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Growth of AIN films on Si(100) and Si(111) substrates by reactive magnetron sputtering

机译:反应磁控溅射在Si(100)和Si(111)衬底上生长AIN膜

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GaN has shown great potential for high-power high-frequency electronic devices and short-wavelength optical devices. To integrate GaN-based optoelectronic devices with Si-based electronic devices and reduce the cost, it is desirable to grow epitaxial GaN thin films and device structures on the Si substrate. However, a proper buffer layer is essential for epitaxial growth of GaN films on Si substrate due to large mismatch between them in the area of lattice constant, thermal expansion coefficient and chemistry feature. In the present work, the growth of AlN buffer layer was studied. Wurtzite aluminum nitride thin films were grown on Si (111) and Si (100) substrates using reactive sputtering deposition under different discharge powers. X-ray diffraction (XRD) patterns showed that full width at half maximum (FWHM) of AlN (0002) peak grown on Si (111) substrates was smaller than that grown on Si (100) substrates. Vibrational characterization by Fourier transform infrared spectroscopy (FTIR) revealed that the stress in the AlN films deposited on Si (111) substrates was also smaller than that deposited on Si (100) substrates. For Si (100) substrates, the large lattice mismatch between AlN (0001) and Si (100) is a main contribution to the large strain in the formed films. For Si (111) substrates, the strain in the films deposited on Si (111) largely depends on the discharge power in sputtering, and the strain due to defects and thermal mismatch contributes largely to the residual strain in the deposited films. (c) 2004 Elsevier B.V. All rights reserved.
机译:GaN在高功率高频电子器件和短波长光学器件中显示出巨大潜力。为了将基于GaN的光电器件与基于Si的电子器件集成在一起并降低成本,期望在Si衬底上生长外延GaN薄膜和器件结构。但是,适当的缓冲层对于在GaN衬底上外延生长GaN膜是必不可少的,因为它们之间在晶格常数,热膨胀系数和化学特性方面存在很大的不匹配。在目前的工作中,研究了AlN缓冲层的生长。使用反应溅射沉积在不同的放电功率下,将纤锌矿型氮化铝薄膜生长在Si(111)和Si(100)衬底上。 X射线衍射(XRD)图谱显示,在Si(111)衬底上生长的AlN(0002)峰的半峰全宽(FWHM)小于在Si(100)衬底上生长的半峰全宽。傅立叶变换红外光谱(FTIR)的振动表征表明,沉积在Si(111)衬底上的AlN膜中的应力也小于沉积在Si(100)衬底上的应力。对于Si(100)衬底,AlN(0001)和Si(100)之间的较大晶格失配是所形成薄膜中较大应变的主要因素。对于Si(111)衬底,沉积在Si(111)上的膜中的应变在很大程度上取决于溅射中的放电功率,并且由于缺陷和热失配引起的应变在很大程度上造成了沉积膜中的残余应变。 (c)2004 Elsevier B.V.保留所有权利。

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