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D.P. Young, D. Hall, M.E. Torelli, Z. Fisk, J.L. Sarrao, J.D. Thompson, H.-R. Ott, S.B. Oseroff, R.G. Goodrich, and R. Zysier, Nature (London) 397, 412 (1999).
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Young, D.P.1
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Torelli, M.E.3
Fisk, Z.4
Sarrao, J.L.5
Thompson, J.D.6
Ott, H.-R.7
Oseroff, S.B.8
Goodrich, R.G.9
Zysier, R.10
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Massidda, S.1
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De Pascale, T.M.3
Monnier, R.4
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Terakura, C.2
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Kimura, N.4
Aoki, H.5
Kunii, S.6
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Gavilano, J.L.1
Mushkolaj, S.2
Rau, D.3
Ott, H.R.4
Bianchi, A.5
Young, D.P.6
Fisk, Z.7
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84988767664
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cond-mat/0106550 (unpublished)
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R.R. Urbano, C. Rettori, G.E. Barberis, M. Torelli, A. Bianchi, Z. Fisk, P.G. Pagliuso, A. Malinowski, M.F. Hundley, J.L. Sarrao, and S.B. Oseroff, cond-mat/0106550 (unpublished).
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Urbano, R.R.1
Rettori, C.2
Barberis, G.E.3
Torelli, M.4
Bianchi, A.5
Fisk, Z.6
Pagliuso, P.G.7
Malinowski, A.8
Hundley, M.F.9
Sarrao, J.L.10
Oseroff, S.B.11
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84988792076
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cond-mat/0104184 (unpublished)
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D. Hall, D.P. Young, Z. Fisk, T.P. Murphy, E.C. Palm, A. Teklu, and R.G. Goodrich, cond-mat/0104184 (unpublished).
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Hall, D.1
Young, D.P.2
Fisk, Z.3
Murphy, T.P.4
Palm, E.C.5
Teklu, A.6
Goodrich, R.G.7
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16
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0000567574
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Goodrich, R.G.1
Harrison, N.2
Vuillemin, J.J.3
Teklu, A.4
Hall, D.W.5
Fisk, Z.6
Young, D.7
Sarrao, J.8
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0000108786
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84988784210
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cond-mat/0107429; Phys. Rev. Lett. (to be published)
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J.D. Denlinger, J.A. Clack, J.W. Allen, G.-H. Gweon, D.M. Poirier, C.G. Olson, J.L. Sarrao, A.D. Bianchi, and Z. Fisk, cond-mat/0107429; Phys. Rev. Lett. (to be published).
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Denlinger, J.D.1
Clack, J.A.2
Allen, J.W.3
Gweon, G.-H.4
Poirier, D.M.5
Olson, C.G.6
Sarrao, J.L.7
Bianchi, A.D.8
Fisk, Z.9
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21
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84988792100
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note
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We adopt the theoretical lattice parameters and atomic positions in Ref. 3.
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22
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84988779435
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note
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5, symmetry should be doubly degenerated. But their energies are slightly different from each other due to the numerical errors.
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23
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84988792104
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note
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The present linear muffin-tin-orbital atomic sphere approximation ASA has some arbitrariness in the choice of atomic sphere radii. Small band gap or small band overlap (Ref. 2-4) depends on a such choice. The important aspect here is how the GWA modifies the LDA band structure.
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24
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84988792109
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note
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z directions, respectively.
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25
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84988792110
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note
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VT-2 and VT-3 have higher quasiparticle energies than VT-1. VT, VT-2, and VT-3 shift in a similar fashion and have relatively higher quasiparticle energies than the other valence levels.
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27
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24444471611
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H.J. Tromp, P. van Gelderen, P.J. Kelly, G. Brocks, and P.A. Bobbert, Phys. Rev. Lett. 87, 016401 (2001).
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(2001)
Phys. Rev. Lett.
, vol.87
, pp. 016401
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Tromp, H.J.1
Van Gelderen, P.2
Kelly, P.J.3
Brocks, G.4
Bobbert, P.A.5
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29
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84988755383
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note
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This error is not a simple numerical one, but one inherent in the scheme. Part of the error stems from conduction contribution above the Fermi level beyond a few Rydberg. In addition, there is an error arising from the ASA.
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