CN100495682C - A Method for Monolithic Integration of RTD and HEMT Using Dry Etching Technology - Google Patents
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Abstract
一种采用干法刻蚀技术实现RTD与HEMT单片集成的方法,包括如:在衬底上依次生长典型的HEMT材料结构和RTD材料结构;光刻出RTD发射区的图形制备AuGeNi金属层,形成RTD金属发射极;光刻,形成有源区;光刻出HEMT的源漏电极;高温退火;光刻出HEMT栅槽图形刻蚀掉部分重掺杂帽层;在器件表面淀积生长一层钝化介质层;光刻出HEMT的栅电极图形生成TiPtAu金属作为HEMT器件的栅电极;光刻出引线孔;光刻出引线互连区域,蒸发或溅射厚TiAlTiAu金属电极,去胶剥离。
A method for realizing monolithic integration of RTD and HEMT by using dry etching technology, including such as: growing a typical HEMT material structure and RTD material structure sequentially on a substrate; photoetching out the pattern of the RTD emission region to prepare an AuGeNi metal layer, Form the RTD metal emitter; photolithography, form the active region; photolithography out the source and drain electrodes of the HEMT; high temperature annealing; layer passivation dielectric layer; photoetching the gate electrode pattern of HEMT to generate TiPtAu metal as the gate electrode of HEMT device; photoetching the lead hole; photoetching the lead interconnection area, evaporating or sputtering thick TiAlTiAu metal electrode, peeling off the glue .
Description
技术领域 technical field
本发明属于半导体技术领域,特别是在III-V族衬底上制备共振隧穿二极管与晶体管单片集成电路工艺方面。The invention belongs to the technical field of semiconductors, in particular to the technology of preparing resonant tunneling diodes and transistor monolithic integrated circuits on III-V substrates.
背景技术 Background technique
自上世纪六十年代硅大规模集成电路实现产业化大生产以来,一直遵循摩尔定律,通过特征尺寸的缩小改善电路性能,实现更高的集成度,更快的速度以及更低的功耗。正由于此,上世纪末,Intel公司将集成度和性能都达到空前高水平的奔腾处理器芯片和个人计算机送到用户手中。目前MOSFET特征尺寸已达到45nm,而后随着特征尺寸向纳米尺度靠近,量子效应逐渐显现并占据主导地位,一些诸如金属互连、电流隧穿以及功耗等问题日益突出,将极大阻碍其向前发展的进程,按比例缩小的办法继续将更加困难。理论分析指出20-30nm可能是CMOS器件特征尺寸的物理极限,这不仅是指量子尺寸效应对现有器件特性影响所带来的物理限制和光刻技术的限制问题,更重要的是将受材料自身性质的限制。Since the industrialized mass production of silicon large-scale integrated circuits in the 1960s, Moore's Law has been followed to improve circuit performance through the reduction of feature size, achieving higher integration, faster speed and lower power consumption. Because of this, at the end of the last century, Intel delivered Pentium processor chips and personal computers with unprecedented levels of integration and performance to users. At present, the characteristic size of MOSFET has reached 45nm, and then as the characteristic size approaches the nanometer scale, quantum effects gradually appear and dominate, and some problems such as metal interconnection, current tunneling and power consumption are becoming more and more prominent, which will greatly hinder its development. Proceeding with the development process, the scaling down approach will be more difficult to continue. Theoretical analysis points out that 20-30nm may be the physical limit of the feature size of CMOS devices. This not only refers to the physical limitations and lithography technology limitations brought about by the influence of quantum size effects on the characteristics of existing devices, but more importantly, it will be affected by the material limitations of its own nature.
为了减小器件特征尺寸,从而达到整体提升器件性能的目的,人们希望找到其它的方法来避开上述困难。在设法抑制短沟道效应的实验中发现,当特征尺寸接近物理极限时,基于量子隧道效应的隧道效应器件比传统MOSFET好。换言之,基于隧道效应器件的量子器件比MOSFET更适合于纳米电子学的发展。In order to reduce the feature size of the device, thereby achieving the purpose of improving the performance of the device as a whole, people hope to find other methods to avoid the above-mentioned difficulties. In experiments that sought to suppress short-channel effects, it was found that tunneling devices based on quantum tunneling outperform conventional MOSFETs when the feature size approaches the physical limit. In other words, quantum devices based on tunneling devices are more suitable for the development of nanoelectronics than MOSFETs.
