Approaching the basis-set limit of the dRPA correlation energy with explicitly correlated and Projector Augmented-wave methods
The direct random-phase approximation (dRPA) is used to calculate and compare atomization energies for the HEAT set and 10 selected molecules of the G2-1 set using both plane waves and Gaussian-type orbitals. We describe detailed procedures to obtain highly accurate and well converged results for th...
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Abstract | The direct random-phase approximation (dRPA) is used to calculate and compare atomization energies for the HEAT set and 10 selected molecules of the G2-1 set using both plane waves and Gaussian-type orbitals. We describe detailed procedures to obtain highly accurate and well converged results for the projector augmented-wave (PAW) method as implemented in the Vienna Ab-initio Simulation Package (VASP) as well as the explicitly correlated dRPA-F12 method as implemented in the TURBOMOLE package. The two approaches agree within chemical accuracy (1 kcal/mol) for the atomization energies of all considered molecules, both for the exact exchange as well as for the dRPA. The root mean-square deviation is 0.41 kcal/mol for the exact exchange (evaluated using density functional theory orbitals) and 0.33 kcal/mol for exact exchange plus the random-phase approximation. |
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AbstractList | The direct random-phase approximation (dRPA) is used to calculate and compare
atomization energies for the HEAT set and 10 selected molecules of the G2-1 set
using both plane waves and Gaussian-type orbitals. We describe detailed
procedures to obtain highly accurate and well converged results for the
projector augmented-wave (PAW) method as implemented in the Vienna Ab-initio
Simulation Package (VASP) as well as the explicitly correlated dRPA-F12 method
as implemented in the TURBOMOLE package. The two approaches agree within
chemical accuracy (1 kcal/mol) for the atomization energies of all considered
molecules, both for the exact exchange as well as for the dRPA. The root
mean-square deviation is 0.41 kcal/mol for the exact exchange (evaluated using
density functional theory orbitals) and 0.33 kcal/mol for exact exchange plus
the random-phase approximation. The direct random-phase approximation (dRPA) is used to calculate and compare atomization energies for the HEAT set and 10 selected molecules of the G2-1 set using both plane waves and Gaussian-type orbitals. We describe detailed procedures to obtain highly accurate and well converged results for the projector augmented-wave (PAW) method as implemented in the Vienna Ab-initio Simulation Package (VASP) as well as the explicitly correlated dRPA-F12 method as implemented in the TURBOMOLE package. The two approaches agree within chemical accuracy (1 kcal/mol) for the atomization energies of all considered molecules, both for the exact exchange as well as for the dRPA. The root mean-square deviation is 0.41 kcal/mol for the exact exchange (evaluated using density functional theory orbitals) and 0.33 kcal/mol for exact exchange plus the random-phase approximation. |
Author | Klopper, Wim Harding, Michael E Sukurma, Zoran Kresse, Georg Schlipf, Martin Taheridehkordi, Amir Humer, Moritz |
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BackLink | https://doi.org/10.48550/arXiv.2208.14726$$DView paper in arXiv https://doi.org/10.1063/5.0124019$$DView published paper (Access to full text may be restricted) |
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Snippet | The direct random-phase approximation (dRPA) is used to calculate and compare atomization energies for the HEAT set and 10 selected molecules of the G2-1 set... The direct random-phase approximation (dRPA) is used to calculate and compare atomization energies for the HEAT set and 10 selected molecules of the G2-1 set... |
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SubjectTerms | Approximation Atomizing Correlation Density functional theory Exchanging Mathematical analysis Orbitals Physics - Chemical Physics Physics - Computational Physics Plane waves |
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Title | Approaching the basis-set limit of the dRPA correlation energy with explicitly correlated and Projector Augmented-wave methods |
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