气浓度和电场强度,器件关断状态下,可减小2DEG,提高HEMT器件的阈值电压,减小泄漏电流和提高击穿电压,增强器件的可靠性。器件导通时,PN结正向导通,降低导通电阻,提高导通电流。The p-type gate 11 is arranged in contact with the p-type buried layer 4 to form a p-type gate. Specifically, along the thickness direction, the p-type buried layer 4 is arranged to extend a certain depth from the surface of the buffer layer 3 in contact with the gate 11 toward the side of the buffer layer away from the channel layer 5 . Along the length direction, the p-type buried layer 4 extends from directly below the gate 11 to directly below the gate trench. In this embodiment, a p-type buried layer is introduced to form a p-type gate, p-type GaN and GaN channel layer form a PN junction, and the characteristics of the PN junction diode are used to adjust the electron gas concentration and electric field strength in the channel layer, and the device is turned off. Under this condition, 2DEG can be reduced, the threshold voltage of the HEMT device can be increased, the leakage current can be reduced, the breakdown voltage can be increased, and the reliability of the device can be enhanced. When the device is turned on, the PN junction is forward-conducting, which reduces the on-resistance and increases the on-current.

源极10、漏极9和p型栅极11为欧姆接触。优选地,源极10、漏极9和p型栅极11选用Ti/Al/Ni/Au合金、Ti/Al/Mo/Au合金或Ti/Al/Ti/TiN合金。Γ型栅14为肖特基接触。优选地,Γ型栅选用Ni/Au合金。The source 10, the drain 9 and the p-type gate 11 are ohmic contacts. Preferably, the source 10 , the drain 9 and the p-type gate 11 are Ti/Al/Ni/Au alloy, Ti/Al/Mo/Au alloy or Ti/Al/Ti/TiN alloy. The Γ-shaped gate 14 is a Schottky contact. Preferably, Ni/Au alloy is used for the Γ-shaped gate.

图2是优选实施例的横向HEMT器件处于工作状态的示意图。该工作状态中,p型GaN栅极接正电压,源极接负电压,PN结处于正向导通状态,空间电荷区减小,降低了源漏导通电阻,提高了正向输出电流。同时,P-GaN埋层与GaN缓冲层形成的PN结也可以减小部分泄漏电流。参见图5的器件直流特性图,在栅极电压为3V恒定不变的条件下,源漏电压增至10V时,导通电流可高达827mA/mm。Fig. 2 is a schematic diagram of a lateral HEMT device in a preferred embodiment in an operating state. In this working state, the p-type GaN gate is connected to a positive voltage, the source is connected to a negative voltage, the PN junction is in a forward conduction state, the space charge area is reduced, the source-drain on-resistance is reduced, and the forward output current is increased. At the same time, the PN junction formed by the P-GaN buried layer and the GaN buffer layer can also reduce part of the leakage current. Referring to the DC characteristic diagram of the device in Figure 5, under the condition that the gate voltage is constant at 3V, when the source-drain voltage increases to 10V, the conduction current can reach as high as 827mA/mm.

图3为优选实施例的横向HEMT器件处于击穿状态的示意图。P-GaN栅极接负电压,GaN沟道层的漏极接正电压,PN结处于反向截止状态,同时与GaN缓冲层也形成PN结反向偏压,不仅减少了栅极泄漏电流,也减少了缓冲层的泄漏电流,大大提高了器件的耐压特性。如图6所示,该状态下,横向HEMT器件的击穿电压可高达2500V。Fig. 3 is a schematic diagram of a lateral HEMT device in a breakdown state of a preferred embodiment. The P-GaN gate is connected to a negative voltage, the drain of the GaN channel layer is connected to a positive voltage, and the PN junction is in a reverse cut-off state. At the same time, it forms a PN junction reverse bias with the GaN buffer layer, which not only reduces the gate leakage current, It also reduces the leakage current of the buffer layer and greatly improves the withstand voltage characteristics of the device. As shown in Figure 6, in this state, the breakdown voltage of the lateral HEMT device can be as high as 2500V.

功率器件的优值FOM定义为: The figure of merit FOM of a power device is defined as:

其中,Bv是器件的击穿电压,RON是器件的特征导通电阻。高的击穿电压,小的特征导通电阻是功率器件所追求的目标。上述优选实施例获得的优值FOM高达15.39GW·cm2where Bv is the breakdown voltage of the device and R ON is the characteristic on-resistance of the device. High breakdown voltage and small characteristic on-resistance are the goals pursued by power devices. The figure of merit FOM obtained by the above preferred embodiment is as high as 15.39GW·cm 2 .

