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重新审视电子接受和电子给予能力:关于局部亲电性和局部亲核性描述符的建议

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

作者信息

Morell Christophe, Gázquez José L, Vela Alberto, Guégan Frédéric, Chermette Henry

机构信息

Université de Lyon, Université Lyon 1(UCBL) et UMR CNRS 5280 Sciences Analytiques, 5 rue de la Doua, F-69622 Villeurbanne Cedex, France.

出版信息

Phys Chem Chem Phys. 2014 Dec 28;16(48):26832-42. doi: 10.1039/c4cp03167a.

Abstract

The electrophilicity index, μ(2)/2η, where μ is the chemical potential and η 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 μ 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.

摘要

亲电指数,即μ(2)/2η,其中μ为化学势,η为硬度,是由帕尔、冯·森特帕利和刘(《美国化学会志》,1999年,121卷,1922页)定义的,它表示在一个电子系统的化学势从μ升高到零并接受-μ/η个电子的过程中,该电子系统能量的降低。在这项工作中,结果表明亲电指数也是衡量亲核性的合理选择。实际上,在巨正则系综中,当一个系统的化学势从μ增加到零时,该系统会给出μ/η个电子。在这个过程中,巨势的变化为μ(2)/2η。此外,通过使用密度作为电子数的函数在恒定外势下的二阶泰勒级数展开(这取决于福井函数和双描述符),局部亲电性被定义为当系统获得-μ/η个电子时电子密度的实际变化,而局部亲核性则类似地定义为系统失去μ/η个电子的情况。

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