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024 7 _ |a 10.1103/PhysRevB.83.121101
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041 _ _ |a eng
082 _ _ |a 530
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|a Physics, Condensed Matter
100 1 _ |0 P:(DE-Juel1)VDB63896
|a Sasioglu, E.
|b 0
|u FZJ
245 _ _ |a Effective Coulomb interaction in transition metals from constrained random-phase approximation
260 _ _ |a College Park, Md.
|b APS
|c 2011
300 _ _ |a 121101
336 7 _ |a Journal Article
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440 _ 0 |0 4919
|a Physical Review B
|v 83
|x 1098-0121
|y 12
500 _ _ |3 POF3_Assignment on 2016-02-29
500 _ _ |a Fruitful discussions with F. Freimuth, A. Schindlmayr, T. Miyake, F. Aryasetiawan, and R. Sakuma are gratefully acknowledged. This work has been supported in part by the DFG through the Research Unit FOR-1346.
520 _ _ |a The effective on-site Coulomb interaction (Hubbard U) between localized d electrons in 3d, 4d, and 5d transition metals is calculated employing a parameter-free realization of the constrained random-phase approximation using Wannier functions within the full-potential linearized augmented-plane-wave method. The U values lie between 1.5 and 5.7 eV and depend on the crystal structure, spin polarization, d electron number, and d orbital filling. On the basis of the calculated U parameters, we discuss the strength of the electronic correlations and the instability of the paramagnetic state toward the ferromagnetic one for 3d metals.
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700 1 _ |0 P:(DE-Juel1)130548
|a Blügel, S.
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773 1 8 |a 10.1103/physrevb.83.121101
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773 _ _ |a 10.1103/PhysRevB.83.121101
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