CN110660851A - High-voltage n-channel HEMT device - Google Patents
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Abstract
一种高压n沟道HEMT器件,属于半导体功率器件技术领域。鉴于在HEMT这类异质结器件上制备超结有较高的工艺难度,本发明针对n沟道HEMT器件提出了一种表面超结结构,通过在器件漂移区表面制备梳指状的p型半导体条块,并将该p型半导体条块与栅极进行电学连接,可在关断条件下实现漂移区沟道大范围耗尽,该耗尽区可耐受较高电压,从而器件击穿特性得以增强。另一方面,由于与栅极连接的梳指状p型表面耐压结构仅覆盖小部分漂移区面积,当器件导通时,与其关联的寄生电阻和寄生电容也相对较小,这使得器件具有相对较好的直流导通特性和高频特性。A high-voltage n-channel HEMT device belongs to the technical field of semiconductor power devices. In view of the high technological difficulty of preparing superjunctions on heterojunction devices such as HEMTs, the present invention proposes a surface superjunction structure for n-channel HEMT devices, by preparing p-type p-type comb fingers on the surface of the device drift region The semiconductor strip, and the p-type semiconductor strip is electrically connected to the gate, can achieve large-scale depletion of the drift region channel under the off condition, and the depletion region can withstand higher voltages, so that the device breaks down Features are enhanced. On the other hand, since the p-type surface withstand voltage structure connected to the gate only covers a small part of the drift region area, when the device is turned on, the parasitic resistance and parasitic capacitance associated with it are also relatively small, which makes the device have Relatively good DC conduction characteristics and high frequency characteristics.
Description
技术领域technical field
本发明属于半导体功率器件技术领域,特别涉及一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件。The invention belongs to the technical field of semiconductor power devices, and particularly relates to an n-channel HEMT device with a p-type surface withstand voltage structure connected to a gate electrode.
背景技术Background technique
在射频、功率集成电路领域,随着电路的集成度不断提高,电路对器件的各项特性要求也越来越高。在传统硅器件性能几乎达到理论极限的情况下,亟需发展一种具有高频、高速、大功率、低噪声和低功耗等性能的新器件,以满足高速大容量计算机和大容量远距离通信的要求,半导体异质结器件应运而生。其中,高电子迁移率晶体管(High ElectronMobility Transistor,HEMT)凭借其超高速、低功耗等优点(尤其在低温下),受到业内人士的广泛关注。In the field of radio frequency and power integrated circuits, with the continuous improvement of the integration of the circuit, the requirements of the circuit on the characteristics of the device are also getting higher and higher. Under the circumstance that the performance of traditional silicon devices has almost reached the theoretical limit, it is urgent to develop a new device with high frequency, high speed, high power, low noise and low power consumption to meet the needs of high-speed and large-capacity computers and large-capacity long-distance Communication requirements, semiconductor heterojunction devices came into being. Among them, high electron mobility transistor (High Electron Mobility Transistor, HEMT) has received extensive attention of the industry due to its advantages such as ultra-high speed and low power consumption (especially at low temperature).
HEMT的基本结构就是一个调制掺杂异质结,以n沟道HEMT器件为例,基本的HEMT器件结构如图1所示,自下而上依次为:衬底、缓冲层、势垒层和电极。衬底(Substrate)上外延生长缓冲层(Buffer),然后在缓冲层上生长势垒层(Barrier),该势垒层可以根据具体情况选择掺杂与否,而在势垒层上分布着源极(Source)、栅极(Gate)和漏极(Drain),源极和漏极一般通过合金化方法实现与二维导电沟道的欧姆接触,而栅极与势垒层形成肖特基接触。在缓冲层和势垒层接触形成异质结界面进一步形成的三角形势阱中存在有二维电子气(2-DEG),由于该电子气远离表面态,同时在空间上和处在势垒层的杂质中心是分离的,不受电离杂质散射的影响,所以有高的迁移率,通过栅电压可以控制三角型势阱的深度和宽度,从而可以改变二维电子气的浓度,以达到控制HEMT电流的目的。另外,如何提高器件的击穿电压是本领域的研究重点之一。因为HEMT器件在工作状态下,栅极和漏极边缘形成的电场峰会降低器件的击穿电压,进而限制器件的最大输出功率。因此,为了将HEMT器件作为功率器件应用,高压HEMT器件的研究意义重大。有鉴于此,目前已经发展出多种耐压结构,其中场板结构是最常见的一种。但是,场板结构对于工艺精度要求较高,且其对HEMT的击穿电压提升有限,这限制了其在实际中的应用。另外,不乏研究者考虑借鉴LDMOS中的超结结构,提出在HEMT中引入类似的超结。但是由于HEMT是一种异质结外延器件,在工艺上比传统Si基器件有更多限制,这造成现有针对HEMT的超结结构实际上是一种多层外延结构,工艺难度较大,同时耐压提升效果也有限。针对这一现状,发展一种适用于HEMT的类似于超结的新型耐压结构十分必要。