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Revisiting electroaccepting and electrodonating powers: proposals for local electrophilicity and local nucleophilicity descriptors

机译:再次探讨电接受能力和供电能力:关于局部亲电性和局部亲核性描述符的建议

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The electrophilicity index, μ~2/2η, where μ is the chemical potential and n is the hardness, has been defined by Parr, Von Szentpaly, and Liu (J. Am. Chem. Soc. 1999, 121, 1922) as the lowering in energy of an electronic system during a process in which the chemical potential of the system raises from μ to zero, accepting -μ/η electrons. In this work, it is shown that the electrophilicity index is also a rational choice for measuring nucleophilicity. Indeed, within the grand canonical ensemble, when the chemical potential of a system increases from n to zero, the system gives away μ/η electrons. During the process, the variation of the grand potential is μ~2/2η. Additionally, through the use of a second order Taylor series expansion of the density as a function of the number of electrons, at constant external potential, which depends on the Fukui function and the dual descriptor, the local electrophilicity is defined as the actual variation of the electron density when the system acquires -μ/η electrons, while the local nucleophilicity is similarly defined for the case when the system loses μ/η electrons.
机译:亲电性指数μ〜2 /2η,其中μ是化学势,n是硬度,由Parr,Von Szentpaly和Liu(J. Am。Chem。Soc。1999,121,1922)定义为在系统的化学势从μ上升到零并接受-μ/η电子的过程中降低电子系统的能量。在这项工作中,表明亲电指数也是测量亲核性的合理选择。实际上,在大正则合奏中,当系统的化学势从n增加到零时,系统释放出μ/η电子。在此过程中,大势的变化为μ〜2 /2η。此外,通过在恒定的外部电势下使用二阶泰勒级数随电子数量变化的密度展开式(取决于Fukui函数和对偶描述符),将局部亲电性定义为电子的实际变化系统获得-μ/η电子时的电子密度,而系统失去μ/η电子时的局部亲核性也被类似地定义。

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