2006
DOI: 10.1088/1742-6596/30/1/033
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A microscopic model of oxygen vacancies inCa-dopedYIG

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Cited by 2 publications
(2 citation statements)
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“…Taking YIG as an example [18,19], with t = 0.8 eV, and I = 0.61a, we get E SO = 3.0 eV and λ = 1.13 Å. This is indeed several orders of magnitude larger than λ c and opens the way to practical schemes of electric control of the phase of spin waves.…”
mentioning
confidence: 84%
“…Taking YIG as an example [18,19], with t = 0.8 eV, and I = 0.61a, we get E SO = 3.0 eV and λ = 1.13 Å. This is indeed several orders of magnitude larger than λ c and opens the way to practical schemes of electric control of the phase of spin waves.…”
mentioning
confidence: 84%
“…The large repulsion energy U (∼ 8 eV) between two electrons on the same metal ion allows for a maximum occupancy of two electrons per ion (the repulsion between the electrons in the oxygen ligand is negligible in comparison). The fact [18,19] that t ( 0.8 eV) is much smaller that U allows us to use perturbation theory. Keeping up to the fourth order of t yields the effective interaction between the spins on the magnetic ions (see Appendix A):…”
Section: Heisenberg Hamiltonian Modified By Spin-orbit Couplingmentioning
confidence: 99%