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Communication: Convergence of many-body wave-function expansions using a plane-wave basis in the thermodynamic limit

机译:交流:在热力学极限中使用平面波为基础的多体波函数展开的收敛

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摘要

Basis set incompleteness error and finite size error can manifest concurrently in systems for which the two effects are phenomenologically well-separated in length scale. When this is true, we need not necessarily remove the two sources of error simultaneously. Instead, the errors can be found and remedied in different parts of the basis set. This would be of great benefit to a method such as coupled cluster theory since the combined cost of n(occ)(6)n(virt)(4) could be separated into n(occ)(6) and n(virt)(4) costs with smaller prefactors. In this Communication, we present analysis on a data set due to Baardsen and co-workers, containing 2D uniform electron gas coupled cluster doubles energies for r(s) = 0.5, 1.0, and 2.0 a. u. at a wide range of basis set sizes and particle numbers. In obtaining complete basis set limit thermodynamic limit results, we find that within a small and removable error the above assertion is correct for this simple system. We then use this method to obtain similar results for the 3D electron gas at r(s) = 1.0, 2.0, and 5.0 a. u. and make comparison to the Ceperley-Alder quantum Monte Carlo results. This approach allows for the combination of methods which separately address finite size effects and basis set incompleteness error. Published by AIP Publishing.
机译:基集不完全性误差和有限大小误差可以在长度效应的现象学上很好地分开的两个系统中同时出现。当这是事实时,我们不必同时消除两个错误源。相反,可以在基础集的不同部分中找到并纠正错误。由于n(occ)(6)n(virt)(4)的组合成本可以分为n(occ)(6)和n(virt)( 4)具有较小因素的成本。在本交流中,我们对由于Baardsen及其同事而产生的数据集进行了分析,其中包含2个均匀的电子气耦合的团簇,使r(s)= 0.5、1.0和2.0 a的能量加倍。你具有各种基本尺寸和颗粒数。在获得完整的基准集极限热力学极限结果时,我们发现在一个小的可移动误差内,上述断言对于这个简单的系统是正确的。然后,我们使用此方法在r(s)= 1.0、2.0和5.0 a时获得3D电子气的相似结果。你并与Ceperley-Alder量子Monte Carlo结果进行比较。这种方法允许将分别解决有限大小效应和基集不完整性误差的方法组合在一起。由AIP Publishing发布。

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