电子束蒸发硅铁制备多晶/spl β /-FeSi2薄膜的光学、电学和结构特性

H. Katsumata, Y. Makita, H. Takahashi, Hajime Shibata, N. Kobayashi, Masataka Hasegawa, Shinji Kimura, A. Obara, J. Tanabe, S. Uekusa
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引用次数: 1

摘要

采用电子束沉积技术在室温下将99.9%的硅铁(FeSi/sub 2/)晶粒蒸发到(100)取向n型FZ Si衬底上。在400/spl sim/950/spl℃范围内,系统地研究了随后的等时(2小时)退火温度(T/sub / a/)对光学、电学和结构性能的影响。x射线衍射和拉曼散射分析表明,在T/sub a/=500/spl度/C以上形成多晶/spl β /-FeSi/sub 2/,而在T/sub a/=800/spl度/C以上形成Si团聚。样品的电阻率在T/sub a/=700/spl℃时达到最大值(0.542 /spl ω //spl middot/cm),随后随T/sub a/的增大而减小。它的减少过程可以通过考虑Si空位的产生来解释,这些空位可能起到空穴的作用。在T/sub /=600/spl sim/800/spl度/C时,大多数载流子从n型转换为p型,这是非常有趣的。典型载流子浓度和迁移率分别为:/spl mu//sub n/=39.4 cm/sup 2//V/spl middot/sec, n型/spl beta/-FeSi/sub 2/ n/sub e/=6.59/spl倍/10/sup 17/ cm/sup -3/, T/sub a/=600/spl度/C, n/sub e/= 20.3 cm/sup 2//V/spl middot/sec, p型/spl beta/-FeSi/sub 2/ T/sub a/=850/spl度/C, n/sub h/=2.22/spl倍/10/sup 18/ cm/sup -3/。光学吸收测量表明,随着Ta的增加,带隙的性质从间接到直接变化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Optical, electrical and structural properties of polycrystalline /spl beta/-FeSi2 thin films fabricated by electron beam evaporation of ferrosilicon
Ferrosilicon (FeSi/sub 2/) grains (99.9%) were evaporated at room temperature onto a (100)-oriented n-type FZ Si substrate using electron beam deposition technique. Optical, electrical and structural properties were systematically investigated as a function of subsequent isochronal (2 hrs) annealing temperature (T/sub a/) in the range of 400/spl sim/950/spl deg/C. X-ray diffraction and Raman scattering analysis suggested the formation of polycrystalline /spl beta/-FeSi/sub 2/ above T/sub a/=500/spl deg/C, whereas above T/sub a/=800/spl deg/C, Si agglomeration was observed to form. The electrical resistivity of these samples reached a maximum (0.542 /spl Omega//spl middot/cm) at T/sub a/=700/spl deg/C, and then it decreased with increasing T/sub a/. Its decrease process was explained by considering the creation of Si vacancies, which could presumably be acting as holes. It is of great interest that in T/sub a/=600/spl sim/800/spl deg/C, the majority carrier converts from n- to p-type. Typical carrier concentrations and mobilities were determined to be /spl mu//sub n/=39.4 cm/sup 2//V/spl middot/sec, n/sub e/=6.59/spl times/10/sup 17/ cm/sup -3/ for n-type /spl beta/-FeSi/sub 2/ with T/sub a/=600/spl deg/C and /spl mu//sub h/=20.3 cm/sup 2//V/spl middot/sec, n/sub h/=2.22/spl times/10/sup 18/ cm/sup -3/ for p-type /spl beta/-FeSi/sub 2/ with T/sub a/=850/spl deg/C. Optical absorption measurements revealed that the nature of the bandgap varies from an indirect to direct one with increasing Ta.
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