The basic structure of HEMT is a modulated doped heterojunction. Taking an n-channel HEMT device as an example, the basic HEMT device structure is shown in Figure 1. From bottom to top, it is: substrate, buffer layer, barrier layer and electrode. The buffer layer (Buffer) is epitaxially grown on the substrate, and then the barrier layer (Barrier) is grown on the buffer layer. The barrier layer can be doped or not according to the specific situation, and the source is distributed on the barrier layer. Source, gate and drain, the source and drain generally achieve ohmic contact with the two-dimensional conductive channel by alloying, while the gate and the barrier layer form Schottky contact . There is a two-dimensional electron gas (2-DEG) in the triangular potential well formed by the contact between the buffer layer and the barrier layer to form a heterojunction interface. Since the electron gas is far away from the surface state, it is spatially and in the barrier layer. The impurity center is separated and is not affected by the scattering of ionized impurities, so it has high mobility, and the depth and width of the triangular potential well can be controlled by the gate voltage, so that the concentration of the two-dimensional electron gas can be changed to achieve control HEMT purpose of current. In addition, how to improve the breakdown voltage of the device is one of the research focuses in this field. Because the HEMT device is in the working state, the electric field formed at the gate and drain edges will reduce the breakdown voltage of the device, thereby limiting the maximum output power of the device. Therefore, in order to apply HEMT devices as power devices, research on high-voltage HEMT devices is of great significance. In view of this, a variety of pressure-resistant structures have been developed, of which the field plate structure is the most common one. However, the field plate structure requires high process precision, and its breakdown voltage improvement of HEMT is limited, which limits its practical application. In addition, many researchers consider borrowing the superjunction structure in LDMOS and propose to introduce a similar superjunction in HEMT. However, since HEMT is a heterojunction epitaxial device, it has more limitations in process than traditional Si-based devices, which causes the existing superjunction structure for HEMT to be a multi-layer epitaxial structure, which is difficult to process. At the same time, the effect of pressure resistance improvement is also limited. In view of this situation, it is necessary to develop a new type of pressure-resistant structure similar to superjunction suitable for HEMT.
发明内容SUMMARY OF THE INVENTION
针对现有技术中针对HEMT器件提出耐压结构存在工艺难度大,击穿电压提升有限等缺陷,本发明提出了一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件。In view of the defects in the prior art that the withstand voltage structure proposed for HEMT devices is difficult to process and the breakdown voltage is limited, the present invention proposes an n-channel with a comb-finger p-type surface withstand voltage structure connected to the gate. HEMT device.
为强化n沟道HEMT器件的耐压特性,本发明提供如下技术方案:In order to strengthen the withstand voltage characteristics of the n-channel HEMT device, the present invention provides the following technical solutions:
一种高压n沟道HEMT器件,包括:衬底1、设置在衬底1上表面的缓冲层2,设置在缓冲层2上表面的势垒层3和设置在势垒层3上表面的栅极4、源极5和漏极6;缓冲层2和势垒层3在其接触界面形成异质结,在所述异质结界面上具有二维导电沟道9;所述源极5和漏极6分别设置在势垒层3上两侧且均与所述二维导电沟道9形成欧姆接触;所述栅极4设置在源极5与漏极6之间的势垒层3上且与所述势垒层3形成肖特基接触;其特征在于,A high-voltage n-channel HEMT device, comprising: a
栅极4与漏极6之间的势垒层3上具有表面耐压结构,所述表面耐压结构包括多个梳指状排列的p型半导体块7,其中每个p型半导体块7沿栅漏方向延伸;梳指状排列的p型半导体块7与所述栅极4进行电连接,而与漏极6互不接触。There is a surface withstand voltage structure on the
进一步地,至少在相邻p型半导体块7之间填充有绝缘介质8。Further, an
更进一步地,所述绝缘介质8与漏极6接触或者隔离。Furthermore, the
作为一种实施方式,设置在相邻p型半导体块7之间的绝缘介质8的两端与p型半导体块7齐平,即p型半导体块7和绝缘介质8的首尾沿p型半导体块7排列方向齐平。As an embodiment, both ends of the
作为一种实施方式,设置在相邻p型半导体块7之间的绝缘介质8可以沿p型半导体块7排列方向相互连通半包围p型半导体块7,所述绝缘介质8与漏极6相隔离。As an embodiment, the
作为一种实施方式,设置在相邻p型半导体块7之间的绝缘介质8可以向所述漏极6方向延伸,并且完全填充p型半导体块7与漏极6之间间隙,即绝缘介质8可以沿p型半导体块7排列方向相互连通半包围p型半导体块7,所述绝缘介质8与漏极6相接触。As an embodiment, the
进一步地,所述表面耐压结构可与场板等耐压结构联合使用。Further, the surface pressure-resistant structure can be used in combination with a pressure-resistant structure such as a field plate.
