Pavošević Fabijan, Culpitt Tanner, Hammes-Schiffer Sharon
Department of Chemistry, Yale University, 225 Prospect Street, New Haven, Connecticut 06520, United States.
Chem Rev. 2020 May 13;120(9):4222-4253. doi: 10.1021/acs.chemrev.9b00798. Epub 2020 Apr 13.
In multicomponent quantum chemistry, more than one type of particle is treated quantum mechanically with either density functional theory or wave function based methods. In particular, the nuclear-electronic orbital (NEO) approach treats specified nuclei, typically hydrogen nuclei, on the same level as the electrons. This approach enables the incorporation of nuclear quantum effects, such as nuclear delocalization, anharmonicity, zero-point energy, and tunneling, as well as non-Born-Oppenheimer effects directly into quantum chemistry calculations. Such effects impact optimized geometries, molecular vibrational frequencies, reaction paths, isotope effects, and dynamical simulations. Multicomponent density functional theory (NEO-DFT) and time-dependent DFT (NEO-TDDFT) achieve an optimal balance between computational efficiency and accuracy for computing ground and excited state properties, respectively. Multicomponent wave function based methods, such as the coupled cluster singles and doubles (NEO-CCSD) method for ground states and the equation-of-motion counterpart (NEO-EOM-CCSD) for excited states, attain similar accuracy without requiring any parametrization and can be systematically improved but are more computationally expensive. Variants of the orbital-optimized perturbation theory (NEO-OOMP2) method achieve nearly the accuracy of NEO-CCSD for ground states with significantly lower computational cost. Additional approaches for computing excited electronic, vibrational, and vibronic states include the delta self-consistent field (NEO-ΔSCF), complete active space SCF (NEO-CASSCF), and nonorthogonal configuration interaction methods. Multireference methods are particularly important for describing hydrogen tunneling processes. Other types of multicomponent systems, such as those containing electrons and positrons, have also been studied within the NEO framework. The NEO approach allows the incorporation of nuclear quantum effects and non-Born-Oppenheimer effects for specified nuclei into quantum chemistry calculations in an accessible and computationally efficient manner.
在多组分量子化学中,使用密度泛函理论或基于波函数的方法对不止一种类型的粒子进行量子力学处理。特别是,核电子轨道(NEO)方法将特定的原子核(通常是氢原子核)与电子置于同一水平进行处理。这种方法能够将核量子效应(如核离域、非谐性、零点能和隧穿)以及非玻恩 - 奥本海默效应直接纳入量子化学计算。这些效应会影响优化的几何结构、分子振动频率、反应路径、同位素效应和动力学模拟。多组分密度泛函理论(NEO - DFT)和含时密度泛函理论(NEO - TDDFT)分别在计算基态和激发态性质时,在计算效率和准确性之间实现了最佳平衡。基于多组分波函数的方法,如用于基态的耦合簇单双激发(NEO - CCSD)方法和用于激发态的运动方程对应方法(NEO - EOM - CCSD),无需任何参数化即可达到类似的精度并且可以系统地改进,但计算成本更高。轨道优化微扰理论(NEO - OOMP2)方法的变体在计算基态时能达到接近NEO - CCSD的精度,且计算成本显著更低。计算激发电子态、振动态和振转电子态的其他方法包括δ自洽场(NEO - ΔSCF)、完全活性空间自洽场(NEO - CASSCF)和非正交组态相互作用方法。多参考方法对于描述氢隧穿过程尤为重要。其他类型的多组分系统,如包含电子和正电子的系统,也已在NEO框架内进行了研究。NEO方法允许以一种易于理解且计算高效的方式将特定原子核的核量子效应和非玻恩 - 奥本海默效应纳入量子化学计算。