Physics – Condensed Matter – Strongly Correlated Electrons
Scientific paper
2006-07-07
Phys. Rev. B 74, 113307 (2006)
Physics
Condensed Matter
Strongly Correlated Electrons
5 pages, 1 figure
Scientific paper
10.1103/PhysRevB.74.113307
We first exploit the spin symmetry relation $f^{\rm xc}_{s\bar s} (\zeta)=f^{\rm xc}_{\bar s s}(-\zeta)$ for the exact exchange correlation kernel $f^{\rm xc}_{s\bar s}(\zeta)$ in an inhomogeneous many electron system with arbitrary spin polarization $\zeta$. The physical condition required to satisfy the specific symmetry relation $f^{\rm xc}_{s\bar s}(\zeta) = f^{\rm xc}_{\bar s s}(\zeta)$ is derived and examined for simple ferromagnetic-nonmagnetic structure by taking the electrochemical potential into account. The condition is then applied to several composite systems useful in spintronics applications such as the magnetic system with net spin polarization.
Yeo Ina
Yi Kyung--Soo
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