基于上述横向HEMT器件,参见图4,本发明一优选实施例还提供了该器件的制备方法,该制备方法工艺流程简单,可行性高,制备的器件稳定性良好。该方法包括以下步骤:Based on the above-mentioned lateral HEMT device, referring to FIG. 4 , a preferred embodiment of the present invention also provides a preparation method of the device. The preparation method has a simple process flow, high feasibility, and good stability of the prepared device. The method includes the following steps:

在衬底上依次外延生长缓冲层和沟道层。在一优选实施例中,衬底选用蓝宝石衬底,缓冲层和衬底之间还设置一AlN成核层。具体地,首先,清洗蓝宝石衬底1。将衬底依次置于丙酮、乙醇、去离子水中各超声10分钟,取出后用去离子水进行冲洗,最后用N2吹干,去除衬底表面的污染物。然后选用MOCVD技术生长厚度为1nm的AlN成核层和厚度为3.53μm的GaN缓冲层3。A buffer layer and a channel layer are epitaxially grown sequentially on the substrate. In a preferred embodiment, the substrate is a sapphire substrate, and an AlN nucleation layer is arranged between the buffer layer and the substrate. Specifically, first, the sapphire substrate 1 is cleaned. Place the substrate in acetone, ethanol, and deionized water in sequence for 10 minutes of ultrasonication, rinse with deionized water after taking it out, and finally blow dry with N2 to remove pollutants on the substrate surface. Then the MOCVD technique is used to grow an AlN nucleation layer with a thickness of 1 nm and a GaN buffer layer 3 with a thickness of 3.53 μm.

接着,采用离子注入机将F+离子源直接注入GaN缓冲层3的选定表面,注入能量为11keV,注入剂量为2×1018cm-2,注入角度为正8°,在GaN缓冲层的特定区域形成p型GaN埋层4。Next, use an ion implanter to directly implant F + ion source into the selected surface of the GaN buffer layer 3, the implantation energy is 11keV, the implantation dose is 2×10 18 cm -2 , and the implantation angle is positive 8°. A p-type GaN buried layer 4 is formed in a specific region.

之后,继续用MOCVD工艺依次生长厚度为10nm的GaN沟道层5、厚度为1nm的AlN插入层6和厚度为30nm的AlGaN势垒层7,形成GaN/AlN/AlGaN异质结。其中,AlGaN势垒层7的Al组分为1%~3%。Afterwards, continue to grow GaN channel layer 5 with a thickness of 10nm, AlN insertion layer 6 with a thickness of 1nm, and AlGaN barrier layer 7 with a thickness of 30nm by MOCVD process to form a GaN/AlN/AlGaN heterojunction. Wherein, the Al composition of the AlGaN barrier layer 7 is 1%˜3%.

接着,采用感应耦合等离子体刻蚀(ICP)工艺对外延片选定区域进行刻蚀至p型GaN埋层4的表面。Next, the selected region of the epitaxial wafer is etched to the surface of the p-type GaN buried layer 4 by using an inductively coupled plasma etching (ICP) process.

之后,选用离子增强型化学气相沉积(PECVD)工艺,在p型GaN埋层4和AlGaN势垒层7表面沉积SiNx钝化层8。Afterwards, an ion-enhanced chemical vapor deposition (PECVD) process is used to deposit a SiNx passivation layer 8 on the surface of the p-type GaN buried layer 4 and the AlGaN barrier layer 7 .

继续刻蚀钝化层,在p型埋层的钝化层中和势垒层的钝化层中形成栅极和源/漏极开孔。优选地,选用反应离子刻蚀(RIE),在SiNx钝化层8选定区域进行开孔,用于沉积金属电极。Continue to etch the passivation layer to form gate and source/drain openings in the passivation layer of the p-type buried layer and the passivation layer of the barrier layer. Preferably, reactive ion etching (RIE) is used to open holes in selected areas of the SiNx passivation layer 8 for depositing metal electrodes.

