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Optical, electrical and structural properties of polycrystalline /spl beta/-FeSi/sub 2/ thin films fabricated by electron beam evaporation of ferrosilicon

机译:通过硅铁电子束蒸发制备的多晶/ spl beta / -FeSi / sub 2 /薄膜的光学,电学和结构性质

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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.
机译:使用电子束沉积技术在室温下将硅铁(FeSi / sub 2 /)晶粒(99.9%)蒸发到(100)取向的n型FZ Si衬底上。系统地研究了光学,电学和结构性能,作为随后的等时(2小时)退火温度(T / sub a /)的函数,退火温度在400 / spl sim / 950 / spl deg / C范围内。 X射线衍射和拉曼散射分析表明,高于T / sub a / = 500 / spl deg / C时,形成了多晶/ spl beta / -FeSi / sub 2 /,而高于T / sub a / = 800 / spl deg / C C,观察到形成Si团聚。这些样品的电阻率在T / sub a / = 700 / spl deg / C时达到最大值(0.542 / splΩ// spl中点/ cm),然后随T / sub a /的增加而降低。考虑到硅空位的产生解释了其减少过程,该空位可能起着空洞的作用。非常有趣的是,在T / sub a / = 600 / spl sim / 800 / spl deg / C中,多数载流子从n型转变为p型。确定的典型载流子浓度和迁移率是/ spl mu // sub n / = 39.4 cm / sup 2 // V / spl middot / sec,n / sub e / = 6.59 / spl次/ 10 / sup 17 / cm / sup -3 /用于n型/ spl beta / -FeSi / sub 2 /,T / sub a / = 600 / spl deg / C和/ spl mu // sub h / = 20.3 cm / sup 2 // V / spl middot / sec,n / sub h / = 2.22 / spl次/ 10 / sup 18 / cm / sup -3 /对于p型/ spl beta / -FeSi / sub 2 / T / sub a / = 850 /升/摄氏度光吸收测量表明,带隙的性质随Ta的增加从间接变为直接。

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