Harpale Abhilash, Panesi Marco, Chew Huck Beng
Department of Aerospace Engineering, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA.
J Chem Phys. 2015 Feb 14;142(6):061101. doi: 10.1063/1.4907716.
Using first principle calculations, we study the surface-to-bulk diffusion of C atoms in Ni(111) and Cu(111) substrates, and compare the barrier energies associated with the diffusion of an isolated C atom versus multiple interacting C atoms. We find that the preferential Ni-C bonding over C-C bonding induces a repulsive interaction between C atoms located at diagonal octahedral voids in Ni substrates. This C-C interaction accelerates C atom diffusion in Ni with a reduced barrier energy of ∼1 eV, compared to ∼1.4-1.6 eV for the diffusion of isolated C atoms. The diffusion barrier energy of isolated C atoms in Cu is lower than in Ni. However, bulk diffusion of interacting C atoms in Cu is not possible due to the preferential C-C bonding over C-Cu bonding, which results in C-C dimer pair formation near the surface. The dramatically different C-C interaction effects within the different substrates explain the contrasting growth mechanisms of graphene on Ni(111) and Cu(111) during chemical vapor deposition.
通过第一性原理计算,我们研究了C原子在Ni(111)和Cu(111)衬底中的表面到体相扩散,并比较了与孤立C原子扩散以及多个相互作用C原子扩散相关的势垒能量。我们发现,相对于C-C键,优先形成的Ni-C键会在位于Ni衬底对角八面体空隙处的C原子之间引发排斥相互作用。这种C-C相互作用加速了Ni中C原子的扩散,其势垒能量降低至约1 eV,而孤立C原子扩散的势垒能量约为1.4 - 1.6 eV。孤立C原子在Cu中的扩散势垒能量低于在Ni中的。然而,由于相对于C-Cu键优先形成C-C键,相互作用的C原子在Cu中无法进行体相扩散,这导致在表面附近形成C-C二聚体对。不同衬底内显著不同的C-C相互作用效应解释了化学气相沉积过程中石墨烯在Ni(111)和Cu(111)上生长机制的差异。