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Self Diffusion in Liquid Titanium: Quasielastic Neutron Scattering and Molecular Dynamics Simulation

机译:液体钛中的自扩散:拟力中子散射和分子动力学模拟

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Self diffusion in liquid titanium was measured at 2000 K by quasielastic neutron scattering (QNS) in combination with container less processing via electromagnetic levitation. At small wavenumbers q the quasielastic signal is dominated by incoherent scattering. Up to about 1.2 A~(-1) the width of the quasielastic line exhibits a q~2 dependence as expected for long range atomic transport, thus allowing to measure the self diffusion coefficient D_(Ti) As a result the value D_(Ti) = (5.3 ± 0.2) × 10~(-9) m~2s~(-1) was obtained. With a molecular dynamics (MD) computer simulation using an embedded atom model (EAM) for Ti, the self diffusion coefficient is determined from the mean square displacement as well as from the decay of the incoherent intermediate scattering function at different q. By comparing both methods, we show that the hydrodynamic prediction of a q~2 dependence indeed extends up to about 1.2 A~(-1). Since this result does not depend significantly on the details of the interatomic potential, our findings show that accurate values of self diffusion coefficients in liquid metals can be measured by QNS on an absolute scale.
机译:在液态钛自扩散在2000K的测量通过在组合准弹性中子散射(QNS)与容器较少经由电磁悬浮处理。在小波数q上的准弹性信号被非相干散射。至多约1.2 A〜(-1)的准弹性线展品水溶液〜2依赖性预期长范围原子传输,从而允许以测量自扩散系数D_(Ti)的作为结果的值D_的宽度(Ti)的=(5.3±0.2)×10〜(-9)米〜2秒〜(-1)获得。与使用钛的嵌入原子模型(EAM)的分子动力学(MD)的计算机模拟中,自扩散系数是从均方位移以及从在不同q中的非相干散射中间函数的衰减来确定。通过比较这两种方法,我们表明,A Q〜2依赖的流体动力学预测确实向上延伸至约1.2 A〜(-1)。由于这个结果不会对相互作用势的细节显著依赖,我们的研究结果表明,在液态金属自扩散系数的准确值可以通过QNS从绝对规模来衡量。

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