2021
DOI: 10.1038/s41524-021-00590-w
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Spin–spin interactions in defects in solids from mixed all-electron and pseudopotential first-principles calculations

Abstract: Understanding the quantum dynamics of spin defects and their coherence properties requires an accurate modeling of spin-spin interaction in solids and molecules, for example by using spin Hamiltonians with parameters obtained from first principles calculations. We present a real-space approach based on density functional theory for the calculation of spin-Hamiltonian parameters, where only selected atoms are treated at the all-electron level, while the rest of the system is described with the pseudopotential a… Show more

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Cited by 18 publications
(11 citation statements)
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References 67 publications
(87 reference statements)
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“…1 MHz [41] (about 1 MHz is also the electron linewidth for the neutral divacancy in SiC [28]). For HF strengths > 2π • 6 kHz, the nuclei are within a distance of R < 15 Å from the vacancy site, while strengths on the order of 2π • 1 kHz correspond to a range of within R ∼ 25 Å [42].…”
Section: Synchronous Controlled Gates On Multiple Nuclei a Maximizati...mentioning
confidence: 99%
“…1 MHz [41] (about 1 MHz is also the electron linewidth for the neutral divacancy in SiC [28]). For HF strengths > 2π • 6 kHz, the nuclei are within a distance of R < 15 Å from the vacancy site, while strengths on the order of 2π • 1 kHz correspond to a range of within R ∼ 25 Å [42].…”
Section: Synchronous Controlled Gates On Multiple Nuclei a Maximizati...mentioning
confidence: 99%
“…In particular, FE basis provides systematic convergence for any materials system [22], can accommodate periodic, non-periodic and semi-periodic boundary conditions, and can offer excellent parallel scalability owing to the locality of the FE basis functions [28]. Furthermore, the FE basis sets are amenable to adaptive spatial resolution, not only allowing the possibility of large-scale all-electron calculations [26; 35] by combining with enrichment functions, but also mixed all-electron and pseudopotential calculations [36].…”
Section: Introductionmentioning
confidence: 99%
“…[48][49][50][51][52][53][54][55][56][57][58] ), recent developments 59,60 have demonstrated the utility of FE basis for conducting fast and accurate large-scale pseudopotential DFT calculations involving many tens of thousands of electrons [59][60][61][62] . However, for all-electron electronic structure calculations, although prior works 48,49,57,58,[63][64][65][66][67][68][69][70][71][72][73] have demonstrated the systematic convergence of the FE basis, the computational cost remains high, given the large number of FE basis functions that are needed to accurately describe the all-electron wavefunctions. The EFE basis, which enriches the FE basis with compactly supported enrichment functions-such as, for e.g., those constructed from single-atom wavefunctions-can be used to significantly reduce the number of FE basis functions, and consequently improve the computational efficiency of all-electron calculations.…”
Section: Introductionmentioning
confidence: 99%