Abstract:Electronic structure methods emerging from the combination of multiconfigurational wave functions and density functional theory (DFT) aim to take advantage of the strengths of the two nearly antagonistic theories. One of the common strategies employed to merge wave function theory (WFT) with DFT relies on the range separation of the Coulomb operator in which DFT functionals take care of the short-distance part, while long-range inter-electronic interactions are evaluated by using the chosen wave function metho… Show more
“…Recently, yet another non‐SCF method has been applied to nonsinglet excited states from RASCI wavefunctions 176 . The approach absorbs the SR exchange in the wavefunction part by representing the SR exchange functional with the Hartree–Fock expression.…”
Range-separated multiconfigurational density functional theory (RS MC-DFT) rigorously combines density functional (DFT) and wavefunction (WFT) theories. This is achieved by partitioning of the electron interaction operator into long-and short-range components and modeling them with WFT and DFT, respectively. In contrast to other methods, mixing wavefunctions with density functionals, RS MC-DFT is free from electron correlation double counting. The general formulation of RS MC-DFT allows for merging any ab initio approximation with density functionals. Implementations of RS MC-DFT aim at increasing both versatility and accuracy of the underlying methods, while reducing the computational cost of the ab initio problem. Variants of the RS MC-DFT approach can be divided into single-determinant-based range-separated methods and range-separated multideterminantal WFT methods. In these approaches the electron correlation energy is described both by a pertinent short-range density functional and by the wavefunction theory. We review the short-range functionals and correlated wavefunction theories employed in the framework of RS MC-DFT. We discuss applications of the RS MC-DFT methods to ground-state properties of molecules and to noncovalent interactions. Time-dependent linear-response theory and direct approaches to excited states are also presented. For each area of applications, we assess advantages of RS MC-DFT over conventional DFT and ab initio methods.
“…Recently, yet another non‐SCF method has been applied to nonsinglet excited states from RASCI wavefunctions 176 . The approach absorbs the SR exchange in the wavefunction part by representing the SR exchange functional with the Hartree–Fock expression.…”
Range-separated multiconfigurational density functional theory (RS MC-DFT) rigorously combines density functional (DFT) and wavefunction (WFT) theories. This is achieved by partitioning of the electron interaction operator into long-and short-range components and modeling them with WFT and DFT, respectively. In contrast to other methods, mixing wavefunctions with density functionals, RS MC-DFT is free from electron correlation double counting. The general formulation of RS MC-DFT allows for merging any ab initio approximation with density functionals. Implementations of RS MC-DFT aim at increasing both versatility and accuracy of the underlying methods, while reducing the computational cost of the ab initio problem. Variants of the RS MC-DFT approach can be divided into single-determinant-based range-separated methods and range-separated multideterminantal WFT methods. In these approaches the electron correlation energy is described both by a pertinent short-range density functional and by the wavefunction theory. We review the short-range functionals and correlated wavefunction theories employed in the framework of RS MC-DFT. We discuss applications of the RS MC-DFT methods to ground-state properties of molecules and to noncovalent interactions. Time-dependent linear-response theory and direct approaches to excited states are also presented. For each area of applications, we assess advantages of RS MC-DFT over conventional DFT and ab initio methods.
“…Very recently, the performance of the RAS‐ sr DFT method, and the WFT‐ sr DFT scheme in general, has been tested in the characterization of open‐shell atoms and molecules 46 . These investigations have revealed a noticeable unbalance in the treatment of open and closed‐shell systems by RAS‐ sr DFT.…”
Section: Recovering Dynamic Correlationmentioning
confidence: 99%
“…In the last decade, several developments have appeared in order to generalize the RAS‐SF method to other (non‐spin‐flip) excitation operators and optimize its computational implementation, 41–43 improve the accuracy of electronic energies, 44–46 characterize the nature of the wave function in complex systems, 47,48 and to the computation of molecular properties 49 . The present work reviews the theoretical foundations of the general RASCI methodology within the hole and particle truncation of the excitation operator.…”
In this review we outline the theory and recent progress of the restricted active space configuration interaction (RASCI) methodology within the hole and particle approximation. The RASCI is a single reference approach based on the splitting of the orbital space in different subsets, in which the target CI space is expressed by the concomitant number of electrons and empty orbitals in each subspace. Initially, the method was born as a spin complete version of the spin‐flip ansatz able to deal with any number of unpaired electrons. Since then, the method has experienced several improvements related to its theoretical foundations, its efficient implementation, in the characterization of RASCI wave functions, and in the calculation of molecular properties. It has shown to be especially suitable for the characterization of medium to large molecular diradicals and polyradicals, and to the study of photophysical processes involving open‐shell species and/or multiexcitonic states, like in the singlet fission reaction. But, despite this success, several limitations emerge from the sever truncation of the excitation operator, which might translate into inaccurate relative energies between different regions of the potential energy surface, and overestimated (or underestimated) excitation energies. These errors are associated with the lack of dynamic correlation, which has motivated the development and implementation of various improvements based on multi‐reference perturbation theory and to blend the RASCI wave function with density functional theory through range separation of electron–electron interactions. Finally, we discuss some of the properties available from RASCI wave functions and give potential future developments.
This article is categorized under:
Electronic Structure Theory > Ab Initio Electronic Structure Methods
Software > Quantum Chemistry
Quantum Computing > Theory Development
“…However, the neglected dynamic correlation from the huge number of weakly correlated orbitals, which are outside the active space, escapes a treatment on the same level of accuracy; typically only multi-reference perturbation theory to second order represents the highest level of accuracy achievable. [31] Continuous efforts have tried to improve on this situation; examples are tailored coupled cluster, [32][33][34] combinations with short-range DFT [35][36][37][38][39][40][41] or transcorrelation [42][43][44][45][46] to treat the electron-electron cusp due to the singularity of the Coulomb interaction, to mention only a few. Already the amount of suggestions for accurate multi-configurational methods (not reflected in the list of references of this work and beyond its scope) may be taken as an indication that no universally satisfactory and generally accepted best solution has been found so far.…”
Solving the electronic Schrödinger equation for changing nuclear coordinates provides access to the Born-Oppenheimer potential energy surface. This surface is the key starting point for almost all theoretical studies of chemical processes in electronic ground and excited states (including molecular structure prediction, reaction mechanism elucidation, molecular property calculations, quantum and molecular dynamics). Electronic structure models aim at a sufficiently accurate approximation of this surface. They have therefore become a cornerstone of theoretical and computational chemistry, molecular physics, and materials science. In this work, we elaborate on general features of approximate electronic structure models such as accuracy, efficiency, and general applicability in order to arrive at a perspective for future developments, of which a vanguard has already arrived. Our quintessential proposition is that meaningful quantum mechanical predictions for chemical phenomena require system-specific uncertainty information for each and every electronic structure calculation, if objective conclusions shall be drawn with confidence.
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