本发明的工作原理为:The working principle of the present invention is:
由于在栅极与漏极之间增加与栅极连接的梳指状分布的p型表面耐压结构,p型半导体块能够抬高势垒层的能带,使异质结界面处的三角形势阱抬升,耗尽或部分耗尽沟道中的二维电子气。The p-type semiconductor block can raise the energy band of the barrier layer due to the p-type surface withstand voltage structure with a comb-finger distribution connected to the gate between the gate and the drain, making the triangular potential at the interface of the heterojunction. The well lifts up, depleting or partially depleting the two-dimensional electron gas in the channel.
当器件关断时,当漏极上正电压增大时,与栅极接触的梳指状p型半导体块会被逐渐耗尽,这一耗尽区中的固定负电荷会对二维导电沟道中的二维电子气有耗尽作用。在这一过程中,各个p型半导体块下方的二维电子气会首先耗尽。随着漏极正电压进一步增大,与栅极连接的梳指状p型表面耐压结构的梳指间隙区域下方的二维电子气也会被逐步耗尽。When the device is turned off, when the positive voltage on the drain increases, the p-type p-type semiconductor block in contact with the gate will be gradually depleted, and the fixed negative charge in this depletion region will affect the two-dimensional conduction channel. The two-dimensional electron gas in the channel has a depletion effect. During this process, the two-dimensional electron gas under each p-type semiconductor block is first depleted. With the further increase of the positive voltage of the drain, the two-dimensional electron gas under the finger gap region of the p-type surface withstand voltage structure connected to the gate will be gradually depleted.
如果要漂移区的所有半导体结构在漏压足够大时完全耗尽,需要满足电离生成的固定正电荷总量等于固定负电荷总量。根据这一原理可适当设置梳指状p型表面耐压结构的掺杂浓度,使得与栅极连接的梳指状p型半导体块与梳指间隙区域下方的二维电子气同时耗尽。这样,HEMT器件的源漏之间的表面耐压结构及其下方延伸区域形成了一个较大的耗尽区,该耗尽区可以承受较高的正电压,其直接结果是器件耐压得以提高。If all the semiconductor structures in the drift region are to be completely depleted when the drain voltage is large enough, the total amount of fixed positive charges generated by ionization needs to be equal to the total amount of fixed negative charges. According to this principle, the doping concentration of the comb-finger p-type surface withstand voltage structure can be appropriately set, so that the comb-finger p-type semiconductor block connected to the gate and the two-dimensional electron gas under the interdigital gap region are simultaneously depleted. In this way, the surface withstand voltage structure between the source and drain of the HEMT device and its extension area below form a larger depletion region, which can withstand a higher positive voltage, and the direct result is that the device withstand voltage is improved. .
