首页> 外文期刊>Journal of Computational Methods in Sciences and Engineering >Molecular geometry, charge distribution and polarization in platinum nitrides. An ab initio and density functional theory study of PtNN, PtPtNN, NPtPtN, and NNPtNN
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Molecular geometry, charge distribution and polarization in platinum nitrides. An ab initio and density functional theory study of PtNN, PtPtNN, NPtPtN, and NNPtNN

机译:氮化铂中的分子几何结构,电荷分布和极化。 PtNN,PtPtNN,NPtPtN和NNPtNN的从头算和密度泛函理论研究

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We have calculated molecular geometries, atomic charges, dipole moments and polarizabilities for the linear platinum nitrides PtNN, PtPtNN, PtNNPt and NNPtNN. The calculation of the electric properties relies on finite-field M011er-Plesset perturbation theory and Coupled Cluster techniques. Our best values for the polar PtNN and PtPtNN molecules are calculated at the CCSD(T) level of theory and are μ/ea_0 = -0.7089 (PtNN) and -0.1196 (PtPtNN), α/e~2 a_0~2E_h~(-1) = 56.60 (PtNN) and 123.06 (PtPtNN), Δα/e~2a_0~2E_h~(-1) = 27.40 (PtNN) and 68.18 (PtPtNN). For PtNNPt and NNPtNN we obtain α/e~2a_0~2E_h~(-1) = 120.51 (PtNN) and 79.02 (PtPtNN), Δα/e~2a_0~2E_h~(-1) = 116.38 (PtNN) and 76.75 (PtPtNN). Compared to the best values, the performance of the DFT methods is rather erratic.
机译:我们已经计算了线性氮化铂PtNN,PtPtNN,PtNNPt和NNPtNN的分子几何结构,原子电荷,偶极矩和极化率。电特性的计算依赖于有限域M011er-Plesset微扰理论和耦合簇技术。我们对极性PtNN和PtPtNN分子的最佳值是在CCSD(T)的理论水平上计算得出的,即μ/ ea_0 = -0.7089(PtNN)和-0.1196(PtPtNN),α/ e〜2 a_0〜2E_h〜(- 1)= 56.60(PtNN)和123.06(PtPtNN),Δα/ e〜2a_0〜2E_h〜(-1)= 27.40(PtNN)和68.18(PtPtNN)。对于PtNNPt和NNPtNN,我们获得α/ e〜2a_0〜2E_h〜(-1)= 120.51(PtNN)和79.02(PtPtNN),Δα/ e〜2a_0〜2E_h〜(-1)= 116.38(PtNN)和76.75(PtPtNN )。与最佳值相比,DFT方法的性能相当不稳定。

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