预辅Al及AlN缓冲层厚度对GaN/Si(111)材料特性的影响

主要研究了采用高温AlN缓冲层外延生长GaN/Si(111)材料的工艺技术。利用高分辨X射线双晶衍射(HRXRD)分析研究了GaN/Si(111)样品外延层的应变状态和晶体质量,通过原子力显微镜(AFM)分析研究了不同厚度的高温AlN缓冲层对GaN外延层的表面形貌的影响。实验结果表明,AlN缓冲层生长前预通三甲基铝(TMAl)的时间、AlN缓冲层的厚度对GaN外延层的应变状态、外延层的晶体质量以及表面形貌都有显著影响。得到最优的预辅Al时间为10s,AlN缓冲层的厚度为40nm。在此条件下外延生长的GaN样品(厚度约为1μm)表面形貌较好,X射线衍射(XRD)双晶摇摆曲线半峰全宽(FWHM)(0002)面和(10-12)面分别为452″和722″。     

AlN缓冲层厚度对脉冲激光沉积技术生长的GaN薄膜性能的影响

在蓝宝石(Al2O3)衬底上应用脉冲激光沉积技术(PLD)生长不同厚度的AlN缓冲层后进行GaN薄膜外延生长。采用高分辨X射线衍射仪(HRXRD)和扫描电子显微镜(SEM)对外延生长所得GaN薄膜的晶体质量和表面形貌进行了表征。测试结果表明: 相比直接在Al2O3衬底上生长的GaN薄膜, 通过生长AlN缓冲层的GaN薄膜虽然晶体质量较差, 但表面较平整; 而且随着AlN缓冲层厚度的增加, GaN薄膜的晶体质量和表面平整度均逐渐提高。可见, AlN缓冲层厚度对在Al2O3衬底上外延生长GaN薄膜的晶体质量和表面形貌有着重要的影响。     

AlN缓冲层厚度对脉冲激光沉积技术生长的GaN薄膜性能的影响

在蓝宝石(Al2O3)衬底上应用脉冲激光沉积技术(PLD)生长不同厚度的AlN缓冲层后进行GaN薄膜外延生长。采用高分辨X射线衍射仪(HRXRD)和扫描电子显微镜(SEM)对外延生长所得GaN薄膜的晶体质量和表面形貌进行了表征。测试结果表明:相比直接在Al2O3衬底上生长的GaN薄膜,通过生长AlN缓冲层的GaN薄膜虽然晶体质量较差,但表面较平整;而且随着AlN缓冲层厚度的增加,GaN薄膜的晶体质量和表面平整度均逐渐提高。可见,AlN缓冲层厚度对在Al2O3衬底上外延生长GaN薄膜的晶体质量和表面形貌有着重要的影响。     

6H-SiC衬底上采用不同厚度AlN缓冲层对GaN外延层的影响

采用不同厚度AlN作为缓冲层在6H-SiC衬底上生长了GaN外延层,并利用X射线衍射,拉曼散射和透射电子显微镜等对GaN性质进行了研究。AlN缓冲层的应变状态对GaN的晶体质量和表面形貌有很大影响。较厚的AlN缓冲层会导致GaN表面出现裂纹,而太薄的AlN缓冲层会导致GaN层较高的位错密度,从而恶化器件性能。分析了GaN产生裂纹和高位错密度的机制,并采用较优厚度（100nm）的AlN缓冲层生长出高质量的GaN外延层。     

AlGaN缓冲层结构对Si基GaN材料性能的影响

Si衬底与GaN之间较大的晶格失配和热失配引起的张应力使GaN外延层极易产生裂纹,如何补偿GaN所受到的张应力是进行Si基GaN外延生长面临的首要问题.采用金属有机化合物化学气相沉积(MOCVD)技术在4英寸(1英寸=2.54 cm)Si (111)衬底上制备了GaN外延材料并研究了不同AlGaN缓冲层结构对Si基GaN外延材料性能的影响,并采用高分辨X射线衍射仪(HRXRD)、原子力显微镜(AFM)、喇曼光谱以及光学显微镜对制备的GaN材料的性能进行了表征.采用3层A1GaN缓冲层结构制备了表面光亮、无裂纹的GaN外延材料,其(002)晶面半高宽为428 arcsec,表面粗糙度为0.194 nm.结果表明,采用3层A1GaN缓冲层结构可以有效地降低GaN材料的张应力和位错密度,进而遏制表面裂纹的出现,提高晶体质量.     

采用AlN缓冲层在Si(111)衬底上生长GaN的形貌

针对Si衬底上生长GaN具有的特有形貌进行了研究,分析采用扫描电镜(SEM)、X射线能谱仪(EDS)、原子力显微镜(AFM)等手段,研究了使用AlN作为缓冲层的GaN的生长模式、缺陷形成机理、应力释放机制.并且发现缓冲层厚度和外延层生长温度对裂纹和表面缺陷的形成有很大的影响.     

