Explicitly correlated Gaussian functions with shifted-center and projection techniques in pre-Born-Oppenheimer calculations
arXiv:1807.11727 · doi:10.1063/1.5050462
Abstract
Numerical projection methods are elaborated for the calculation of eigenstates of the non-relativistic many-particle Coulomb Hamiltonian with selected rotational and parity quantum numbers employing shifted explicitly correlated Gaussian functions, which are, in general, not eigenfunctions of the total angular momentum and parity operators. The increased computational cost of numerically projecting the basis functions onto the irreducible representations of the three dimensional rotation-inversion group is the price to pay for the increased flexibility of the basis functions. This increased flexibility allowed us to achieve a substantial improvement for the variational upper bound to the Pauli-allowed ground-state energy of the Hpppee molecular ion treated as an explicit five-particle system. We compare our pre-Born-Oppenheimer result for this molecular ion with rovibrational results including non-adiabatic corrections.
arXiv comment29 pages, 3 figures, 4 tables
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- Relativistic two-electron atomic and molecular energies using coupling and double groups: role of the triplet contributions to singlet states
- Gaussians for Electronic and Rovibrational Quantum Dynamics
- Analytically projected rotationally symmetric explicitly correlated Gaussian Functions with one-axis-shifted centers
- Sub-percent accuracy for the intensity of a near infrared water line at 10670 cm: experiment and analysis
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