Allouti Fayçal, Manceron Laurent, Alikhani Mohammad Esmaïl
Université Pierre et Marie Curie-Paris 6, CNRS Laboratoire de Dynamique, Interactions et Réactivité, UMR 7075 Case 49, 4 Place Jussieu, 75252, Paris Cedex 05, France.
Phys Chem Chem Phys. 2006 Aug 28;8(32):3715-25. doi: 10.1039/b606248b. Epub 2006 Jul 4.
The formation of Ni2O2 can be observed from the condensation of effusive beams of Ni and O2 in neon or argon matrices. Observation of 58Ni(2)16O2, 58Ni60Ni16O2, 60Ni2(16)O2, Ni(2)18O2 and Ni(2)16O18O isotopic data for five fundamental transitions enable a discussion of structural parameters for matrix-isolated Ni2O2 in its cyclic ground state. Analysis of the nickel isotopic effects on the 58,60Ni2(16)O18O fundamentals suggest an elongated rhombic structure with a Ni-O bond force constant (240+/-10 N m-1) and NiONi bond angles around 79 degrees. The latter points to a Ni-Ni internuclear distance shorter than the O-O one. Low-lying singlet, triplet and quintet states have been studied using density functional theory with an unrestricted wave function and broken symmetry formalism. The high spin states and closed shell singlet states have been also investigated at the CCSD(T) level. The Ni2O2 ground state is calculated to be an antiferromagnetic singlet state with all the hybrid functionals. The first order properties (energies, geometry) calculated with a hybrid functional are very similar when different exchange-correlation functionals with different exact exchange fractions are used and the calculated ground state geometry (NiONi bond angle near 80 degrees, NiO bond distance around 179.5 pm) is in good agreement with the experimental estimate. Nevertheless, a correct reproduction of the experimental vibrational properties is found only when a hybrid functional containing an exact exchange fraction in the 0.4-0.5 range is used. The orbital and topological bonding analyses of Ni2O2 reveal that the relatively short Ni-Ni internuclear distance within the molecule should not be interpreted as a remaining metal-metal bonding interaction, but clearly indicate that the bonding driving force is due to the formation of four strong and highly polarized Ni-O bonds. Even in such an early stage of metal oxidation, the Ni-Ni interaction has virtually disappeared.
在氖或氩基质中,通过镍和氧气的喷射束冷凝可观察到Ni2O2的形成。对五个基本跃迁的58Ni(2)16O2、58Ni60Ni16O2、60Ni2(16)O2、Ni(2)18O2和Ni(2)16O18O同位素数据的观察,使得能够对处于环状基态的基质隔离Ni2O2的结构参数进行讨论。对镍同位素效应在58,60Ni2(16)O18O基本跃迁上的分析表明,其结构为拉长的菱形,Ni - O键力常数为(240±10 N m-1),NiONi键角约为79度。后者表明Ni - Ni核间距比O - O核间距短。使用具有无限制波函数和破缺对称性形式的密度泛函理论研究了低能单重态、三重态和五重态。还在CCSD(T)水平上研究了高自旋态和闭壳层单重态。计算得出,所有杂化泛函给出的Ni2O2基态均为反铁磁单重态。当使用具有不同精确交换分数的不同交换关联泛函时,用杂化泛函计算得到的一阶性质(能量、几何结构)非常相似,且计算得到的基态几何结构(NiONi键角接近80度,NiO键距约为179.5 pm)与实验估计值吻合良好。然而,只有当使用精确交换分数在0.4 - 0.5范围内的杂化泛函时,才能正确再现实验振动性质。Ni2O2的轨道和拓扑键分析表明,分子内相对较短的Ni - Ni核间距不应被解释为残留的金属 - 金属键相互作用,而是清楚地表明键合驱动力源于四个强且高度极化的Ni - O键的形成。即使在金属氧化的早期阶段,Ni - Ni相互作用实际上也已消失。