选用电子束蒸发工艺,分别在栅极开孔位置和源/漏极开孔位置沉积Ti/Al/Ni/Au金属电极,之后在880℃的氮气气氛中快速退火40s,形成欧姆接触的源极、漏极和p型GaN栅极。优选地,金属Ti层、Al层、Ni层和Au层的厚度分别为20nm、100nm、40nm和120nm。The electron beam evaporation process is used to deposit Ti/Al/Ni/Au metal electrodes at the gate opening position and the source/drain opening position respectively, and then rapidly annealed in a nitrogen atmosphere at 880°C for 40s to form an ohmic contact source , drain and p-type GaN gate. Preferably, the thicknesses of the metal Ti layer, Al layer, Ni layer and Au layer are 20 nm, 100 nm, 40 nm and 120 nm, respectively.

接着,采用光刻工艺刻蚀源极和漏极之间的钝化层形成凹槽图形,之后选用ICP干法刻蚀工艺继续刻蚀部分AlGaN势垒层形成栅槽。优选地,势垒层的刻蚀深度为10nm。Next, a photolithography process is used to etch the passivation layer between the source and drain to form a groove pattern, and then an ICP dry etching process is used to continue etching part of the AlGaN barrier layer to form a gate groove. Preferably, the etching depth of the barrier layer is 10 nm.

接着在栅槽中生长高介电介质层,优选地,选用PEALD工艺在栅槽内壁上生长6nm的HfO2高介电介质层作为栅介质层。Next, a high dielectric layer is grown in the gate groove, preferably, a 6nm HfO2 high dielectric layer is grown on the inner wall of the gate groove by PEALD process as the gate dielectric layer.

接着淀积栅极金属,采用电子束蒸发工艺在栅槽中沉积Ni/Au金属作为栅电极,并在氮气气氛下,温度为40℃的条件下退火10min,形成MIS槽栅。Next, gate metal is deposited, and Ni/Au metal is deposited in the gate groove by electron beam evaporation process as the gate electrode, and annealed at 40°C for 10 minutes in a nitrogen atmosphere to form the MIS groove gate.

继续采用电子束蒸发工艺在上述形成的MIS槽栅旁继续沉积Ni/Au金属,并在氮气气氛下,温度为40℃的条件下退火10min,形成肖特基接触的Γ型栅。Continue to use the electron beam evaporation process to continue to deposit Ni/Au metal next to the MIS groove gate formed above, and anneal for 10 minutes at a temperature of 40°C in a nitrogen atmosphere to form a Γ-shaped gate with Schottky contact.

上述实施例为本发明较佳的实施方式,但本发明的实施方式并不受上述实施例的限制,其他的任何未背离本发明的精神实质与原理下所作的改变、修饰、替代、组合、简化,均应为等效的置换方式,都包含在本发明的保护范围之内。The above-mentioned embodiment is a preferred embodiment of the present invention, but the embodiment of the present invention is not limited by the above-mentioned embodiment, and any other changes, modifications, substitutions, combinations, Simplifications should be equivalent replacement methods, and all are included in the protection scope of the present invention.

Claims (9)

