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Phase transition in crown-jewel structured Au-Ir nanoalloys with different shapes: a molecular dynamics study

机译:不同形状的冠珠宝结构金-铱纳米合金的相变:分子动力学研究

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We have studied the melting process for crown-jewel structured Ir-55, Ir54Au, Ir43Au12, Ir25Au30, Ir13Au42, and Au-55 nanoclusters in the icosahedral, Ir-55, Ir54Au, Ir43Au12, Ir19Au36, Ir13Au42, and Au-55 nanoclusters in the cuboctahedral, and Ir-54, Ir53Au, Ir47Au7, Ir17Au37, Ir-7 Au-47, and Au-54 nanoclusters in the decahedral morphologies. We have investigated the different thermodynamic, structural, and dynamical properties for the different nanoclusters in the different structures. Our thermodynamic results indicated that as the concentration of Au atoms in the nanoclusters increases, the absolute value of internal energy, and so the melting points, of the nanoclusters decrease. It is also shown that the Au atoms decrease the melting temperature of the pure cuboctahedral cluster more than that of the other structures. We have also found that the Au atoms were located in favorable positions at the surface sites of nanoalloys. Also, the doping of the Ir nanocluster by Au atoms makes the cluster more stable. It is also found that nanoclusters with different morphologies have almost the same stability. Our structural results indicated that after the melting process, the Au atoms generally tend to lie in the outer shell of the cluster, but the Ir atoms generally tend to lie in the core of the cluster (see the Ir13Au42 and Ir7Au47 nanoclusters, for example). We have also found the interesting result that the Ir7Au47 nanocluster shows a solid-solid transition from a decahedral structure to an icosahedral structure before melting. The Ir43Au12 nanocluster also shows a transformation from a cuboctahedral structure to an icosahedral-like structure before melting. Our dynamical results showed that doping of the Ir-55 cluster with an Au atom sharply increases the self-diffusion coefficient in the initial state in the solid phase, especially in icosahedral and cuboctahedral structures. It is also shown that the Ir13Au42 cluster in icosahedral and cuboctahedral and the Ir7Au47 and Ir17Au37 clusters in decahedral morphologies have smaller values of self-diffusion coefficients than other clusters after the melting point and that this could be due to the formation of core-shell structures.
机译:我们研究了二十面体,Ir-55,Ir54Au,Ir43Au12,Ir19Au36,Ir13Au42和Au-55纳米团簇中冠状宝石结构的Ir-55,Ir54Au,Ir43Au12,Ir25Au30,Ir13Au42和Au-55纳米团簇的熔化过程十面体形态中的立方八面体和Ir-54,Ir53Au,Ir47Au7,Ir17Au37,Ir-7 Au-47和Au-54纳米簇。我们已经研究了不同结构中不同纳米团簇的不同热力学,结构和动力学性质。我们的热力学结果表明,随着纳米团簇中Au原子浓度的增加,纳米团簇的内能绝对值和熔点降低。还表明,金原子比其他结构降低了纯立方八面体簇的熔化温度。我们还发现金原子位于纳米合金表面位置的有利位置。而且,通过Au原子对Ir纳米团簇的掺杂使团簇更加稳定。还发现具有不同形态的纳米团簇具有几乎相同的稳定性。我们的结构结果表明,在熔化过程之后,Au原子通常倾向于位于团簇的外壳中,而Ir原子通常倾向于位于团簇的内核中(例如,参见Ir13Au42和Ir7Au47纳米团簇) 。我们还发现了有趣的结果,即Ir7Au47纳米簇在熔化之前显示出从十面体结构到二十面体结构的固-固过渡。 Ir43Au12纳米簇在熔化前也显示出从立方八面体结构到二十面体状结构的转变。我们的动力学结果表明,在Au-Ir-55团簇中以Au原子掺杂会大大增加固相初始状态下的自扩散系数,尤其是在二十面体和立方八面体结构中。还显示了二十面体和立方八面体中的Ir13Au42团簇以及十面体形态中的Ir7Au47和Ir17Au37团簇在熔点后具有比其他团簇小的自扩散系数值,这可能是由于形成了核-壳结构。

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