共振隧穿二极管(RTD)是一种利用纳米尺度上的隧穿效应实现开关特性的量子器件。作为率先实用化以及当前发展最成熟的纳米电子器件,RTD峰谷转换频率的理论值高达2.5THz,实际器件振荡频率达到712GHz,实际器件开关时间达到1.5ps。由于它的高速度与低功耗,同时其所特有的微分负阻特性可以简化电路的复杂性,吸引着人们的关注。RTD最主要的优点,一是它所具有的、多重稳态特性可以用来制作出十分紧凑的电路,二是它的本征速度可进入GHz范畴。RTD如今已经在诸如A/D和D/A转换器、触发器、时钟量化器、分频器、移位寄存器、加法器、存储器、可编程逻辑门等许多方面得到了应用。Resonant tunneling diode (RTD) is a quantum device that utilizes the tunneling effect on the nanometer scale to achieve switching characteristics. As the first practical and currently most mature nanoelectronic device, the theoretical value of RTD peak-to-valley transition frequency is as high as 2.5THz, the actual device oscillation frequency reaches 712GHz, and the actual device switching time reaches 1.5ps. Because of its high speed and low power consumption, and its unique differential negative resistance characteristics can simplify the complexity of the circuit, it attracts people's attention. The main advantage of RTD is that its multiple steady-state characteristics can be used to make very compact circuits, and its intrinsic speed can enter the GHz range. RTDs are used today in many applications such as A/D and D/A converters, flip-flops, clock quantizers, frequency dividers, shift registers, adders, memories, programmable logic gates, and many others.
材料方面,RTD主要采用分子束外延(MBE)技术或金属有机化合物汽相淀积(MOCVD)技术生长厚度合适的窄禁带半导体薄层制得量子阱区,在其上再生长宽禁带半导体层得到势垒层。由于MOCVD和MBE技术生长的薄层厚度可控制在几个纳米以内,量子阱和势垒的厚度都可控制在几个纳米内。RTD的势垒厚度相当于MOSFET的“沟道”长度,电子渡越这种“沟道”靠的是比漂移运动快得多的量子隧穿运动,因而RTD的速度性能应比MOSFET好。而RTD事实上不存在MOSFET那样的沟道,所以不会出现短沟道效应。其所特有的微分电阻特性可用较少数量的器件完成相当的功能:如用两个背靠背连接的RTD和一个晶体管构成SRAM单元,既节省芯片面积,又降低功耗。制作RTD的材料主要是III-V族化合物半导体,最合适的是InAlAs/InGaAs材料系,即以量子阱为窄禁带半导体InGaAs,势垒为宽禁带半导体AlAs。InP和GaAs与硅不同,它们都是直接带隙材料,具有电子饱和漂移速度高,耐高温,抗辐照等特点。在超高速、超高频、低功耗、低噪音器件和电路,特别在光电子器件和光电集成方面占有独特的优势。In terms of materials, RTD mainly uses molecular beam epitaxy (MBE) technology or metal organic compound vapor deposition (MOCVD) technology to grow a thin layer of narrow-bandgap semiconductor with a suitable thickness to form a quantum well region, and then grow a wide-bandgap semiconductor on it. layer to get the barrier layer. Since the thickness of the thin layer grown by MOCVD and MBE technology can be controlled within a few nanometers, the thickness of quantum wells and potential barriers can be controlled within a few nanometers. The barrier thickness of the RTD is equivalent to the length of the "channel" of the MOSFET. The electrons crossing the "channel" rely on the quantum tunneling motion which is much faster than the drift motion, so the speed performance of the RTD should be better than that of the MOSFET. In fact, RTD does not have a channel like MOSFET, so there will be no short channel effect. Its unique differential resistance characteristics can be used to complete equivalent functions with a small number of devices: for example, two RTDs connected back-to-back and a transistor are used to form an SRAM unit, which not only saves chip area but also reduces power consumption. The materials for making RTD are mainly III-V compound semiconductors, and the most suitable material is the InAlAs/InGaAs material system, that is, the quantum well is the narrow bandgap semiconductor InGaAs, and the potential barrier is the wide bandgap semiconductor AlAs. InP and GaAs are different from silicon, they are all direct bandgap materials, which have the characteristics of high electron saturation drift speed, high temperature resistance, and radiation resistance. It has unique advantages in ultra-high-speed, ultra-high-frequency, low-power, low-noise devices and circuits, especially in optoelectronic devices and optoelectronic integration.