1.一种高耐压双栅极横向HEMT器件,其特征在于,包括:衬底、位于衬底上的GaN缓冲层以及依次层叠于GaN缓冲层上的GaN沟道层、AlN插入层和AlGaN势垒层组成的叠层,还包括p型埋层、位于p型埋层上的p型栅极和位于势垒层上的源极、漏极和Γ型栅;其中,1. A high withstand voltage dual-gate lateral HEMT device, characterized in that it comprises: a substrate, a GaN buffer layer on the substrate, and a GaN channel layer, an AlN insertion layer, and an AlGaN stacked on the GaN buffer layer in sequence The stack of barrier layers also includes a p-type buried layer, a p-type gate positioned on the p-type buried layer, and a source electrode, a drain electrode, and a Γ-type gate positioned on the barrier layer; wherein, 沿厚度方向上,p型埋层自所述缓冲层靠近沟道层的表面朝向缓冲层中远离所述沟道层的一侧延伸一定深度;Along the thickness direction, the p-type buried layer extends to a certain depth from the surface of the buffer layer close to the channel layer toward the side of the buffer layer away from the channel layer; 源极和漏极位于势垒层表面;The source and drain are located on the surface of the barrier layer; 源极和漏极之间还设置一栅槽,该栅槽延伸至势垒层中一定深度,一高介电介质层设置于该栅槽内壁,Γ型栅位于该栅槽中并沿栅槽指向漏极的方向延伸;A gate groove is also arranged between the source and the drain, the gate groove extends to a certain depth in the barrier layer, a high dielectric dielectric layer is arranged on the inner wall of the gate groove, the Γ-shaped gate is located in the gate groove and extends along the gate groove extending in the direction of the drain; 所述栅极与所述叠层之间设置有第一钝化层,所述Γ型栅与源极之间以及所述Γ型栅与漏极之间设置有第二钝化层;A first passivation layer is provided between the gate and the laminate, a second passivation layer is provided between the Γ-shaped gate and the source and between the Γ-shaped gate and the drain; 沿长度方向上,p型埋层自栅极下方延伸至栅槽下方,所述p型埋层在所述缓冲层中离子注入形成,p型埋层与GaN沟道层形成PN结;Along the length direction, the p-type buried layer extends from below the gate to below the gate groove, the p-type buried layer is formed by ion implantation in the buffer layer, and the p-type buried layer forms a PN junction with the GaN channel layer; 在器件工作状态下,p型栅极接正电压,Γ型栅接正电压,源极接负电压,漏极接正电压,所述PN结正向导通;In the working state of the device, the p-type gate is connected to a positive voltage, the Γ-type gate is connected to a positive voltage, the source is connected to a negative voltage, and the drain is connected to a positive voltage, and the PN junction is forward-conducting; 在器件关断状态下,p型栅极接负电压,Γ型栅接负电压,源极接负电压,漏极接正电压,所述PN结反向截止。In the off state of the device, the p-type gate is connected to a negative voltage, the Γ-type gate is connected to a negative voltage, the source is connected to a negative voltage, and the drain is connected to a positive voltage, and the PN junction is reversely cut off. 2.根据权利要求1的所述高耐压双栅极横向HEMT器件,其特征在于,所述p型埋层的掺杂浓度大于等于108cm-3,厚度为70~150nm,长度为3~5μm。2. The high withstand voltage double-gate lateral HEMT device according to claim 1, characterized in that the doping concentration of the p-type buried layer is greater than or equal to 10 8 cm -3 , the thickness is 70-150 nm, and the length is 3 ~5 μm. 3.根据权利要求1的所述高耐压双栅极横向HEMT器件,其特征在于,AlGaN势垒层、高介电介质层和Γ型栅构成MIS Γ型槽栅结构。3. The high withstand voltage double gate lateral HEMT device according to claim 1, characterized in that, the AlGaN barrier layer, the high dielectric layer and the Γ-type gate form a MIS Γ-type groove gate structure. 4.根据权利要求1至3之一的所述高耐压双栅极横向HEMT器件,其特征在于,所述p型埋层选用F+离子源注入缓冲层中形成。4. The high withstand voltage double-gate lateral HEMT device according to any one of claims 1 to 3, wherein the p-type buried layer is formed by implanting an F + ion source into the buffer layer. 5.根据权利要求1至3之一的所述高耐压双栅极横向HEMT器件,其特征在于,所述GaN沟道层的厚度为8~15nm;所述势垒层选用Al组分为1%~3%,厚度为15~30nm 的AlGaN势垒层;所述AlN插入层的厚度为1~2nm。5. The high withstand voltage double-gate lateral HEMT device according to any one of claims 1 to 3, wherein the thickness of the GaN channel layer is 8-15 nm; the Al composition of the barrier layer is 1%~3%, an AlGaN barrier layer with a thickness of 15~30nm; the thickness of the AlN insertion layer is 1~2nm. 6.根据权利要求1至3之一的所述高耐压双栅极横向HEMT器件,其特征在于,所述高介电介质层选用HfO2、Al2O3或TiO2,其厚度为4~6nm。6. The high withstand voltage double-gate lateral HEMT device according to any one of claims 1 to 3, wherein the high dielectric layer is selected from HfO 2 , Al 2 O 3 or TiO 2 , and its thickness is 4 ~6nm. 7.根据权利要求1至3之一的所述高耐压双栅极横向HEMT器件,其特征在于,所述钝化层包括SiNx、SiO2、HfO2或Al2O37 . The high withstand voltage double-gate lateral HEMT device according to claim 1 , wherein the passivation layer comprises SiN x , SiO 2 , HfO 2 or Al 2 O 3 . 8.根据权利要求1至3之一的所述高耐压双栅极横向HEMT器件,其特征在于,所述栅槽靠近所述源极。8 . The high withstand voltage double-gate lateral HEMT device according to claim 1 , wherein the gate groove is close to the source. 