当器件导通时,通过金属线与栅极连接的梳指状p型表面耐压结构的梳指间隙区域下方的二维电子气并未受到多个p型半导体块的影响,具有较高的电子浓度,因而是良好的导电通路,这保证了器件导通电阻不会因采用耐压结构而显著劣化。另外,在器件设计时,与栅极连接的梳指状p型表面耐压结构仅覆盖小部分漂移区面积,这样表面耐压结构所引入的寄生电容也相对较小。基于该耐压结构的器件具有较小的导通电阻和附加电容,这使得其具有较好的高频特性。When the device is turned on, the two-dimensional electron gas under the interdigital gap region of the comb-finger p-type surface withstand voltage structure connected to the gate through the metal wire is not affected by the multiple p-type semiconductor blocks, and has a high The electron concentration is thus a good conduction path, which ensures that the on-resistance of the device will not be significantly deteriorated by the use of a withstand voltage structure. In addition, when designing the device, the p-type surface withstand voltage structure connected to the gate only covers a small part of the drift region area, so that the parasitic capacitance introduced by the surface withstand voltage structure is relatively small. The device based on this withstand voltage structure has smaller on-resistance and additional capacitance, which makes it have better high-frequency characteristics.
本发明的有益效果为:The beneficial effects of the present invention are:
本发明提出的HEMT器件在保证高击穿电压的同时实现了较小的导通电阻和耐压结构寄生电容,适用于对于输出功率和工作频率均有较高要求的应用领域。The HEMT device proposed by the invention realizes smaller on-resistance and parasitic capacitance of the withstand voltage structure while ensuring high breakdown voltage, and is suitable for application fields with higher requirements for output power and operating frequency.
附图说明Description of drawings
图1为传统的n沟道HEMT器件的立体结构示意图。FIG. 1 is a schematic three-dimensional structure diagram of a conventional n-channel HEMT device.
图2为本发明提供一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件结构的具体实现方式之一。FIG. 2 is one of the specific implementation manners of the n-channel HEMT device structure provided by the present invention having a p-type surface withstand voltage structure connected to the gate.
图3为本发明提供一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件结构的具体实现方式之二。FIG. 3 is a second specific implementation manner of an n-channel HEMT device structure with a comb-finger p-type surface withstand voltage structure connected to the gate according to the present invention.
图4为本发明提供一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件结构的具体实现方式之二的俯视图。FIG. 4 is a top view of the second specific implementation manner of an n-channel HEMT device structure with a p-type surface withstand voltage structure connected to the gate according to the present invention.
图5为本发明提供一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件结构的具体实现方式之三。FIG. 5 is a third specific implementation manner of an n-channel HEMT device structure with a comb-finger p-type surface withstand voltage structure connected to the gate according to the present invention.
图6为本发明提供一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件结构的具体实现方式之三的俯视图。FIG. 6 is a top view of the third specific implementation manner of an n-channel HEMT device structure with a comb-finger p-type surface withstand voltage structure connected to the gate according to the present invention.
图7为本发明提供一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件结构的具体实现方式之四。FIG. 7 is a fourth specific implementation manner of an n-channel HEMT device structure with a comb-finger p-type surface withstand voltage structure connected to the gate according to the present invention.
图8为本发明提供一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件结构的具体实现方式之四的俯视图。FIG. 8 is a plan view of the fourth specific implementation manner of the n-channel HEMT device structure with the p-type surface withstand voltage structure connected to the gate according to the present invention.
图9为本发明提供一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件中梳指状分布的多个p型半导体块下方形成耗尽区的立体结构示意图。9 is a three-dimensional schematic diagram of a depletion region formed under a plurality of p-type semiconductor blocks distributed in a comb-finger shape in an n-channel HEMT device with a p-type surface withstand voltage structure connected to the gate provided by the present invention .
图10为本发明提供一种具有与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件中梳指状分布的多个p型半导体块下方的耗尽区向多个p型半导体块间隙下方区域扩展并最终形成近似为矩形的大片耗尽的立体结构示意图。FIG. 10 is an illustration of a depletion region under a plurality of p-type semiconductor blocks distributed in a comb-finger shape in an n-channel HEMT device with a p-type surface withstand voltage structure connected to the gate provided by the present invention to a plurality of p-type semiconductor blocks. Schematic diagram of the three-dimensional structure of the expansion of the region under the gap of the type semiconductor block and finally forming an approximately rectangular large-scale depletion.
图11为本发明提供的在衬底上表面形成GaN缓冲层的立体结构示意图。FIG. 11 is a schematic three-dimensional structure diagram of forming a GaN buffer layer on the upper surface of the substrate provided by the present invention.
图12为本发明提供的在GaN缓冲层上表面生长AlGaN势垒层并形成二维导电沟道的立体结构示意图。FIG. 12 is a schematic three-dimensional structure diagram of growing an AlGaN barrier layer on the upper surface of the GaN buffer layer and forming a two-dimensional conductive channel provided by the present invention.