采用AlN缓冲层在Si(111)衬底上生长GaN的形貌

针对Si衬底上生长GaN具有的特有形貌进行了研究,分析采用扫描电镜(SEM)、X射线能谱仪(EDS)、原子力显微镜(AFM)等手段,研究了使用AlN作为缓冲层的GaN的生长模式、缺陷形成机理、应力释放机制.并且发现缓冲层厚度和外延层生长温度对裂纹和表面缺陷的形成有很大的影响.     

Si(111)衬底上GaN外延材料的应力分析

对Si(111)衬底上GaN外延材料的应力随着低温AlN插入层数的变化进行了分析研究。通过喇曼散射谱在高频E2(TO)模式下的测试分析发现,随着低温AlN插入层数的增加,GaN材料的E2(TO)峰位逐渐接近体GaN材料的E2(TO)峰位(无应力体GaN材料的E2(TO)峰位为568cm-1),计算得出GaN材料的应力从1.09GPa减小到0.42GPa。同时,使用室温光荧光谱进行了分析验证。结果表明,Si衬底上GaN外延材料受到的是张应力,通过低温AlN插入层技术可以有效降低GaN材料的应力,并且最终实现了表面光亮的厚层无裂纹GaN材料。     

插入δAl/AlN缓冲层在Si(111)上生长GaN

采用MOCVD(metal organic chemical vapor deposition)生长方法,对比在AlN层上加入δAl/AlN缓冲层和不加入δAl/AlN缓冲层两种生长结构,在Si(111)衬底上生长GaN.实验结果表明,在加入δAl/AlN缓冲层后,GaN外延层的裂纹密度得到了有效的降低,晶体质量也得到了明显的提高.通过MOCVD生长方法,利用光学显微镜、XRD和Raman等分析测试手段,研究了δAl/AlN缓冲层对GaN外延层的影响,获得了裂纹密度小、晶体质量高的GaN材料.     

插入δAl/AlN缓冲层在Si(111)上生长GaN

采用MOCVD(metal organic chemical vapor deposition)生长方法,对比在AlN层上加入δAl/AlN缓冲层和不加入δAl/AlN缓冲层两种生长结构,在Si(111)衬底上生长GaN.实验结果表明,在加入δAl/AlN缓冲层后,GaN外延层的裂纹密度得到了有效的降低,晶体质量也得到了明显的提高.通过MOCVD生长方法,利用光学显微镜、XRD和Raman等分析测试手段,研究了δAl/AlN缓冲层对GaN外延层的影响,获得了裂纹密度小、晶体质量高的GaN材料.     

Effects of high-temperature AIN buffer on the microstructure of AlGaN/GaN HEMTs

Effects on AlGaN/GaN high-electron-mobility transistor structure of a high-temperature AlN buffer on sapphire substrate have been studied by high-resolution x-ray diffraction and atomic force microscopy techniques. The buffer improves the microstructural quality of GaN epilayer and reduces approximately one order of magnitude the edge-type threading dislocation density. As expected, the buffer also leads an atomically flat surface with a low root-mean-square of 0.25 nm and a step termination density in the range of 10⁸ cm^?2. Due to the high-temperature buffer layer, no change on the strain character of the GaN and AlGaN epitaxial layers has been observed. Both epilayers exhibit compressive strain in parallel to the growth direction and tensile strain in perpendicular to the growth direction. However, an high-temperature AlN buffer layer on sapphire substrate in the HEMT structure reduces the tensile stress in the AlGaN layer.     

引入GaN过渡层对Si（111）衬底上生长GaN外延的影响

本文研究了在Si(111)衬底上生长GaN外延层的方法。相比于直接在AlN缓冲层上生长GaN外延层,引入GaN过渡层显著地提高了外延层的晶体质量并降低了外延层的裂纹密度。使用X射线双晶衍射仪、光学显微镜以及在位监测曲线分析了GaN过渡层对外延层的晶体质量以及裂纹密度的影响。实验发现,直接在AlN缓冲层上生长外延层,晶体质量较差, X射线(0002)面半高宽最优值为0.686°,引入GaN过渡层后,通过调整生长条件,控制岛的长大与合并的过程,从而控制三维生长到二维生长过渡的过程,外延层的晶体质量明显提高, (0002)面半高宽降低为0.206°,并且裂纹明显减少。研究结果证明,通过生长合适厚度的GaN过渡层,可以得到高质量、无裂纹的GaN外延层。     

MOCVD Growth of Device—quality GaN on Sapphire

An AIN Layer grown by an ALE has been developed to improve the growth quality of GaN ON Al2O3 substrate by low-pressure metalorganic vapor phase epitaxy(LP-MOVPE).An ALE AIN layer grown on Al2O3 substrate has a high quality and the structure is similar to GaN, this AIN layer can release the stress between Al2O3 substrate and GaN epilayer.By using this method, the orientation of substrate is extended to GaN epilayer, and the column tilt and the twist are improved, so as to obtain the device-quality GaN.     