9.一种高耐压双栅极横向HEMT器件的制备方法,其特征在于,包括以下步骤:9. A method for preparing a high-voltage double-gate lateral HEMT device, comprising the following steps: 在衬底上外延生长GaN缓冲层;Epitaxial growth of a GaN buffer layer on the substrate; 在所述缓冲层的特定区域离子注入形成p型埋层;ion implantation in a specific region of the buffer layer to form a p-type buried layer; 在所述p型埋层以及缓冲层的表面依次外延生长GaN沟道层、AlN插入层和AlGaN势垒层形成叠层;Epitaxially growing a GaN channel layer, an AlN insertion layer, and an AlGaN barrier layer on the surface of the p-type buried layer and the buffer layer in sequence to form a stack; 刻蚀该叠层的预定区域暴露部分p型埋层区域;Etching a predetermined region of the stack to expose a part of the p-type buried layer region; 在p型埋层和AlGaN势垒层表面沉积钝化层;Depositing a passivation layer on the surface of the p-type buried layer and the AlGaN barrier layer; 刻蚀p型埋层表面的钝化层和势垒层表面的钝化层,形成栅极和源/漏极开孔;Etching the passivation layer on the surface of the p-type buried layer and the passivation layer on the surface of the barrier layer to form gate and source/drain openings; 沉积金属层形成欧姆接触的源/漏极和p型栅极,所述p型栅极与所述叠层之间设置有钝化层;Depositing a metal layer to form an ohmic contact source/drain and a p-type gate, a passivation layer is provided between the p-type gate and the stack; 刻蚀源极和漏极之间的钝化层至势垒层中一定深度形成栅槽;Etching the passivation layer between the source and the drain to a certain depth in the barrier layer to form a gate groove; 在栅槽内壁生长一定厚度的高介电介质层;A high dielectric layer with a certain thickness is grown on the inner wall of the gate groove; 沉积金属层形成肖特基接触的Γ型栅,所述Γ型栅与所述源极和所述漏极之间设置有钝化层;Depositing a metal layer to form a Schottky-contact Γ-shaped gate, a passivation layer is provided between the Γ-shaped gate and the source and the drain; 其中,所述特定区域是指,沿厚度方向上,p型埋层自所述缓冲层靠近沟道层的表面朝向缓冲层中远离所述沟道层的一侧延伸一定深度,沿长度方向上,p型埋层自p型栅极下方延伸至栅槽下方,p型埋层与GaN沟道层形成PN结;Wherein, the specific region refers to that, along the thickness direction, the p-type buried layer extends to a certain depth from the surface of the buffer layer close to the channel layer toward the side of the buffer layer away from the channel layer, and along the length direction , the p-type buried layer extends from under the p-type gate to under the gate groove, and the p-type buried layer forms a PN junction with the GaN channel layer; 在器件工作状态下,p型栅极接正电压,Γ型栅接正电压,源极接负电压,漏极接正电压,所述PN结正向导通;In the working state of the device, the p-type gate is connected to a positive voltage, the Γ-type gate is connected to a positive voltage, the source is connected to a negative voltage, and the drain is connected to a positive voltage, and the PN junction is forward-conducting; 在器件关断状态下,p型栅极接负电压,Γ型栅接负电压,源极接负电压,漏极接正电压,所述PN结反向截止。In the off state of the device, the p-type gate is connected to a negative voltage, the Γ-type gate is connected to a negative voltage, the source is connected to a negative voltage, and the drain is connected to a positive voltage, and the PN junction is reversely cut off.
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Publication number Priority date Publication date Assignee Title
CN113594233B (en) * 2021-08-09 2024-07-19 迪优未来科技(清远)有限公司 A high voltage enhanced HEMT with integrated Schottky diode and preparation method thereof
CN113871477B (en) * 2021-08-30 2024-08-16 瑶芯微电子科技(上海)有限公司 Double heterojunction HEMT device based on gate field plate and source field plate and preparation method thereof
CN113871478B (en) * 2021-09-02 2024-07-30 桂林电子科技大学 A new semiconductor device with P-type channel characteristics based on dual gates
CN113964192A (en) * 2021-09-06 2022-01-21 西安电子科技大学 Non-polar GaN-based Schottky diode and preparation method thereof
CN114038907A (en) * 2021-10-21 2022-02-11 华南师范大学 A kind of double gate control high withstand voltage double channel enhancement type HEMT and preparation method thereof
CN114284355A (en) * 2021-12-27 2022-04-05 西交利物浦大学 Dual-gate MIS-HEMT device, bidirectional switch device and preparation method thereof
CN114883403A (en) * 2022-04-07 2022-08-09 华南理工大学 GaN-based double-channel HEMT and preparation method and application thereof
CN114744039A (en) * 2022-04-13 2022-07-12 华南师范大学 High-withstand-voltage enhanced double-heterojunction gate HEMT and preparation method thereof
CN115566053B (en) * 2022-09-30 2023-10-20 苏州汉骅半导体有限公司 Semiconductor device and preparation method thereof
CN116613194B (en) * 2023-06-09 2025-02-14 河源市众拓光电科技有限公司 HEMT device and preparation method thereof
CN119008670B (en) * 2024-08-09 2025-05-27 北京大学 p-GaN gate gallium nitride high electron mobility transistor with dual gate structure

