A previously proposed non-canonical coupled-perturbed Kohn-Sham density functional theory (KS-DFT)/Hartree-Fock (HF) treatment for spin-orbit coupling is here generalized to infinite periodic systems. The scalar-relativistic periodic KS-DFT/HF solution, obtained with a relativistic effective core potential, is taken as the zeroth-order approximation. Explicit expressions are given for the total energy through 3rd-order, which satisfy the 2N + 1 rule (i.e. requiring only the 1st-order perturbed wave function for determining the energy through 3rd-order). Expressions for additional 2nd-order corrections to the perturbed wave function (as well as related one-electron properties) are worked out at the uncoupled-perturbed level of theory. The approach is implemented in the \textsc{Crystal} program and validated with calculations of the total energy, electronic band structure, and density variables of spin-current DFT on the tungsten dichalcogenide hexagonal bilayer series (i.e. WSe$_2$, WTe$_2$, WPo$_2$, WLv$_2$), including 6p and 7p elements as a stress test. The computed properties through second- or third-order match well with those from reference two-component self-consistent field (2c-SCF) calculations. For total energies, $E^{(3)}$ was found to consistently improve the agreement against the 2c-SCF reference values. For electronic band structures, visible differences w.r.t. 2c-SCF remained through second-order in only the single-most difficult case of WLv$_2$. As for density variables of spin-current DFT, the perturbed electron density, being vanishing in first-order, is the most challenging for the perturbation theory approach. The visible differences in the electron densities are, however, largest close to the core region of atoms and smaller in the valence region. Perturbed spin-current densities, on the other hand, are well reproduced in all tested cases.
Equation of state and Raman-active $E_{2g}$ lattice phonon in phases I, II, and III of solid hydrogen and deuterium
我们提出的$P-V$状态方程的晶格动力学计算的结果和拉曼活性$E_{2g}$晶格声子的压力依赖性$p-$ H $_2$和$o-$ D $_2$在一个宽的压力范围高达$\sim$ 2兆巴使用我们最近开发的半经验多体势，和密度泛函理论。与现有的实验和理论结果的比较表明，所采用的多体势是一个可靠的基础，高精度计算的第一，第二和第三阶段的固体氢。
