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ELECTRONIC PROPERTIES AND MICROSTRUCTURE OF UNDOPED, AND B- OR P-DOPED POLYSILICON DEPOSITED BY LPCVD

机译:LPCVD沉积的非掺杂和B或P掺杂的多晶硅的电子性质和微观结构

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In this paper, we present some results on the electrical and optical properties of thin layers of polysilicon obtained by LPCVD in a sector reactor [1]. This reactor is representative of annular reactor, in which a large batch can be processed (total area up to 150 m(2)). The layers are either undoped, or in situ doped with boron or phosphorus, The optical constants were determined by the analysis of absorption and transmission spectra. We show that the absorption coefficient of the layers (doped or undoped) enable a total absorption in the visible range with a thickness of 10 mu m. We then show that uniform growth rate can be obtained on 100 cm(2) substrates, with a value of 200 Angstrom/mn at 660 degrees C for undoped or P-doped silicon, and 700 Angstrom/mn for B-doped silicon. The carrier concentrations ranges between 1 x 10(17) and 1 x 10(20) cm(-3), which allows the realization of doping gradient during the process and potentially good solar cells with a high productivity. [References: 17]
机译:在本文中,我们介绍了在扇区反应器中通过LPCVD获得的多晶硅薄层的电学和光学性质的一些结果。该反应器是环形反应器的代表,其中可以处理大批量(总面积最大为150 m(2))。这些层是未掺杂的,或者是原位掺杂有硼或磷的。通过分析吸收和透射光谱来确定光学常数。我们表明,各层(掺杂或未掺杂)的吸收系数使可见光范围内的总吸收达到10μm。然后,我们表明可以在100 cm(2)的基板上获得均匀的生长速率,对于未掺杂或P掺杂的硅,在660摄氏度时的值为200 / mn,对于B掺杂的硅为700 700 / mn。载流子浓度范围在1 x 10(17)和1 x 10(20)cm(-3)之间,这可以实现工艺过程中的掺杂梯度,并可能以高生产率实现良好的太阳能电池。 [参考:17]

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