由于RTD属于两端器件,不能实现电流的调制,因此在形成电路时需要与三端器件相结合。由于具有高的电子迁移率,GaAs和InP等化合物半导体材料制造的高速器件,在微波毫米波范围内得到广泛应用,高电子迁移率晶体管(HEMT)便是其中的代表。利用半导体平面工艺将基于量子隧穿效应的RTD和HEMT等器件在GaAs或InP衬底上集成起来,所形成的电路不仅保持了高频率、低噪声和低功耗的特点,而且比实现相同功能的其它器件电路所需的元件数要少得多,因此大大简化了电路结构,减小了芯片面积,提高了集成度,在数字以及混合电路中有着重要的应用。Since RTD is a two-terminal device and cannot realize current modulation, it needs to be combined with a three-terminal device when forming a circuit. Due to the high electron mobility, high-speed devices made of compound semiconductor materials such as GaAs and InP are widely used in the microwave and millimeter wave range, and the high electron mobility transistor (HEMT) is one of the representatives. Using semiconductor planar technology to integrate RTDs and HEMTs based on quantum tunneling effects on GaAs or InP substrates, the formed circuits not only maintain the characteristics of high frequency, low noise and low power consumption, but also achieve the same function The number of components required by other device circuits is much smaller, so the circuit structure is greatly simplified, the chip area is reduced, and the integration level is improved. It has important applications in digital and hybrid circuits.
目前RTD与HEMT的单片集成主要采用湿法腐蚀的方法实现的,但由于湿法工艺普遍存在着侧向腐蚀,不能精确控制器件的尺寸,不适应小尺寸器件电路的制作。而且由于湿法的一致性问题不能在整个片子上(尤其是4英寸以上)实现较均匀的腐蚀,不利于大规模器件的集成,并不适应产业化批量生产的需要。At present, the monolithic integration of RTD and HEMT is mainly realized by wet etching. However, due to the common lateral corrosion in the wet process, the size of the device cannot be accurately controlled, and it is not suitable for the production of small-sized device circuits. Moreover, due to the consistency of the wet method, uniform corrosion cannot be achieved on the entire wafer (especially above 4 inches), which is not conducive to the integration of large-scale devices, and does not meet the needs of industrialized mass production.
发明内容 Contents of the invention
本发明的目的在于,提供一种采用干法刻蚀技术实现RTD与HEMT单片集成的方法,对器件造成的损伤低,同时方向性更好,更适用于微小尺寸的制作;使小线条工艺得以实现,提高了良品率,适用于未来微纳米尺寸RTD与HEMT单片集成电路产业化生产的需要。The object of the present invention is to provide a method for monolithic integration of RTD and HEMT using dry etching technology, which causes less damage to the device, and has better directionality, and is more suitable for the production of tiny sizes; It can be realized, the yield rate is improved, and it is suitable for the needs of industrial production of micro-nano-sized RTD and HEMT monolithic integrated circuits in the future.
本发明一种采用干法刻蚀技术实现RTD与HEMT单片集成的方法,其特征在于,包括如下步骤:A kind of method adopting dry etching technique of the present invention to realize RTD and HEMT monolithic integration is characterized in that, comprises the following steps:
步骤1:在衬底上采用分子束外延或金属有机化学气相电极的方法依次生长典型的HEMT材料结构和RTD材料结构;Step 1: sequentially grow a typical HEMT material structure and RTD material structure on the substrate by molecular beam epitaxy or metal organic chemical vapor electrode;
步骤2:光刻出RTD发射区的图形,采用蒸发或溅射的方法制备AuGeNi金属层,去胶剥离,形成RTD金属发射极;Step 2: Lithograph the pattern of the RTD emission area, prepare the AuGeNi metal layer by evaporation or sputtering, remove the glue and peel off, and form the RTD metal emitter;
步骤3:采用非选择ICP干法刻蚀技术,以RTD金属发射极作为掩蔽,刻蚀RTD结构到重掺杂的InGaAs收集区接触层;Step 3: Using non-selective ICP dry etching technology, using the RTD metal emitter as a mask, etch the RTD structure to the heavily doped InGaAs collector contact layer;