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104167445A (en) * 2014-08-29 2014-11-26 电子科技大学 GaN-based enhancement/depletion mode heterojunction field effect transistor with buried gate structure
CN106298911A (en) * 2016-10-31 2017-01-04 电子科技大学 A kind of double junction gate gallium nitride heterojunction field effect transistor
CN107658334A (en) * 2016-07-25 2018-02-02 瑞萨电子株式会社 The method of semiconductor devices and manufacture semiconductor devices
CN109004028A (en) * 2018-06-22 2018-12-14 杭州电子科技大学 A GaN Field Effect Transistor with Source Connected P Buried Layer and Drain Field Plate
CN109037325A (en) * 2018-06-22 2018-12-18 杭州电子科技大学 A GaN Field Effect Transistor with PIN Buried Tubes Connected to Electrodes
CN109037326A (en) * 2018-07-18 2018-12-18 大连理工大学 A kind of enhanced HEMT device and preparation method thereof with p type buried layer structure
CN111415986A (en) * 2019-01-07 2020-07-14 半导体元件工业有限责任公司 electronic device

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7915643B2 (en) * 2007-09-17 2011-03-29 Transphorm Inc. Enhancement mode gallium nitride power devices
JP2010206020A (en) * 2009-03-04 2010-09-16 Panasonic Corp Semiconductor device
GB2482308A (en) * 2010-07-28 2012-02-01 Univ Sheffield Super junction silicon devices
US10192980B2 (en) * 2016-06-24 2019-01-29 Cree, Inc. Gallium nitride high-electron mobility transistors with deep implanted p-type layers in silicon carbide substrates for power switching and radio frequency applications and process for making the same
US11430882B2 (en) * 2016-06-24 2022-08-30 Wolfspeed, Inc. Gallium nitride high-electron mobility transistors with p-type layers and process for making the same

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104167445A (en) * 2014-08-29 2014-11-26 电子科技大学 GaN-based enhancement/depletion mode heterojunction field effect transistor with buried gate structure
CN107658334A (en) * 2016-07-25 2018-02-02 瑞萨电子株式会社 The method of semiconductor devices and manufacture semiconductor devices
CN106298911A (en) * 2016-10-31 2017-01-04 电子科技大学 A kind of double junction gate gallium nitride heterojunction field effect transistor
CN109004028A (en) * 2018-06-22 2018-12-14 杭州电子科技大学 A GaN Field Effect Transistor with Source Connected P Buried Layer and Drain Field Plate
CN109037325A (en) * 2018-06-22 2018-12-18 杭州电子科技大学 A GaN Field Effect Transistor with PIN Buried Tubes Connected to Electrodes
CN109037326A (en) * 2018-07-18 2018-12-18 大连理工大学 A kind of enhanced HEMT device and preparation method thereof with p type buried layer structure
CN111415986A (en) * 2019-01-07 2020-07-14 半导体元件工业有限责任公司 electronic device

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
"Mg掺与GaN晶格匹配的InAlN特性研究";尹以安等;《电子元件与材料》;第34卷(第8期);第1-4页 *

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