图13本发明提供的在AlGaN势垒层上表面制作与二维导电沟道形成欧姆接触的源极和漏极的立体结构示意图。13 is a schematic three-dimensional structural diagram of the source and drain electrodes that form ohmic contact with the two-dimensional conductive channel on the upper surface of the AlGaN barrier layer provided by the present invention.
图14本发明提供的在AlGaN势垒层上表面制作与AlGaN势垒层形成肖特基接触的栅极的立体结构示意图。FIG. 14 is a schematic three-dimensional structural diagram of the gate electrode formed on the upper surface of the AlGaN barrier layer to form Schottky contact with the AlGaN barrier layer provided by the present invention.
图15为本发明提供的在栅极与漏极之间的AlGaN势垒层的上表面覆盖有与漏极保持一定间隙而与栅极电学连接的p型GaN层的立体结构示意图。15 is a schematic three-dimensional structural diagram of a p-type GaN layer electrically connected to the gate while maintaining a certain gap with the drain and covering the upper surface of the AlGaN barrier layer between the gate and the drain provided by the present invention.
图16为本发明提供的刻蚀p型GaN层形成多个p型GaN块的立体结构示意图。FIG. 16 is a schematic three-dimensional structural diagram of etching a p-type GaN layer to form a plurality of p-type GaN blocks provided by the present invention.
图17为本发明提供的在与栅极连接的梳指状p型表面耐压结构上方靠近栅极一侧淀积薄绝缘介质并与栅极相连的立体结构示意图。FIG. 17 is a schematic three-dimensional structural diagram of depositing a thin insulating medium on the side of the p-type surface withstanding voltage structure connected to the gate, which is close to the gate, and connected to the gate, provided by the present invention.
图18为本发明提供的在栅极与薄绝缘介质上方淀积金属场板的立体结构示意图。FIG. 18 is a schematic three-dimensional structural diagram of depositing a metal field plate on the gate electrode and the thin insulating medium provided by the present invention.
图中:1为衬底,2为缓冲层,3为势垒层,4为栅极,5为源极,6为漏极,7为p型半导体块,8为绝缘介质,9为二维导电沟道,10为GaN缓冲层,11为AlGaN势垒层,12为p型GaN块。In the figure: 1 is the substrate, 2 is the buffer layer, 3 is the barrier layer, 4 is the gate, 5 is the source, 6 is the drain, 7 is a p-type semiconductor block, 8 is an insulating medium, and 9 is a two-dimensional Conductive channel, 10 is a GaN buffer layer, 11 is an AlGaN barrier layer, and 12 is a p-type GaN bulk.
具体实施方式Detailed ways
为了使得所属领域技术人员能够更加清楚本发明方案及原理,下面结合附图和具体实施例进行详细描述。本发明的内容不局限于任何具体实施例,也不代表是最佳实施例,本领域技术人员所熟知的一般替代也涵盖在本发明的保护范围内。In order to make the solutions and principles of the present invention clearer to those skilled in the art, the following detailed description is given in conjunction with the accompanying drawings and specific embodiments. The content of the present invention is not limited to any specific embodiment, nor does it represent the best embodiment, and general substitutions known to those skilled in the art are also included within the protection scope of the present invention.
实施例:Example:
本发明提供一种含与栅极连接的梳指状p型表面耐压结构的n沟道HEMT器件,包括衬底1、缓冲层2、势垒层3、栅极4、源极5和漏极6,衬底1上依次设置缓冲层2和势垒层3,势垒层3与缓冲层2接触的界面处形成二维导电沟道9;源极5和漏极6分别设置在HEMT器件两侧且均与二维导电沟道9形成欧姆接触;源极5与漏极6之间设置栅极4,且栅极4位于势垒层3上与势垒层3形成肖特基接触;栅极4与漏极6之间的势垒层3上设置有表面耐压结构,所述表面耐压结构包括多个梳指状排列的p型半导体块7,其中每个p型半导体块7沿栅漏方向延伸;梳指状排列的p型半导体块7与所述栅极4进行电连接,而与漏极6互不接触。The present invention provides an n-channel HEMT device with a comb-finger p-type surface withstand voltage structure connected to a gate, comprising a substrate 1, a buffer layer 2, a barrier layer 3, a gate 4, a source 5 and a drain Electrode 6, a buffer layer 2 and a barrier layer 3 are sequentially arranged on the substrate 1, and a two-dimensional conductive channel 9 is formed at the interface between the barrier layer 3 and the buffer layer 2; the source electrode 5 and the drain electrode 6 are respectively arranged on the HEMT device Both sides are in ohmic contact with the two-dimensional conductive channel 9; a gate electrode 4 is provided between the source electrode 5 and the drain electrode 6, and the gate electrode 4 is located on the barrier layer 3 to form Schottky contact with the barrier layer 3; The barrier layer 3 between the gate 4 and the drain 6 is provided with a surface withstand voltage structure, and the surface withstand voltage structure includes a plurality of p-type semiconductor blocks 7 arranged in a comb finger shape, wherein each p-type semiconductor block 7 Extending along the gate-drain direction; the p-type semiconductor blocks 7 arranged in the form of comb fingers are electrically connected to the gate 4 , but are not in contact with the drain 6 .