步骤4:采用高选择性的湿法腐蚀液去除残余的InGaAs层,露出中间的选择性腐蚀停止层;Step 4: using a highly selective wet etching solution to remove the residual InGaAs layer to expose the middle selective etching stop layer;
步骤5:去除选择性腐蚀停止层;Step 5: removing the selective etch stop layer;
步骤6:光刻,形成有源区,采用ICP干法刻蚀技术刻蚀有源区外部分至半绝缘InP衬底,去胶;Step 6: Photolithography, forming the active area, using ICP dry etching technology to etch the outer part of the active area to the semi-insulating InP substrate, and removing the glue;
步骤7:光刻出HEMT的源漏电极,蒸发或溅射AuGeNi金属制备HEMT源电极、漏电极;Step 7: Photoetching the source and drain electrodes of the HEMT, evaporating or sputtering AuGeNi metal to prepare the source and drain electrodes of the HEMT;
步骤8:在保护气体气氛下实行快速高温退火;Step 8: performing rapid high-temperature annealing under a protective gas atmosphere;
步骤9:光刻出HEMT栅槽图形,采用选择性ICP干法刻蚀技术刻蚀掉部分重掺杂帽层,刻蚀停止于InAlAs势垒上,去胶;Step 9: Photoetch the HEMT gate groove pattern, use selective ICP dry etching technology to etch away part of the heavily doped cap layer, stop the etching on the InAlAs barrier, and remove the glue;
步骤10:在器件表面淀积生长一层钝化介质层;Step 10: Depositing and growing a passivation dielectric layer on the surface of the device;
步骤11:光刻出HEMT的栅电极图形,挖去部分的钝化介质层,采用蒸发或溅射的方法生成TiPtAu金属作为HEMT器件的栅电极;Step 11: photoetching the gate electrode pattern of the HEMT, digging out part of the passivation medium layer, and using evaporation or sputtering to generate TiPtAu metal as the gate electrode of the HEMT device;
步骤12:光刻出引线孔,挖去金属电极上面的钝化介质层,去胶;Step 12: Lithographically cut out the lead hole, dig out the passivation medium layer on the metal electrode, and remove the glue;
步骤13:光刻出引线互连区域,蒸发或溅射厚TiAlTiAu金属电极,去胶剥离。Step 13: Photoetching out the lead interconnection area, evaporating or sputtering thick TiAlTiAu metal electrodes, and removing the glue.
其中衬底为半绝缘InPIII-V族衬底。The substrate is a semi-insulating InPIII-V substrate.
其中HEMT材料结构包括依次生长的InAlAs缓冲层、InGaAs沟道、InAlAs隔离层、delta掺杂层、InAlAs势垒、重掺杂InGaAs帽层以及InP选择性腐蚀停止层。The HEMT material structure includes an InAlAs buffer layer, an InGaAs channel, an InAlAs isolation layer, a delta doped layer, an InAlAs barrier, a heavily doped InGaAs cap layer, and an InP selective etching stop layer grown sequentially.
其中RTD材料结构包括依次生长的重掺杂的InGaAs收集区接触层、InGaAs收集区隔离层、AlAs势垒、InGaAs/InAs/InGaAs阱、AlAs势垒、InGaAs发射区隔离层以及重掺杂的InGaAs发射区接触层。The RTD material structure includes sequentially grown heavily doped InGaAs collector contact layer, InGaAs collector isolation layer, AlAs barrier, InGaAs/InAs/InGaAs well, AlAs barrier, InGaAs emitter isolation layer and heavily doped InGaAs Emitter contact layer.
其中光刻步骤采用常规的光学方法或采用电子束投影光刻或浸入式光刻技术的方法实现。The photolithography step is realized by conventional optical method or electron beam projection lithography or immersion photolithography.
其中最后的引线互连,采用常规的介质层上金属互连或采用空气桥技术进行互连。Among them, the final lead wire interconnection is performed by conventional metal interconnection on dielectric layer or by air bridge technology.
其中衬底既可以是InP,也可以是GaAs,GaN等化合物半导体;The substrate can be either InP or GaAs, GaN and other compound semiconductors;
其中HEMT材料结构和RTD材料结构的生长,使用MBE的方法或使用MOCVD方法,或是二者结合的方法生长。The growth of the HEMT material structure and the RTD material structure adopts the method of MBE or the method of MOCVD, or a combination of the two methods.
其中高选择性的湿法腐蚀液是无机酸溶液或有机酸溶液。Among them, the highly selective wet etching solution is an inorganic acid solution or an organic acid solution.
