Kieken Laurent D, Neurock Matthew, Mei Donghai
NovoDynamics, Inc., 123 North Ashley Street, Suite 210, Ann Arbor, Michigan 48104, USA.
J Phys Chem B. 2005 Feb 17;109(6):2234-44. doi: 10.1021/jp048865c.
An ab initio-based kinetic Monte Carlo algorithm was developed to simulate the direct decomposition of NO over Pt and different PtAu alloy surfaces. The algorithm was used to test the influence of the composition and the specific atomic surface structure of the alloy on the simulated activity and selectivity to form N2. The apparent activation barrier found for the simulation of lean NO decomposition over Pt(100) was 7.4 kcal/mol, which is lower than the experimental value of 11 kcal/mol that was determined over supported Pt nanoparticles. Differences are likely due to differences in the surface structure between the ideal (100) surface and supported Pt particles. The apparent reaction orders for lean NO decomposition over the Pt(100) substrate were calculated to be 0.9 and -0.5 for NO and O2, respectively. Oxygen acts to poison Pt. Simulations on the different Pt-Au(100) surface alloys indicate that the turnover frequency goes through a maximum as the Au composition in the surface is increased, and the maximum occurs near 44% Au. Turnover frequencies, however, are dictated by the actual arrangements of Pt and Au atoms in the surface rather than by their overall composition. Surfaces with similar compositions but different alloy arrangements can lead to very different activities. Surfaces composed of 50% Pt and 50% Au (Pt4 and Au4 surface ensembles) showed very little enhancement in the activity over that which was found over pure Pt. The Pt-Pt bridge sites required for NO adsorption and decomposition were still effectively poisoned by atomic oxygen. The well-dispersed Pt(50%)Au(50%) alloy, on the other hand, increased the TOF over that found for pure Pt by a factor of 2. The most active surface alloy was one in which the Pt was arranged into "+" ensembles surrounded by Au atoms. The overall composition of this surface is Pt(56.2%)Au(43.8%). The unique "+" ensembles maintain Pt bridge sites for NO to adsorb on but limit O2 as well as NO activation by eliminating next-nearest neighbor Pt-bridge sites. The repulsive interactions between two adatoms prevent them from sharing the same metal atoms. The decrease in the oxygen coverage leads to a greater number of vacant sites available for NO adsorption. This increases the NO coupling reaction and hence N2 formation. The inhibition of the rate of N2 formation by O2 is therefore suppressed. The coverage of atomic oxygen decreases from 53% on the Pt(100) surface down to 19% on the "+" ensemble surface. This increases the rate of N2 formation by a factor of 4.3 over that on pure Pt. The reaction kinetics over the "+" ensemble Pt(56.2%)Au(43.8%) surface indicate apparent reaction orders in NO and oxygen of 0.7 and 0.0, respectively. This suggests that oxygen does not poison the PtAu "+" alloy ensemble. The activity and selectivity of the PtAu ensembles significantly decrease for alloys that go beyond 60% Au. Higher coverages of Au shut down sites for NO adsorption and, in addition, weaken the NO and O bond strengths, which subsequently promotes desorption as well as NO oxidation. The computational approach identified herein can be used to more rapidly test different metal compositions and their explicit atomic arrangements for improved catalytic performance. This can be done "in silico" and thus provides a method that may aid high-throughput experimental efforts in the design of new materials. The synthesis and stability of the metal complexes suggested herein still ultimately need to be tested.
开发了一种基于从头算的动力学蒙特卡罗算法,用于模拟NO在Pt及不同PtAu合金表面上的直接分解。该算法用于测试合金的组成和特定原子表面结构对模拟活性以及生成N2的选择性的影响。在Pt(100)上模拟贫燃NO分解时发现的表观活化能垒为7.4 kcal/mol,低于在负载型Pt纳米颗粒上测定的11 kcal/mol的实验值。差异可能是由于理想(100)表面与负载型Pt颗粒之间的表面结构不同。计算得出在Pt(100)基底上贫燃NO分解时,NO和O2的表观反应级数分别为0.9和 -0.5。氧会使Pt中毒。对不同的Pt-Au(100)表面合金进行的模拟表明,随着表面Au组成的增加,周转频率会达到最大值,且最大值出现在Au含量接近44%时。然而,周转频率取决于表面上Pt和Au原子的实际排列,而非它们的总体组成。组成相似但合金排列不同的表面可能导致活性差异很大。由50% Pt和50% Au组成的表面(Pt4和Au4表面组合)的活性相较于纯Pt几乎没有增强。NO吸附和分解所需的Pt-Pt桥位仍然被原子氧有效中毒。另一方面,充分分散的Pt(50%)Au(50%)合金使周转频率比纯Pt提高了2倍。最具活性的表面合金是其中Pt排列成被Au原子包围的“+”组合的合金。该表面的总体组成为Pt(56.2%)Au(43.8%)。独特的“+”组合保留了供NO吸附的Pt桥位,但通过消除次近邻的Pt桥位限制了O2以及NO的活化。两个吸附原子之间的排斥相互作用阻止它们共享相同的金属原子。氧覆盖率的降低导致有更多空位可用于NO吸附。这增加了NO偶联反应,进而促进了N2的形成。因此,O2对N2形成速率的抑制作用得到了抑制。原子氧的覆盖率从Pt(1)表面的53%降至“+”组合表面的19%。这使得N2形成速率比纯Pt提高了4.3倍。在“+”组合Pt(56.2%)Au(43.8%)表面上的反应动力学表明,NO和氧的表观反应级数分别为0.7和0.0。这表明氧不会使PtAu“+”合金组合中毒。对于Au含量超过60%的合金,PtAu组合的活性和选择性显著降低。更高的Au覆盖率会关闭NO吸附位点,此外,还会削弱NO和O的键强度,这随后会促进脱附以及NO氧化。本文确定的计算方法可用于更快速地测试不同的金属组成及其明确的原子排列,以提高催化性能。这可以在“计算机模拟”中完成,从而提供一种可能有助于高通量实验努力进行新材料设计的方法。本文提出的金属配合物的合成和稳定性最终仍需进行测试。