由于与栅极连接的梳指状p型表面耐压结构之间存在间隙,使得多个p型半导体块7没有全部覆盖势垒层3上方的全部区域,使得没有被覆盖的区域下方的二维电子气不受到多个p型半导体块7的耗尽作用的影响,从而减小导通电阻,并减小了引入的附加电容。Due to the existence of gaps between the p-type surface withstand voltage structures connected to the gate, the plurality of p-type semiconductor blocks 7 do not fully cover the entire area above the
一些实施例中,可以在多个p型半导体块7之间填充绝缘介质8,如图3所示,多个p型半导体块7与介质块8互相交替,绝缘介质8可以向漏极6方向延伸,如图5和图7所示;多个p型半导体块7与漏极6不直接连接,p型半导体块7与漏极6之间可以如图2所示不设置任何介质,或如图5所示将绝缘介质8延伸但不接触漏极6,也可以如图7所示将绝缘介质8延伸至与漏极6接触,使得多个p型半导体块7与漏极6之间通过绝缘介质8间接连接。In some embodiments, an insulating
下面结合图9和图10详细说明本发明的工作过程。The working process of the present invention will be described in detail below with reference to FIG. 9 and FIG. 10 .
对于传统的n沟道HEMT器件,当漏极施加大的正电压时,由于栅漏之间的漂移区难以完全耗尽,造成电压主要降落在栅极边缘附近,这就会形成很大的电场峰,使得器件击穿。For conventional n-channel HEMT devices, when a large positive voltage is applied to the drain, it is difficult to completely deplete the drift region between the gate and drain, causing the voltage to mainly drop near the gate edge, which creates a large electric field peak, causing the device to break down.
本发明在n沟道HEMT器件栅极4与漏极6之间的势垒层3表面设置呈梳指状分布的多个p型半导体块7构成的表面耐压结构。在器件关断时,随着漏极上正电压的增大,p型半导体块7下方的二维电子气会率先耗尽;当漏极正电压足够大时,各个p型半导体块7下方的耗尽区会向四周扩展,使得整个梳指状表面耐压结构间隙下方区域的二维电子气也被耗尽,耗尽区逐渐扩展直到相连形成一个近似为矩形的大片耗尽区,在此过程中,p型半导体块7也逐步耗尽。由于p型半导体块掺杂浓度适当,可以保证其与漂移区二维电子气几乎同时耗尽,这如图10所示。基于该耗尽区可以起到耐压的作用,使得原本集中降落在栅极边缘的电压分布区域得到极大的扩展,使栅漏之间的漂移区电场峰得到有效抑制,从而提高器件的击穿电压,使器件的耐压能力得以大幅提升。In the present invention, a surface withstand voltage structure composed of a plurality of p-type semiconductor blocks 7 distributed in a comb-finger shape is arranged on the surface of the
如图11至图16所示给出了一种制造本发明的n沟道HEMT器件的制造方法,本实施例以GaN基n沟道HEMT器件为例,结合附图详细描述本实施例中GaN基n沟道HEMT器件的制造过程,包括如下步骤:As shown in FIG. 11 to FIG. 16, a manufacturing method for manufacturing an n-channel HEMT device of the present invention is given. In this embodiment, a GaN-based n-channel HEMT device is taken as an example, and the GaN-based HEMT device in this embodiment is described in detail with reference to the accompanying drawings. The manufacturing process of the base n-channel HEMT device includes the following steps:
步骤1、在衬底1上生长GaN缓冲层10,如图11所示。
步骤2、在GaN缓冲层10上生长AlGaN势垒层11,GaN缓冲层10与AlGaN势垒层11界面处形成二维导电沟道9,二维导电沟道9中存在二维电子气,如图12所示。
步骤3、进行台面刻蚀制作器件有源区,然后在台面表面制备源极5和漏极6,并且使得源极5和漏极6分别与GaN缓冲层10和AlGaN势垒层11界面处的二维导电沟道9形成欧姆接触,如图13所示。
步骤4、在AlGaN势垒层11上方制作和AlGaN势垒层11肖特基接触的栅极4,如图14所示。
步骤5、在AlGaN势垒层11上方栅极4与漏极6之间区域覆盖p型GaN层到适合的厚度,如图15所示。