其中所述的退火时间为10秒到30分钟,退火温度为200-500摄氏度。The annealing time is 10 seconds to 30 minutes, and the annealing temperature is 200-500 degrees Celsius.
其中钝化介质层是氧化硅或氮化硅或者氮氧化硅绝缘介质层。Wherein the passivation medium layer is an insulating medium layer of silicon oxide or silicon nitride or silicon oxynitride.
本发明的干法刻蚀与湿法腐蚀技术相比,在刻蚀均匀性、方向性以及提高良品率等方面都具有很大优势,广泛应用于工业化生产中。感应耦合等离子体(ICP)刻蚀在低的电压偏置下产生较高的等离子体浓度,与一般的干法刻蚀技术如反应离子束刻蚀(RIE)相比对器件造成的损伤低,同时方向性更好,更适用于微小尺寸的制作。由于具有较好的刻蚀均匀性,使下面的HEMT结构界面保持平整,有利于HEMT阈值电压与跨导一致性的改善。采用低损伤,可重复的ICP干法刻蚀工艺代替传统湿法腐蚀,各向异性腐蚀代替各向各向同性腐蚀,既解决了整片刻蚀的一致性问题,又使小线条工艺得以实现,提高了良品率,适用于未来微纳米尺寸RTD与HEMT单片集成电路产业化生产的需要。Compared with the wet etching technology, the dry etching method of the present invention has great advantages in the aspects of etching uniformity, directionality and improved yield, and is widely used in industrialized production. Inductively coupled plasma (ICP) etching produces higher plasma concentration under low voltage bias, and causes less damage to devices than general dry etching techniques such as reactive ion beam etching (RIE). At the same time, the directionality is better, and it is more suitable for the production of small sizes. Due to the better etching uniformity, the interface of the HEMT structure below is kept flat, which is beneficial to the improvement of the consistency of the threshold voltage and transconductance of the HEMT. The low-damage, repeatable ICP dry etching process is used to replace the traditional wet etching, and the anisotropic etching is used instead of the isotropic etching, which not only solves the problem of the consistency of the entire etching, but also enables the small line process to be realized. The yield rate is improved, and it is suitable for the industrial production of micro-nano size RTD and HEMT monolithic integrated circuits in the future.
附图说明 Description of drawings
为了进一步说明本发明的内容,以下结合实施例对本发明做一详细的描述,其中:In order to further illustrate content of the present invention, the present invention is described in detail below in conjunction with embodiment, wherein:
图1是本发明的材料结构图;Fig. 1 is a material structure diagram of the present invention;
图2是本发明的光刻生成RTD台面后的器件横截面图;Fig. 2 is the cross-sectional view of the device after the photolithography of the present invention generates the RTD mesa;
图3是本发明的光刻器件隔离后横截面图;Figure 3 is a cross-sectional view of the photolithographic device of the present invention after isolation;
图4是本发明的光刻生成HEMT源漏电极后的器件剖面图;Fig. 4 is the sectional view of the device after photolithography of the present invention generates HEMT source and drain electrodes;
图5是本发明的光刻腐蚀栅槽后的器件横截面图;Fig. 5 is the cross-sectional view of the device after photoetching the gate groove of the present invention;
图6是本发明的淀积氧化硅钝化介质层后的器件横截面图;Figure 6 is a device cross-sectional view after depositing a silicon oxide passivation dielectric layer of the present invention;
图7是本发明的光刻生成HEMT栅电极后的器件横截面图;Fig. 7 is a cross-sectional view of the device after the HEMT gate electrode is generated by photolithography of the present invention;
图8是本发明的光刻挖出引线孔后的器件横截面图;Fig. 8 is a cross-sectional view of the device after the lead hole is dug out by photolithography of the present invention;
图9是本发明的光刻引线互连加厚后的器件最终的横截面图。Figure 9 is a final cross-sectional view of the device after thickening of the photolithographic lead interconnects of the present invention.
