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Self-diffusion in crystalline silicon: A single diffusion activation enthalpy down to 755 ℃

机译:晶体硅中的自扩散:单个扩散激活焓低至755℃

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Self-diffusion in silicon and the contribution of vacancies and self-interstitials have been controversially discussed for 50 yr. Most recent results show that the intrinsic silicon self-diffusion coefficient deviates from an Arrhenius-type, single exponential function for temperatures below 950 ℃ [Y. Shimizu, M. Uematsu, and K. M. Itoh, Phys. Rev. Lett. 98, 095901 (2007); R. Kube, H. Bracht, E. Hueger, H. Schmidt, J. L. Hansen, A. N. Larsen, J. W. Ager, E. E. Haller, T. Geue, and J. Stahn, Phys. Rev. B 88, 085206 (2013)]. This led us to propose temperature-dependent thermodynamic properties of vacancies in order to achieve full consistency to vacancy-mediated dopant diffusion in silicon. Concepts of temperature-dependent properties of native defects or distinct forms of defects with different formation entropies suggested by Cowern et al. [N. E. B. Cowern, S. Simdyankin, C. Ahn, N. S. Bennett, J. P. Goss, J.-M. Hartmann, A. Pakfar, S. Hamm, J. Valentin, E. Napolitani, D. De Salvador, E. Bruno, and S. Mirabella, Phys. Rev. Lett. 110,155501 (2013)] question the present understanding on atomic transport in semiconductors. To verify these concepts, additional self-diffusion experiments under particular gettering conditions were performed. As a result, silicon self-diffusion was found to be accurately described by one single diffusion activation enthalpy of (4.73 ± 0.02) eV down to 755 ℃. This provides full consistency to dopant diffusion without claiming native-defect concepts that were originally proposed by Seeger and Chik in 1968 [A. Seeger and K. P. Chik, Phys. Stat. Sol. 29, 455 (1968)] and confirms most recent density functional theory calculations on the activation energy of self-diffusion via vacancies and self-interstitials. Overall, this unravels the old debate of self-diffusion in silicon with the supposed intrinsic temperature dependence.
机译:在硅中的自扩散以及空位和自填隙的贡献已讨论了50年。最新的结果表明,在温度低于950℃时,本征硅的自扩散系数与Arrhenius型单指数函数有所不同[Y. Shimizu,M。Uematsu和K.M. Itoh,物理学牧师98,095901(2007); R.Kube,H.Braccht,E.Hueger,H.Schmidt,J.L.Hansen,A.N.Larsen,J.W.Ager,E.E.Haller,T.Geue和J.Stahn,Phys。 B 88,085206(2013)。因此,我们提出了空位的温度依赖性热力学性质,以实现空位介导的掺杂剂在硅中扩散的完全一致性。 Cowern等人提出了天然缺陷或具有不同形成熵的缺陷的不同形式的温度相关性质的概念。 [N. E. B. Cowern,S。Simdyankin,C。Ahn,N。S. Bennett,J。P. Goss,J.-M。 Hartmann,A。Pakfar,S。Hamm,J。Valentin,E。Napolitani,D。De Salvador,E。Bruno和S. Mirabella,物理。牧师110,155501(2013)]质疑目前对半导体中原子传输的理解。为了验证这些概念,在特定的吸气条件下进行了另外的自扩散实验。结果,发现硅的自我扩散可以通过低至755℃(4.73±0.02)eV的单个扩散活化焓来准确描述。这就为掺杂剂扩散提供了完全的一致性,而没有声称Seeger和Chik最初于1968年提出的自然缺陷概念[A. Seeger和K. P. Chik,物理学。统计索尔29,455(1968)],并证实了最新的密度泛函理论计算,涉及通过空位和自填隙子的自我扩散的活化能。总的来说,这揭开了关于硅自扩散与固有温度相关性的古老争论。

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