利用三步法MOCVD生长器件质量的GaN

在传统的二步MOCVD外延生长的基础上，报道了一种在低压MOCVD中用三步外延生长GaN材料的新方法，它在生长低温缓冲层前，用原子层的方法生长一层高质量的AIN层来减少Al2O3与GaN缓冲层之间的应力以提高缓冲层的质量，从而提高外延层GaN的质量，达到器件制作的要求。     

Influence of AlN buffer layer thickness on the properties of GaN epilayer on Si(1 1 1) by MOCVD

The effect of thickness of the high-temperature (HT) AlN buffer layer on the properties of GaN grown on Si(1 1 1) has been investigated. Optical microscopy (OM), atomic force microscopy (AFM) and X-ray diffraction (XRD) are employed to characterize these samples grown by metal-organic chemical vapor deposition (MOCVD). The results demonstrate that the morphology and crystalline properties of the GaN epilayer strongly depend on the thickness of HT AlN buffer layer, and the optimized thickness of the HT AlN buffer layer is about 110 nm. Together with the low-temperature (LT) AlN interlayer, high-quality GaN epilayer with low crack density can be obtained.     

MOCVD epitaxy of InAlN on different templates

InAlN epilayers were grown on high quality GaN and A1N templates with the same growth parameters. Measurement results showed that two samples had the same In content of～16%,while the crystal quality and surface topography of the InAlN epilayer grown on the AlN template,with 282.3"（002） full width at half maximum （FWHM） of rocking curve,313.5"（102） FWHM,surface roughness of 0.39 nm and V-pit density of 2.8×10⁸ cm^-2,were better than that of the InAlN epilayer grown on the GaN template,309.3",339.1",0.593 nm and 4.2×10⁸ cm^-2.A primary conclusion was proposed that both the crystal quality and the surface topography of the InAlN epilayer grown on the AlN template were better than that of the InAlN epilayer grown on the GaN template. Therefore,the AlN template was a better choice than the GaN template for getting high quality InAlN epilayers.     

Effect of AlN buffer thickness on GaN epilayer grown on Si(1 1 1)

We studied the influence of high temperature AlN buffer thickness on the property of GaN film on Si (1 1 1) substrate. Samples were grown by metal organic chemical vapor deposition. Optical microscopy, atomic force microscopy and X-ray diffraction were employed to characterize the samples. The results demonstrated that thickness of high temperature AlN buffer prominently influenced the morphology and the crystal quality of GaN epilayer. The optimized thickness of the AlN buffer is found to be about 150 nm. Under the optimized thickness, the largest crack-free range of GaN film is 10 mm×10 mm and the full width at half maximum of GaN (0 0 0 2) rocking curve peak is 621.7 arcsec. Using high temperature AlN/AlGaN multibuffer combined with AlN/GaN superlattices interlayer we have obtained 2 μm crack-free GaN epilayer on 2 in Si (1 1 1) substrates.     

Analysis of the growth of GaN epitaxy on silicon

Due to the great potential of GaN based devices,the analysis of the growth of crack-free GaN with high quality has always been a research hotspot.In this paper,two methods for improving the property of the GaN epitaxial layer on Si (111) substrate are researched.Sample A,as a reference,only has an AlN buffer between the Si substrate and the epitaxy.In the following two samples,a GaN transition layer (sample B) and an AlGaN buffer (sample C) are grown on the AlN buffer separately.Both methods improve the quality of GaN.Meanwhile,using the second method,the residual tensile thermal stress decreases.To further study the impact of the two introduced layers,we investigate the stress condition of GaN epitaxial layer by Raman spectrum.According to the Raman spectrum,the calculated residual stress in the GaN epitaxial layer is approximately 0.72 GPa for sample B and 0.42 GPa for sample C.The photoluminescence property of GaN epitaxy is also investigated by room temperature PL spectrum.     

High quality AIN and GaN grown on compliant Si/SiC substrates by gas source molecular beam epitaxy

Epitaxial layers of AlN and GaN were grown by gas source molecular-beam epitaxy on a composite substrate consisting of a thin (250 nm) layer of silicon (111) bonded to a polycrystalline SiC substrate. Two dimensional growth modes of AlN and GaN were observed. We show that the plastic deformation of the thin Si layer results in initial relaxation of the AlN buffer layer and thus eliminates cracking of the epitaxial layer of GaN. Raman, x-ray diffraction, and cathodoluminescence measurements confirm the wurtzite structure of the GaN epilayer and the c-axis crystal growth orientation. The average stress in the GaN layer is estimated at 320 MPa. This is a factor of two less than the stress reported for HVPE growth on 6H-SiC (0001).