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Adatom pair distribution up to half coverage: O-Pd(100)

机译:吸附原子对分布最多覆盖一半:O-Pd(100)

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The superposition approximation and the Born-Green-Yvon (BGY) equation allows calculation of pair distributions in thermal equilibrium from pair potentials. A 2-d variant can be used to derive adatom pair distributions from arbitrary analytical pair potentials. As practical example substrate mediated elastic interactions, fitted previously to first principles (FP) calculations, are used to derive adatom pair distributions of O-Pd(100). The evaluation method utilizes the particle-hole symmetry of the pair interaction lattice gas Hamiltonian. The nonlinear BGY-type integral equation is solved numerically up to half coverage using power series expansion of coverage.The resulting adatom pair- and three-body distributions are used to analyze the short-range order of adatoms. A Monte Carlo (MC) simulation was performed in parallel to compare the current model with established methods. MC derived pair distributions fit well to those found with the analytical model, except in the high coverage region. The Fourier transformed pair correlations are compared with experimental LEED spot data and provide additional insight.Due to significant attraction the model predicts formation of 3rd and 4th nearest neighbors (n,n.) at small 3rd n.n. chains. A long range order of adatoms like a p(2 x 2) lattice is not found with the current model but a glassy structure is proposed as also indicated by the equilibrium Monte Carlo configurations. The glassy structure is assumed to contain fluctuations explaining broad p(2 x 2) LEED spots in the 0.25 monolayer region. The assumptions and limitations of the model towards higher coverages are discussed and open questions are formulated.
机译:通过叠加逼近和Born-Green-Yvon(BGY)方程,可以根据线对电位计算热平衡中的线对分布。二维变体可用于从任意分析对电位导出原子对分布。作为实际示例,预先适应第一原理(FP)计算的基质介导的弹性相互作用可用于得出O-Pd(100)的吸附原子对分布。该评估方法利用了对相互作用晶格气体哈密顿量的粒子-孔对称性。使用覆盖范围的幂级数展开对非线性BGY型积分方程进行数值求解,直至覆盖范围达到一半为止。所得的原子对和三体分布用于分析原子的短程顺序。并行执行了蒙特卡洛(MC)仿真,以将当前模型与已建立的方法进行比较。 MC派生的对分布与分析模型发现的分布非常吻合,除了在高覆盖范围内。将傅立叶变换对对与实验LEED斑点数据进行比较,并提供更多见解。由于具有明显的吸引力,该模型预测在第三小n.n处形成第三和第四最近的邻居(n,n。)。链。在当前模型中未找到像p(2 x 2)晶格这样的长原子级原子,但提出了玻璃状结构,这也由平衡蒙特卡洛构型表示。假定玻璃结构包含波动,解释了在0.25单层区域中的宽p(2 x 2)LEED点。讨论了模型对更高覆盖率的假设和局限性,并提出了未解决的问题。

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