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Thermal generation of vacancies from voids in aluminium

机译:由铝中的空隙热产生空位

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The thermal generation kinetics of vacancies from octahedral voids in aluminium has been studied by the measurement of residual resistance due to vacancies generated during pulse heating of the specimen for short time, and also by electron microscopic observation of the voids. The vacancy generation curves saturated at the levels of 3.2 Delta rho (o) and 2.3 Delta rho (o) for the voids with edge length l = 6 nm at 543 K and 573 K, respectively, where Delta rho (o) is the resistivity due to the thermal equilibrium concentration of vacancies. For the voids with edge length l = 17 nm the generation curves saturated at the levels of (1.02-1.05)Delta rho (o) for both temperatures. These results are consistent with a newly proposed model that takes account of diffusion limited vacancy generation from the edge and the surface parts of the voids, with the respective promotive energies of vacancy formation DeltaE and epsilon. The new model yielded the best rt value sets DeltaE = 0.16 +/- 0.01) eV and epsilon = 0 for the voids with l = 6 nm, and DeltaE = (0.04 +/- 0.01) eV and epsilon = 0 for l = 17 nm voids. These results indicate that the contribution from the surface part to the vacancy generation curves is dominant in the large voids, while the contribution from the edge part becomes significant in the small voids. [References: 11]
机译:铝的八面体空位的空位的热生成动力学已经通过测量由于在短时间脉冲加热样品期间产生的空位而引起的残余电阻,以及通过电子显微镜观察到的空位来进行研究。空位生成曲线分别在543 K和573 K处的边长为l = 6 nm的空洞处分别处于3.2Δrho(o)和2.3Δrho(o)的水平,其中Δrho(o)是电阻率由于空位的热平衡集中。对于边缘长度为l = 17 nm的空隙,在两个温度下,生成曲线均在(1.02-1.05)Δrho(o)的水平上饱和。这些结果与新提出的模型一致,该模型考虑了从空隙的边缘和表面部分扩散受限的空位生成,并具有空位形成DeltaE和epsilon的各自促进能。对于l = 6 nm的空隙,新模型产生了最佳的rt值集DeltaE = 0.16 +/- 0.01)eV和epsilon = 0,而对于l = 17,DeltaE =(0.04 +/- 0.01)eV和epsilon = 0纳米空隙。这些结果表明,从表面部分到空位产生曲线的贡献在大的空隙中占主导,而从边缘部分的贡献在小空隙中变得显着。 [参考:11]

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