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首页> 外文期刊>Computational & theoretical chemistry >Evaluating common QTAIM and NCI interpretations of the electron density concentration through IQA interaction energies and 1D cross-sections of the electron and deformation density distributions
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Evaluating common QTAIM and NCI interpretations of the electron density concentration through IQA interaction energies and 1D cross-sections of the electron and deformation density distributions

机译:通过IQA相互作用能和电子的一维截面以及变形密度分布评估电子密度浓度的常见QTAIM和NCI解释

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Nine kinds of inter- and intramolecular interactions were investigated by exploring the topology of electron density in the interatomic regions using standard protocols of QTAIM, IQA and NCI techniques as well as in-house developed cross-sections of the electron and deformation density distributions. The first four methods provide the properties of the resultant density distribution in a molecular system whereas the later illustrates the process, inflow or outflow of density from fragments to the interatomic region of an interaction on its formation in a molecular system. We used (i) the QTAIM-defined atomic interaction line, AIL (presence or absence), (ii) IQA-defined interaction energy, E-int(A,B), and its components, classical V-cl(A,B) and exchange-correlation V-XC(A,B) term, (iii) NCI-defined isosurfaces to identify local regions of accumulated (lambda(2) < 0) or depleted (lambda(2) > 0) density relative to immediate environment, and (iv) deformation density for which Delta rho(r) > 0 indicates an inflow or otherwise an outflow of density on the interaction formation to explore the nature of the interactions. We found (i) AILS for highly attractive and repulsive interactions, regardless whether an inflow (Delta rho(r) > 0) or outflow of density into the interatomic region, (ii) no correlation between the signs of lambda(2) and E-int(A,B); both, highly repulsive and attractive, interactions might have locally depleted density and vice versa, (iii) locally accumulated density (lambda(2)< 0) does not imply that this is the result of an inflow (Delta rho(r) > 0) of density and this equally applies to attractive and repulsive interactions either with or without an AIL. Results obtained demonstrate that the molecular environment can change the character of an interaction radically, from (i) attractive to repulsive, (ii) lambda(2) < 0 to lambda(2) > 0, or (iii) Delta rho(r) > 0 to Delta rho(r) < 0; hence, none of the topological indices used here, either separately or combined, can be used to definitely predict the (de)stabilizing nature of an interaction except highly repulsive ones for which the absence of AIL, interatomic density depletion and outflow of density on interaction formation are observed. (C) 2014 Elsevier B.V. All rights reserved.
机译:通过使用QTAIM,IQA和NCI技术的标准协议以及内部开发的电子截面和变形密度分布,通过探索原子间区域中电子密度的拓扑结构,研究了9种分子间和分子间的相互作用。前四种方法提供了分子系统中最终密度分布的性质,而后一种方法则说明了在分子系统中相互作用过程中,从片段到相互作用的原子间区域的密度的流入,流出。我们使用(i)QTAIM定义的原子相互作用线AIL(存在或不存在),(ii)IQA定义的相互作用能E-int(A,B)及其组成部分经典V-cl(A,B) )和交换相关V-XC(A,B)项,(iii)NCI定义的等值面,以识别相对于立即数的累积(lambda(2)<0)或耗尽(lambda(2)> 0)密度的局部区域(iv)变形密度,其中Δrho(r)> 0表示相互作用形成上密度的流入或流出,以探讨相互作用的性质。我们发现(i)AILS具有极强的吸引力和排斥性相互作用,无论是流入(Δrho(r)> 0)还是进入原子间区域的密度流出,(ii)lambda(2)和E的征兆之间都没有相关性-int(A,B);排斥力和吸引力都很高,两者的相互作用都可能具有局部耗尽的密度,反之亦然,(iii)局部累积的密度(lambda(2)<0)并不意味着这是流入的结果(Delta rho(r)> 0密度),这同样适用于有或没有AIL的吸引和排斥相互作用。获得的结果表明,分子环境可以从根本上改变相互作用的特性,从(i)吸引到排斥,(ii)lambda(2)<0到lambda(2)> 0或(iii)Delta rho(r) > 0至Delta rho(r)<0;因此,这里使用的拓扑指数,无论是单独使用还是组合使用,都不能用来明确预测相互作用的(去稳定化)性质,除非是高度排斥性的指数,因为它们不存在AIL,原子间密度耗尽和相互作用时密度流出观察到形成。 (C)2014 Elsevier B.V.保留所有权利。

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