步骤6、图形化刻蚀p型GaN层至AlGaN势垒层11表面,使得在AlGaN势垒层11上方形成多个均匀分布且沿着栅漏方向延伸并与栅极4电学连接的p型GaN块12,p型GaN块12与漏极6不直接接触,后续工艺与现有HEMT制作工艺一致,最终得到本实施例的GaN基HEMT器件,如图16所示。
更近一步地,结合图17、18进一步阐明该p型表面耐压结构与场板结构联合使用的n沟道HEMT器件制造方法。Furthermore, with reference to FIGS. 17 and 18 , the fabrication method of the n-channel HEMT device using the p-type surface withstand voltage structure in combination with the field plate structure is further clarified.
本实施例以GaN基n沟道HEMT器件为例,结合附图详细描述本实施例中GaN基n沟道HEMT器件的制造过程,该器件结合应用了金属场板和梳指状表面耐压结构,器件制备包括如下步骤:In this embodiment, a GaN-based n-channel HEMT device is taken as an example, and the manufacturing process of the GaN-based n-channel HEMT device in this embodiment is described in detail with reference to the accompanying drawings. The device combines a metal field plate and a comb-finger surface withstand voltage structure. , the device preparation includes the following steps:
步骤1、在衬底1上生长GaN缓冲层10,如图11所示。
步骤2、在GaN缓冲层10上生长AlGaN势垒层11,GaN缓冲层10与AlGaN势垒层11界面处形成二维导电沟道9,二维导电沟道9中存在二维电子气,如图12所示。
步骤3、进行台面刻蚀制作器件有源区,然后在台面表面制备源极5和漏极6,并且使得源极5和漏极6分别与GaN缓冲层10和AlGaN势垒层11界面处的二维导电沟道9形成欧姆接触,如图13所示。
步骤4、在AlGaN势垒层11上方制作和AlGaN势垒层11肖特基接触的栅极4,如图14所示。
步骤5、在AlGaN势垒层11上方栅极4与漏极6之间区域覆盖p型GaN层到适合的厚度,如图15所示。
步骤6、图形化刻蚀p型GaN层至AlGaN势垒层11表面,使得在AlGaN势垒层11上方形成多个均匀分布且沿着栅漏方向延伸并与栅极4电学连接的p型GaN块12,p型GaN块12与漏极6不直接接触,如图16所示。
步骤7、在栅极4与漏极6之间靠近栅极4一侧的位置上淀积一层薄绝缘介质8,该绝缘介质8与栅极4接触,如图17所示。Step 7: Deposit a thin
步骤8、在栅极4和薄绝缘介质8的上方淀积金属场板,后续工艺与现有HEMT制作工艺一致,最终得到本实施例的GaN基HEMT器件,如图18所示。
本领域的普通技术人员可以根据本发明公开的这些技术启示做出各种不脱离本发明实质的其它各种具体变形和组合,这些变形和组合仍然在本发明的保护范围内。Those skilled in the art can make various other specific modifications and combinations without departing from the essence of the present invention according to the technical teaching disclosed in the present invention, and these modifications and combinations still fall within the protection scope of the present invention.
上述实施例仅例示性说明本发明的原理及其功效,而非用于限制本发明。任何熟悉此技术的人士皆可在不违背本发明的精神及范畴下,对上述实施例进行修饰或改变。因此,凡所属技术领域中具有通常知识者在未脱离本发明所揭示的精神与技术思想下所完成的一切等效修饰或改变,仍应由本发明的权利要求所涵盖。The above-mentioned embodiments merely illustrate the principles and effects of the present invention, but are not intended to limit the present invention. Anyone skilled in the art can modify or change the above embodiments without departing from the spirit and scope of the present invention. Therefore, all equivalent modifications or changes made by those with ordinary knowledge in the technical field without departing from the spirit and technical idea disclosed in the present invention should still be covered by the claims of the present invention.
