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Precise all-electron dynamical response functions: Application to COHSEX and the RPA correlation energy

机译:精确的全电子动力学响应函数:在COHSEX和RPA相关能量中的应用

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We present a methodology to calculate frequency and momentum dependent all-electron response functions determined within Kohn-Sham density functional theory. It overcomes the main obstacle in calculating response functions in practice, which is the slow convergence with respect to the number of unoccupied states and the basis-set size. In this approach, the usual sum-over-states expression of perturbation theory is complemented by the response of the orbital basis functions, explicitly constructed by radial integrations of frequency-dependent Sternheimer equations. To an essential extent an infinite number of unoccupied states are included in this way. Furthermore, the response of the core electrons is treated virtually exactly, which is out of reach otherwise. The method is an extension of the recently introduced incomplete-basis-set correction (IBC) [Betzinger et al, Phys. Rev. B 85,245124 (2012); 88,075130 (2013)] to the frequency and momentum domain. We have implemented the generalized IBC within the all-electron full-potential linearized augmented-plane-wave method and demonstrate for rocksalt BaO the improved convergence of the dynamical Kohn-Sham polarizability. We apply this technique to compute (a) quasiparticle energies employing the COHSEX approximation for the self-energy of many-body perturbation theory and (b) all-electron RPA correlation energies. It is shown that the favorable convergence of the polarizability is passed over to the COHSEX and RPA calculation.
机译:我们提出一种方法来计算在Kohn-Sham密度泛函理论内确定的频率和动量相关的全电子响应函数。它克服了在实践中计算响应函数的主要障碍,即相对于未占用状态数和基集大小的缓慢收敛。在这种方法中,扰动理论中通常的求和状态表示法是由轨道基函数的响应所补充的,该函数是通过频率相关的Sternheimer方程的径向积分而明确构造的。在很大程度上,以这种方式包括了无数个未占用状态。此外,实际上对核心电子的响应进行了精确处理,否则将无法实现。该方法是最近引入的不完全基集校正(IBC)的扩展[Betzinger等,Phys。 B版本85,245124(2012); 88,075130(2013)]应用于频率和动量域。我们已经在全电子全势线性化增强平面波方法中实施了广义IBC,并为岩盐BaO证明了动态Kohn-Sham极化率的改进的收敛性。我们应用该技术来计算(a)多体摄动理论的自能量采用COHSEX近似法计算的准粒子能量,以及(b)全电子RPA相关能量。结果表明,极化率的有利收敛被传递到了COHSEX和RPA计算中。

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