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Reduced density matrix functional theory (RDMFT) and coupled cluster theory restricted to paired double excitations (pCCD) are emerging as efficient methodologies for accounting for the so-called non-dynamic electronic correlation effects. Up to now, molecular calculations have been performed with real-valued orbitals. However, before extending the applicability of these methodologies to extended systems, where Bloch states are employed, the subtleties of working with complex-valued orbitals and the consequences of imposing time-reversal symmetry must be carefully addressed. In this work, we describe the theoretical and practical implications of adopting time-reversal symmetry in RDMFT and pCCD when allowing for complex-valued orbital coefficients. The theoretical considerations primarily affect the optimization algorithms, while the practical implications raise fundamental questions about the stability of solutions. Specifically, we find that complex solutions lower the energy when non-dynamic electronic correlation effects are pronounced. We present numerical examples to illustrate and discuss these instabilities and possible problems introduced by N-representability violations.
The Bethe-Salpeter equation has been extensively employed to compute the two-body electron-hole propagator and its poles which correspond to the neutral excitation energies of the system. Through a different time-ordering, the two-body Green's function can also describe the propagation of two electrons or two holes. The corresponding poles are the double ionization potentials and double electron affinities of the system. In this work, a Bethe-Salpeter equation for the two-body particle-particle propagator is derived within the linear-response formalism using a pairing field and anomalous propagators. This framework allows us to compute kernels corresponding to different self-energy approximations ($GW$, $T$-matrix, and second-Born) as in the usual electron-hole case. The performance of these various kernels is gauged for singlet and triplet valence double ionization potentials using a set of 23 small molecules. The description of double core hole states is also analyzed.
In a recent letter [Phys. Rev. Lett. 131, 216401] we presented the multichannel Dyson equation (MCDE) in which two or more many-body Green's functions are coupled. In this work we will give further details of the MCDE approach. In particular we will discuss: 1) the derivation of the MCDE and the definition of the space in which it is to be solved; 2) the rationale of the approximation to the multichannel self-energy; 3) a diagrammatic analysis of the MCDE; 4) the recasting of the MCDE on an eigenvalue problem with an effective Hamiltonian that can be solved using standard numerical techniques. This work mainly focuses on the coupling between the one-body Green's function and the three-body Green's function to describe photoemission spectra, but the MCDE method can be generalized to the coupling of other many-body Green's functions and to other spectroscopies.
Galvinoxyl, as one of the most extensively studied organic stable free radicals, exhibits a notable phase transition from a high-temperature (HT) phase with a ferromagnetic (FM) intermolecular interaction to a low-temperature (LT) phase with an antiferromagnetic (AFM) coupling at 85 K. Despite significant research efforts, the crystal structure of the AFM LT phase has remained elusive. This study successfully elucidates the crystal structure of the LT phase, which belongs to the P[1 with combining macron] space group. The crystal structure of the LT phase is found to consist of a distorted dimer, wherein the distortion arises from the formation of short intermolecular distances between anti-node carbons in the singly-occupied molecular orbital (SOMO). Starting from the structure of the LT phase, wave function calculations show that the AFM coupling 2J/kB varies significantly from −1069 K to −54 K due to a parallel shift of the molecular planes within the dimer.
Sujets
Dipole
Approximation GW
Azide Anion
Configuration interactions
Chemical concepts
Ab initio calculation
Time reversal violation
3115vn
Range separation
Molecular descriptors
Adiabatic connection
CIPSI
Atrazine
Mécanique quantique relativiste
Excited states
New physics
3470+e
Coupled cluster
Anharmonic oscillator
Configuration Interaction
Relativistic quantum mechanics
Quantum Chemistry
Green's function
Pesticide
Diatomic molecules
Chimie quantique
Electron electric dipole moment
Atomic and molecular structure and dynamics
3115vj
Ground states
Acrolein
Time-dependent density-functional theory
3115ag
A posteriori Localization
3315Fm
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QSAR
Ion
Diffusion Monte Carlo
Atomic and molecular collisions
Carbon Nanotubes
Argile
Atomic data
Biodegradation
Quantum Monte Carlo
Numerical calculations
Wave functions
Anderson mechanism
Atrazine-cations complexes
Quantum chemistry
Atomic processes
Petascale
Electron electric moment
Corrélation électronique
Argon
Polarizabilities
Atom
Rydberg states
Fonction de Green
Xenon
Dirac equation
Line formation
Electron correlation
Atoms
Parity violation
Abiotic degradation
Atomic charges
Auto-énergie
Large systems
Atomic charges chemical concepts maximum probability domain population
AROMATIC-MOLECULES
Relativistic corrections
Théorie des perturbations
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Spin-orbit interactions
X-ray spectroscopy
AB-INITIO CALCULATION
A priori Localization
BIOMOLECULAR HOMOCHIRALITY
Single-core optimization
Coupled cluster calculations
Valence bond
Hyperfine structure
Density functional theory
Analytic gradient
CP violation
États excités
Dispersion coefficients
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Aimantation
Parallel speedup
Path integral
Molecular properties
ALGORITHM
Relativistic quantum chemistry
BENZENE MOLECULE
AB-INITIO
Pesticides Metabolites Clustering Molecular modeling Environmental fate Partial least squares
Perturbation theory