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从真空到水合状态的离子极化率变化:来自 Hirshfeld 分割的见解。

Variation of ion polarizability from vacuum to hydration: insights from Hirshfeld partitioning.

机构信息

Department of Chemistry and Biochemistry, University of Delaware, Newark, Delaware 19716, USA.

出版信息

J Phys Chem A. 2010 Sep 2;114(34):8984-92. doi: 10.1021/jp103691w.

Abstract

The results of iterative Hirshfeld partitioning on the polarizability of monovalent anions (F(-), Cl(-), and Br(-)) and Na(+) in water clusters ranging from n = 0 to n = 25 are presented. In each case, the ions reach a limiting intrinsic polarizability in the fully hydrated state. For F(-), Cl(-), and Br(-) using B3LYP/aug-cc-pVDZ, the intrinsic polarizabilities in the condensed-phase limit are 47.2 +/- 0.7%, 47.2 +/- 0.3%, and 54.2 +/- 0.4% of their gas-phase value at the corresponding level of theory. The extent of this scaling depends on the basis set (we also consider B3LYP/aug-cc-pVTZ), but intrinsic polarizabilities are generally within 35-55% of the gas-phase value. The sodium cation is the least polarizable in the condensed-phase limit. The average intrinsic polarizability of water in these clusters decreases with the size of the cluster, which is consistent with earlier Hirshfeld analysis of intrinsic polarizabilities of pure water (Krishtal, A.; Senet, P.; Yang, M.; van Alsenoy, C. J. Chem. Phys. 2006, 125, 034312). Further analysis demonstrates that water molecules near ions in sufficiently large clusters (n = 25) have intrinsic polarizabilities similar to those of water molecules fully coordinated in a pure aqueous cluster. The observed binodal distribution of the water intrinsic polarizability within the cluster is attributed to polarizability differences between interior and exterior water molecules. This observation is in qualitative agreement with arguments based on Pauli's exclusion principle that suggest a reduced polarizability for condensed-phase water relative to the vacuum value.

摘要

呈现了单价阴离子(F(-)、Cl(-) 和 Br(-))和 Na(+)在水团簇中从 n = 0 到 n = 25 的极化率的迭代 Hirshfeld 分区的结果。在每种情况下,离子在完全水合状态下达到了有限的固有极化率。对于 B3LYP/aug-cc-pVDZ 中的 F(-)、Cl(-) 和 Br(-),凝聚相极限中的固有极化率分别为相应理论气相值的 47.2 +/- 0.7%、47.2 +/- 0.3%和 54.2 +/- 0.4%。这种缩放的程度取决于基组(我们还考虑 B3LYP/aug-cc-pVTZ),但固有极化率通常在气相值的 35-55%之间。钠离子在凝聚相极限中是最非极化的。这些簇中水分子的平均固有极化率随簇的大小而降低,这与先前对纯水固有极化率的 Hirshfeld 分析一致(Krishtal,A.;Senet,P.;Yang,M.;van Alsenoy,C. J. Chem. Phys. 2006, 125, 034312)。进一步的分析表明,在足够大的簇(n = 25)中,离子附近的水分子具有与完全配位在纯水溶液簇中的水分子相似的固有极化率。在簇内观察到的水分子固有极化率的二相分布归因于内外水分子之间的极化率差异。这一观察结果与基于 Pauli 排除原理的论点定性一致,该论点表明相对于真空值,凝聚相水的极化率降低。

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