具体实施方式 Detailed ways
请参阅图1至图9,本发明一种采用干法刻蚀技术实现RTD与HEMT单片集成的方法,包括如下步骤:Please refer to Fig. 1 to Fig. 9, a method for realizing monolithic integration of RTD and HEMT using dry etching technology in the present invention includes the following steps:
步骤1:在衬底100上采用分子束外延或金属有机化学气相电极的方法依次生长典型的HEMT材料结构200和RTD材料结构300(图1中),该衬底100为半绝缘InPIII-V族衬底;所述的HEMT材料结构200包括依次生长的InAlAs缓冲层101、InGaAs沟道102、InAlAs隔离层103、delta掺杂层、InAlAs势垒104、重掺杂InGaAs帽层10Step 1: sequentially grow a typical HEMT material structure 200 and an RTD material structure 300 (in FIG. 1 ) on the
5以及InP选择性腐蚀停止层106;所述的RTD材料结构包括依次生长的重掺杂的InGaAs收集区接触层107、InGaAs收集区隔离层108、AlAs势垒109、InGaAs110/InAs5 and an InP selective
111/InGaAs112阱、AlAs势垒113、InGaAs发射区隔离层114以及重掺杂的InGaAs发射区接触层115;所述的衬底既可以是InP,也可以是GaAs,GaN等化合物半导体;111/InGaAs112 well, AlAs
所述的HEMT材料结构200和RTD材料结构300的生长,使用MBE的方法或使用MOCVD方法,或是二者结合的方法生长The growth of the HEMT material structure 200 and the RTD material structure 300 is grown by MBE method or MOCVD method, or a combination of both
步骤2:光刻出RTD发射区的图形,采用蒸发或溅射的方法制备AuGeNi金属层120,去胶剥离,形成RTD金属发射极(图2中),所述的光刻步骤采用常规的光学方法或采用电子束投影光刻或浸入式光刻技术的方法实现;Step 2: Photoetching out the pattern of the RTD emission area, preparing the
步骤3:采用非选择ICP干法刻蚀技术,以RTD金属发射极作为掩蔽,刻蚀RTD结构到重掺杂的InGaAs收集区接触层107;Step 3: using non-selective ICP dry etching technology, using the RTD metal emitter as a mask, etching the RTD structure to the heavily doped InGaAs
步骤4:采用高选择性的湿法腐蚀液去除残余的InGaAs层107,露出中间的选择性腐蚀停止层106;所述的高选择性的湿法腐蚀液是无机酸溶液或有机酸溶液;Step 4: using a highly selective wet etching solution to remove the remaining
步骤5:去除选择性腐蚀停止层106;Step 5: removing the selective
步骤6:光刻,形成有源区,采用ICP干法刻蚀技术刻蚀有源区外部分至半绝缘InP衬底100,去胶(图3中);Step 6: photolithography, forming an active region, using ICP dry etching technology to etch the outer part of the active region to the
步骤7:光刻出HEMT的源漏电极,蒸发或溅射AuGeNi金属制备HEMT源电极121、漏电极122(图4中);Step 7: Photoetching the source and drain electrodes of the HEMT, evaporating or sputtering AuGeNi metal to prepare the
步骤8:在保护气体气氛下实行快速高温退火,所述的退火时间为10秒到30分钟,退火温度为200-500摄氏度;Step 8: Perform rapid high-temperature annealing under a protective gas atmosphere, the annealing time is 10 seconds to 30 minutes, and the annealing temperature is 200-500 degrees Celsius;
步骤9:光刻出HEMT栅槽图形,采用选择性ICP干法刻蚀技术刻蚀掉部分重掺杂帽层105,刻蚀停止于InAlAs势垒104上,去胶(图5中);Step 9: Photoetching out the HEMT gate groove pattern, using selective ICP dry etching technology to etch away part of the heavily doped
步骤10:在器件表面淀积生长一层钝化介质层130(图6中),其中钝化介质层130是氧化硅或氮化硅或者氮氧化硅绝缘介质层;Step 10: Deposit and grow a passivation dielectric layer 130 (in FIG. 6 ) on the device surface, wherein the
步骤11:光刻出HEMT的栅电极图形,挖去部分的钝化介质层130,采用蒸发或溅射的方法生成TiPtAu金属作为HEMT器件的栅电极123(图7中);Step 11: Photoetching the gate electrode pattern of the HEMT, digging out part of the
步骤12:光刻出引线孔,挖去金属电极上面的钝化介质层130,去胶(图8中);Step 12: photoetching lead holes, digging out the
步骤13:光刻出引线互连区域,蒸发或溅射厚TiAlTiAu金属电极,去胶剥离(图9中),最后的引线互连,采用常规的介质层上金属互连或采用空气桥技术进行互连。Step 13: Lithograph the lead interconnection area, evaporate or sputter the thick TiAlTiAu metal electrode, remove the glue and peel off (in Figure 9), and finally conduct the lead interconnection by conventional metal interconnection on the dielectric layer or air bridge technology interconnection.
