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One- and two-phonon Raman scattering from hydrogenated nanocrystalline silicon films

机译:氢化纳米晶硅膜的一声子和二声子拉曼散射

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One- and two-phonon Raman scattering from intrinsic and boron as well as phosphorus doped hydrogenated nanocrystalline silicon films prepared by plasma enhanced chemical vapor deposition technique were investigated. With regard to one-phonon Raman measurements of intrinsic films, redshifts attending by asymmetrical broadening of one-phonon transverse optical (TO) mode with diminishing mean dimension of Si nanocrystals can be ascribed to incorporating effects of phonon confinement and tensile strain. Photoluminescence behavior of these intrinsic specimens can be interpreted by a consistent way when recombination of quantum-confined excitons in Si nanocrystals is assumed. As to one-phonon Raman signals of doped nc-Si:H materials, besides joint effects of phonon confinement and tensile strain, additional redshifts accompanying with asymmetrical broadening of one-phonon TO band with increasing doping level can be assigned to carrier effect and disorder from doping. With diminishing average size of Si nanocrystals or increasing dopants, the decay of two-phonon Raman amplitudes of intrinsic and doped samples can be attributed to disorder. Raman experiments indicate that all the energies of the two-phonon TO branches are different from twice the energies of the one-phonon TO active bands, which reveal that the two-phonon TO modes do not come from the Raman active phonons at wavevector k = 0. The peak shift of two-phonon transverse optical (2TO) modes relates to phonon confinement and disorder. Negligible peak shift in TO (2TO) modes of intrinsic and doped films on temperature indicates that the interface strain in nc-Si:H/c-Si can be ignored. (c) 2006 Elsevier Ltd. All rights reserved.
机译:研究了通过等离子增强化学气相沉积技术制备的本征和硼以及磷掺杂的氢化纳米晶硅薄膜的一声子和二声子拉曼散射。关于本征膜的单声子拉曼测量,通过单声子横向光学(TO)模的不对称展宽伴随着Si纳米晶体平均尺寸的减小而引起的红移可归因于结合了声子约束和拉伸应变的影响。当假设量子约束激子在Si纳米晶体中重组时,可以用一致的方式解释这些内在标本的光致发光行为。对于掺杂的nc-Si:H材料的单声子拉曼信号,除了声子限制和拉伸应变的共同作用外,随着掺杂水平的提高,伴随着单声子TO谱带不对称展宽的附加红移可以归因于载流子效应和无序。从掺杂。随着Si纳米晶体平均尺寸的减小或掺杂剂的增加,本征和掺杂样品的两个声子拉曼振幅的衰减可归因于无序。拉曼实验表明,两个声子TO支路的所有能量都不同于一个声子TO有源带的两倍,这表明在波矢k =时,两个声子TO模并非来自拉曼有源声子。 0.两声子横向光学(2TO)模式的峰位移与声子约束和无序有关。本征膜和掺杂膜在温度的TO(2TO)模式下的峰位移可忽略不计,这表明nc-Si:H / c-Si中的界面应变可以忽略。 (c)2006 Elsevier Ltd.保留所有权利。

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