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Comparative Analysis of Process of Diffusion of Interstitial Oxygen Atoms and Interstitial Hydrogen Molecules in Silicon and Germanium Crystals: Quantumchemical Simulation

机译:硅和锗晶体间质氧原子和间质氢分子扩散过程的比较分析:量子化学模拟

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A theoretical modeling and comparative analysis of the process of diffusion of the interstitial oxygen atoms and interstitial hydrogen molecules (H2) in silicon and germanium crystals at normal and hydrostatic pressure (HP) have been performed. The process of diffusion of particle with a strong interaction with a crystal lattice (interstitial oxygen atom) is a cooperative process. Three nearest Si (Ge) atoms of crystal lattice are involved in an elementary oxygen jump from a bond-center site to another bond-center site along a path in the (110) plane. It is precisely their optimum position (corresponding to a local minimum of the crystal total energy) determines the value of the diffusion parameters of an interstitial oxygen atom in silicon and germanium crystals. In a sense, the diffusion process may be considered as a diffusion process of qwasiparticle -^s(Oi+3Si). In the case of a particle weakly interacting with a crystal lattice (interstitial hydrogen molecules) we come up against the opposite case - the diffusion of H2 is not a cooperative process. The calculated values of the activation energy and pre-exponential factor for an interstitial oxygen atom ?′E(Si) = 2.59 eV, ?′E(Ge) = 2.05 eV, D0 (Si)= 0.28 cm2 s-1, D0 (Ge)= 0.39 cm2 s-1 and interstitial hydrogen molecule ?′E(Si) = 0.79 - 0.83 eV, ?′E(Ge) = 0.58 - 0.62 eV D0 (Si)= 7.4 10-4 cm2 s-1, D0 (Ge)= 6.510-4 cm2 s-1 are in an excellent agreement with experimental ones and for the first time describe perfectly an experimental temperature dependence of an interstitial oxygen atom and hydrogen molecules diffusion constant in Si crystals.
机译:已经进行了在正常和静水压力(HP)中硅和锗晶体中的间质氧原子和间质氢分子(H2)扩散过程的理论建模和对比分析。颗粒与晶格(间质氧原子)的强相互作用的扩散过程是合作过程。晶格的三个最接近的Si(Ge)原子沿着(110)平面中的路径从键中心部位跳转到另一个键中心部位。正是其最佳位置(对应于晶体总能量的局部最小能量)确定硅和锗晶体中间质氧原子的扩散参数的值。在某种意义上,扩散过程可以被认为是QWasiparticle-^ S(OI + 3SI)的扩散过程。在颗粒与晶格(间质氢分子)弱相互作用的情况下,我们抵靠相反的情况 - H2的扩散不是协作过程。间质氧原子的激活能量和预指数因子的计算值?'E(Si)= 2.59eV,Δ'e(ge)= 2.05eV,d0(si)= 0.28cm2 s-1,d0( Ge)= 0.39cm 2 s-1和间质氢分子θe(si)= 0.79 - 0.83eV,Δe(ge)= 0.58 - 0.62 EV D0(Si)= 7.4 10-4cm 2 S-1,D0 (GE)= 6.510-4cm 2 S-1与实验性的同一致性,并且首次描述完全描述在Si晶体中的间质氧原子和氢分子扩散常数的实验温度依赖性。

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