实施例Example
请再参阅图1—图9,本发明一种采用干法刻蚀技术实现RTD与HEMT单片集成的方法,包括如下步骤:Please refer to Fig. 1-Fig. 9 again, a kind of method that adopts dry etching technology to realize RTD and HEMT monolithic integration of the present invention, comprises the following steps:
步骤1:在半绝缘InP衬底100上采用分子束外延的方法依次生长HEMT和RTD的材料结构:HEMT结构包括2000A非掺杂InAlAs缓冲层101,150A非掺杂InGaAs沟道102,30A非掺杂InAlAs隔离层103,4×1012cm-2delta平面掺杂层,200A非掺杂InAlAs势垒104以及200A重掺杂InGaAs帽层105。紧接着是50AInP选择性腐蚀停止层106,以及RTD结构,包括重掺杂的500AInGaAs收集区接触层107,50A非掺杂的收集区隔离层108,16A非掺杂AlAs势垒109,13A非掺杂InGaAs阱110,18A非掺杂InAs子阱111,13A非掺杂InGaAs阱112,16A非掺杂AlAs势垒113,50A非掺杂InGaAs发射区隔离层114以及500A重掺杂的InGaAs发射区接触层115。生长完毕的材料结构如图1所示;Step 1: On the
步骤2:采用电子束投影光刻出RTD发射区的图形,面积为1×1um2,采用电子束蒸发的方法蒸发Ni/Ge/Au/Ni/Au(50A/300A/800A/50A/1000A)金属,去胶剥离,形成RTD发射极120。电子束投影光刻有利于小尺寸的制作,本步光刻也可采用普通光学光刻或者浸入式曝光的方法实现;Step 2: Use electron beam projection to lithography the pattern of the RTD emission area, with an area of 1×1um2, and use electron beam evaporation to evaporate Ni/Ge/Au/Ni/Au (50A/300A/800A/50A/1000A) metal , remove the glue and peel off to form the
步骤3:采用ICP干法刻蚀技术,以RTD发射极120作为掩蔽,刻蚀RTD结构到重掺杂的InGaAs收集区接触层107,此步为非选择性刻蚀,反应气体为Cl2,射频功率为15W,直流偏压30V。ICP刻蚀在低直流偏压下可产生高的等离子体密度,与湿法腐蚀相比具有方向性好、刻蚀表面一致性好的优点,广泛应用于化合物半导体与深硅刻蚀工艺中;Step 3: Using ICP dry etching technology, using the
步骤4:采用高选择性的柠檬酸腐蚀液去除残余的InGaAs层,露出InP选择性腐蚀停止层106。其中柠檬酸腐蚀液的配比为C6H807:H202=2:1,pH值为5.5,除此之外以丁二酸为代表的有机酸类也可用于此步选择性的腐蚀;Step 4: using a highly selective citric acid etching solution to remove the remaining InGaAs layer to expose the InP selective
步骤5:在1:10的稀盐酸中漂5s钟去除InP选择性腐蚀停止层106,如图2所示;Step 5: remove the InP selective
步骤6:光刻出需要隔离的部分,采用ICP干法刻蚀到半绝缘InP衬底100,此步为非选择性刻蚀,反应气体为Cl2,射频功率为15W,直流偏压30V。去胶后如图3所示;Step 6: Photoetch the parts to be isolated, and etch the
步骤7:光刻出HEMT的源漏电极,蒸发Ni/Ge/Au/Ni/Au(50A/300A/800A/50A/1000A)金属生成HEMT漏电极121和源电极122,如图4所示;Step 7: Photoetching the source and drain electrodes of the HEMT, evaporating Ni/Ge/Au/Ni/Au (50A/300A/800A/50A/1000A) metal to form the
步骤8:在N2:H2=2:1的混合气氛下,在500摄氏度条件下退火10秒。过度退火使杂质离子进入到非掺杂的阱区,造成RTD峰谷电流比的下降,而退火不足不易形成良好的欧姆接触,造成器件直流特性的下降;Step 8: Under the mixed atmosphere of N2:H2=2:1, anneal at 500 degrees Celsius for 10 seconds. Excessive annealing causes impurity ions to enter the non-doped well region, resulting in a decrease in the RTD peak-to-valley current ratio, while insufficient annealing is not easy to form a good ohmic contact, resulting in a decrease in the DC characteristics of the device;
在N2:H2=2:1的混合气氛下,在360摄氏度条件下退火1分钟。过度退火使杂质离子进入到非掺杂的阱区,造成RTD峰谷电流比的下降,而退火不足不易形成良好的欧姆接触,造成器件直流特性的下降;Under the mixed atmosphere of N2:H2=2:1, anneal at 360 degrees Celsius for 1 minute. Excessive annealing causes impurity ions to enter the non-doped well region, resulting in a decrease in the RTD peak-to-valley current ratio, while insufficient annealing is not easy to form a good ohmic contact, resulting in a decrease in the DC characteristics of the device;
