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Quasi-single Crystal Semiconductors on Glass Substrates through Biaxially Oriented Buffer Layers

机译:玻璃基板上的准单晶半导体通过双轴取向缓冲层

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High efficiency photovoltaic devices are normally fabricated on single crystalline substrates. These single crystalline substrates are expensive and volume production for widespread usage has not been realistic. To date, large volume production of solar cells is on less expensive noncrystalline substrates such as glass. Typically the films grown on glass are polycrystalline with less than ideal efficiency. It was proposed that a dramatic gain in the efficiency may be achieved if one uses a biaxially oriented buffer layer on glass to grow biaxial semiconductor films to fabricate solar devices compared to that of films grown directly on glass. Biaxial films are not exactly single crystal but have strongly preferred crystallographic orientations in both the out-of-plane and in-plane directions. Typically the misorientation between grains can be small (within a few degrees) and may possess low carrier recombination rate. In this paper we shall discuss growth techniques that would allow one to produce biaxial buffer layers on glass. A specific strategy using an atomic shadowing mechanism in an oblique angle deposition configuration that allows one to grow biaxial buffer layers such as CaF_2 on glass substrate will be discussed in detail. Results of heteroepitaxy of semiconductor materials such as CdTe and Ge on these biaxial buffer/glass substrates characterized by x-ray pole figure, reflection high energy electron diffraction (RHEED) pole figure and transmission electron microscopy (TEM) will be presented.
机译:高效光伏器件通常在单晶基板上制造。这些单晶基材是昂贵的并且对于广泛使用的体积产生并不逼真。迄今为止,大量的太阳能电池生产在较便宜的非折叠基材上,例如玻璃。通常,在玻璃上生长的薄膜是多晶,效率低于理想效率。建议如果在玻璃上使用双轴取向的缓冲层以生长双轴半导体膜以制造太阳能器件的效率可以实现效率的显着增益,而直接在玻璃上生长的薄膜。双轴膜不完全单晶,但在平面外和面内方向上具有强烈优选的晶形取向。通常,晶粒之间的错误化可以小(在几度内)并且可能具有低载体重组率。在本文中,我们将讨论将在玻璃上生产双轴缓冲层的增长技术。将详细讨论使用允许诸如CAF_2的倾斜角沉积配置中的原子阴影构造中的原子遮蔽构造的特定策略将详细讨论玻璃基板上的双轴缓冲层。通过X射线极值表征的这些双轴缓冲器/玻璃基板上的半导体材料的杂肝的结果,将呈现反射高能电子衍射(RHEED)极值(RHEED)极值(REVEED)极值(REM)。

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