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首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Density functional with full exact exchange, balanced nonlocality of correlation,and constraint satisfaction
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Density functional with full exact exchange, balanced nonlocality of correlation,and constraint satisfaction

机译:具有完全精确交换的密度泛函,相关性的平衡非局部性和约束满足

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摘要

We construct a nonlocal density functional approximation with full exact exchange, while preserving theconstraint-satisfaction approach and justified error cancellations of simpler semilocal functionals. This isachieved by interpolating between different approximations suitable for two extreme regions of the electrondensity. In a "normal" region, the exact exchange-correlation hole density around an electron is semilocalbecause its spatial range is reduced by correlation and because it integrates over a narrow range to —1. Theseregions are well described by popular semilocal approximations (many of which have been constructed non-empirically), because of proper accuracy for a slowly varying density or because of error cancellation betweenexchange and correlation. "Abnormal" regions, where nonlocality is unveiled, include those in which exchangecan dominate correlation (one-electron, nonuniform high density, and rapidly varying limits), and those opensubsystems of fluctuating electron number over which the exact exchange-correlation hole integrates to a valuegreater than -1. Regions between these extremes are described by a hybrid functional mixing exact andsemilocal exchange energy densities locally, i.e., with a mixing fraction that is a function of position r and afunctional of the density. Because our mixing fraction tends to 1 in the high-density limit, we employ full exactexchange according to the rigorous definition of the exchange component of any exchange-correlation energyfunctional. Use of full exact exchange permits the satisfaction of many exact constraints, but the nonlocality ofexchange also requires balanced nonlocality of correlation. We find that this nonlocality can demand at leastfive empirical parameters, corresponding roughly to the four kinds of abnormal regions. Our local hybridfunctional is perhaps the first accurate fourth-rung density functional or hyper-generalized gradient approxi-mation, with full exact exchange, that is size-consistent in the way that simpler functionals are. It satisfies otherknown exact constraints, including exactness for all one-electron densities, and provides an excellent fit to the223 molecular enthalpies of formation of the G3/99 set and the 42 reaction barrier heights of the BH42/03 set,improving both (but especially the latter) over most semilocal functionals and global hybrids. Exact con-straints, physical insights, and paradigm examples hopefully suppress "overfitting."
机译:我们构造具有完全精确交换的非局部密度泛函逼近,同时保留约束满足方法和较简单的半局部泛函的合理误差消除。这是通过在适合电子密度的两个极端区域的不同近似值之间进行插值来实现的。在“正常”区域中,电子周围的确切交换相关空穴密度是半局部的,因为其空间范围会因相关性而减小,并且因为它会在一个狭窄的范围内积分到-1。这些区域可以通过流行的半局部逼近来很好地描述(其中许多是非经验构造的),这是因为对于缓慢变化的密度具有适当的精度,或者由于交换和相关之间的误差抵消。揭示非局部性的“异常”区域包括那些交换能主导相关性的区域(单电子,非均匀的高密度和快速变化的极限),以及那些波动的电子数的开放子系统,在该子系统上精确的交换相关孔集成到一个值大于-1。这些极值之间的区域通过混合功能混合精确和局部局部交换能量密度来描述,即混合分数是位置r的函数和密度的函数。因为我们的混合分数在高密度极限中趋于1,所以我们根据任何交换相关能量函数的交换成分的严格定义进行完全精确交换。使用完全精确交换可以满足许多精确约束,但是交换的非局限性也需要相关性的平衡非局限性。我们发现,这种非局部性至少需要五个经验参数,大致对应于四种异常区域。我们的本地混合函数可能是第一个准确的四阶密度函数或超广义梯度近似,具有完全精确的交换,即在尺寸上与较简单的函数一致。它满足了其他已知的严格约束条件,包括所有单电子密度的精确度,并且非常适合G3 / 99分子组形成的223个分子焓和BH42 / 03分子组形成的42个反应势垒高度,这两个方面都得到了改善(但特别是后者)覆盖大多数半局部功能和全局混合。确切的约束,物理见解和范例示例有望消除“过度拟合”。

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