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Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN111640671A (en) * | 2020-06-03 | 2020-09-08 | 上海新傲科技股份有限公司 | Gallium nitride-based high electron mobility transistor and preparation method thereof |
CN113394283A (en) * | 2021-06-25 | 2021-09-14 | 电子科技大学 | High-voltage HEMT device with composite layer structure |
CN113410281A (en) * | 2020-03-16 | 2021-09-17 | 电子科技大学 | P-channel LDMOS device with surface voltage-resistant structure and preparation method thereof |
CN113410298A (en) * | 2020-03-16 | 2021-09-17 | 电子科技大学 | N-channel LDMOS device with surface voltage-resistant structure and preparation method thereof |
CN114203797A (en) * | 2021-11-29 | 2022-03-18 | 西安电子科技大学 | Super junction gallium oxide transistor based on heterojunction and manufacturing method and application thereof |
CN115411105A (en) * | 2022-08-30 | 2022-11-29 | 杭州云镓半导体科技有限公司 | A GaN device with p-GaN field plate and its manufacturing method |
CN117810249A (en) * | 2024-02-23 | 2024-04-02 | 深圳天狼芯半导体有限公司 | P-type gate HEMT device and preparation method thereof |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20130082277A1 (en) * | 2011-09-30 | 2013-04-04 | Samsung Electro-Mechanics Co., Ltd. | Nitride semiconductor device and manufacturing method thereof |
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 |
US20180301527A1 (en) * | 2014-03-19 | 2018-10-18 | Kabushiki Kaisha Toshiba | Semiconductor device |
CN109461774A (en) * | 2018-11-01 | 2019-03-12 | 电子科技大学 | A kind of HEMT device of the block containing high dielectric coefficient medium |
-
2019
- 2019-10-08 CN CN201910948506.8A patent/CN110660851A/en active Pending
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20130082277A1 (en) * | 2011-09-30 | 2013-04-04 | Samsung Electro-Mechanics Co., Ltd. | Nitride semiconductor device and manufacturing method thereof |
US20180301527A1 (en) * | 2014-03-19 | 2018-10-18 | 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 |
CN109461774A (en) * | 2018-11-01 | 2019-03-12 | 电子科技大学 | A kind of HEMT device of the block containing high dielectric coefficient medium |
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN113410281A (en) * | 2020-03-16 | 2021-09-17 | 电子科技大学 | P-channel LDMOS device with surface voltage-resistant structure and preparation method thereof |
CN113410298A (en) * | 2020-03-16 | 2021-09-17 | 电子科技大学 | N-channel LDMOS device with surface voltage-resistant structure and preparation method thereof |
CN111640671A (en) * | 2020-06-03 | 2020-09-08 | 上海新傲科技股份有限公司 | Gallium nitride-based high electron mobility transistor and preparation method thereof |
CN111640671B (en) * | 2020-06-03 | 2023-04-18 | 上海新傲科技股份有限公司 | Gallium nitride-based high electron mobility transistor and preparation method thereof |
CN113394283A (en) * | 2021-06-25 | 2021-09-14 | 电子科技大学 | High-voltage HEMT device with composite layer structure |
CN113394283B (en) * | 2021-06-25 | 2023-04-14 | 电子科技大学 | High Voltage HEMT Devices with Composite Layer Structure |
CN114203797A (en) * | 2021-11-29 | 2022-03-18 | 西安电子科技大学 | Super junction gallium oxide transistor based on heterojunction and manufacturing method and application thereof |
CN115411105A (en) * | 2022-08-30 | 2022-11-29 | 杭州云镓半导体科技有限公司 | A GaN device with p-GaN field plate and its manufacturing method |
CN115411105B (en) * | 2022-08-30 | 2023-12-15 | 杭州云镓半导体科技有限公司 | GaN device with P-GaN field plate and manufacturing method |
CN117810249A (en) * | 2024-02-23 | 2024-04-02 | 深圳天狼芯半导体有限公司 | P-type gate HEMT device and preparation method thereof |
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