在N2:H2=2:1的混合气氛下,在200摄氏度条件下退火30分钟。过度退火使杂质离子进入到非掺杂的阱区,造成RTD峰谷电流比的下降,而退火不足不易形成良好的欧姆接触,造成器件直流特性的下降;Under the mixed atmosphere of N2:H2=2:1, anneal at 200 degrees Celsius for 30 minutes. Excessive annealing causes impurity ions to enter the non-doped well region, resulting in a decrease in the RTD peak-to-valley current ratio, while insufficient annealing is not easy to form a good ohmic contact, resulting in a decrease in the DC characteristics of the device;
步骤9:光刻出HEMT栅槽图形,采用选择性ICP干法刻蚀技术刻蚀掉重掺杂帽层105,刻蚀停止于InAlAs势垒104上。此步刻蚀为选择性刻蚀,反应气体为比例1:3的SF6与BCl3的混合气体,射频功率为15W,直流偏压30V,去胶后如图5所示。干法刻蚀通过对反应气体的选择可实现对不同材料的选择性腐蚀,而ICP具有低损伤的特点,采用ICP技术进行选择性刻蚀,既保持了对不同材料结构的高选择性,又在方向性与表面一致性等方面得到了改善,适用于未来小尺寸大规模集成电路的需要;Step 9: Photoetching the gate groove pattern of the HEMT, using selective ICP dry etching technology to etch the heavily doped
步骤10:采用PECVD的方法生长一层SiO2钝化介质层130,厚度为3000A,如图6所示。生长温度300摄氏度,功率15W,厚的氧化硅有利于减少结面电容;Step 10: A layer of SiO 2 passivation
步骤11:光刻出HEMT的栅电极图形,使用B OE氧化硅腐蚀液去除表面的SiO2钝化介质层130,采用电子束蒸发的方法蒸发Ti/Pt/Au(500A/500A/2000A)金属作为HEMT器件的栅电极123,如图7所示;Step 11: Photoetching the gate electrode pattern of HEMT, using B OE silicon oxide etching solution to remove the SiO2
步骤12:光刻出引线孔图形,使用BOE氧化硅腐蚀液去除金属电极上面的SiO2钝化介质层130,去胶后如图8所示;Step 12: photolithography lead hole pattern, use BOE silicon oxide etching solution to remove the SiO 2
步骤13:光刻出引线互连加厚的区域,采用电子束蒸发的方法蒸发Ti/Al/Ti/Au(500A/8000A/1500A/2000A)电极,去胶剥离,最终形成如图9所示的结构。在工艺允许的情况下尽量加厚电极,厚的互连电极可降低串联电阻,从而提高电路的直流与高频性能。Step 13: Lithograph the thickened area of the lead interconnection, evaporate Ti/Al/Ti/Au (500A/8000A/1500A/2000A) electrodes by electron beam evaporation, remove the glue and peel off, and finally form as shown in Figure 9 Structure. Thicken the electrodes as much as possible if the process allows. Thick interconnect electrodes can reduce the series resistance, thereby improving the DC and high frequency performance of the circuit.
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CN108648997B (en) * | 2018-05-21 | 2020-02-18 | 雄安华讯方舟科技有限公司 | Preparation method of resonant tunneling diode wafer structure |
CN109216331B (en) * | 2018-07-23 | 2020-07-17 | 西安电子科技大学 | A PIN diode-based millimeter-wave predistortion integrated circuit and its fabrication method |
US20230327008A1 (en) * | 2022-04-06 | 2023-10-12 | International Business Machines Corporation | Semiconductor device with high-electron mobility transistor |
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