1994
DOI: 10.1016/0368-2048(94)02106-6
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Calculated 2D Fermi surfaces and electronic structure of (100) and (110) W

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Cited by 5 publications
(2 citation statements)
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“…As to the dispersion of the ¯ 2 surface state, a good overall agreement among theoretical calculations is established for W(001)-(1 × 1): the surface-state band is located at 0.5-0.8 eV below E F at ¯ , shows flat but slightly upward dispersion along ¯ , crosses the Fermi level at ∼0.6 M and disperses up to 2-2.5 eV above E F at M [48,[83][84][85][86][87][88][89]. The calculations for Mo(001) also show similar results [89,90].…”
Section: Electronic Structure and Mechanism Of The Phase Transition W...supporting
confidence: 55%
“…As to the dispersion of the ¯ 2 surface state, a good overall agreement among theoretical calculations is established for W(001)-(1 × 1): the surface-state band is located at 0.5-0.8 eV below E F at ¯ , shows flat but slightly upward dispersion along ¯ , crosses the Fermi level at ∼0.6 M and disperses up to 2-2.5 eV above E F at M [48,[83][84][85][86][87][88][89]. The calculations for Mo(001) also show similar results [89,90].…”
Section: Electronic Structure and Mechanism Of The Phase Transition W...supporting
confidence: 55%
“…Since we use a fixed geometry and the transport properties depend only on the Fermi energy, it is not necessary at all to use the GGA. The Kohn-Sham equations [13] were solved using the full-potential linearized augmented plane wave (FP-LAPW) method in slab geometry [14,15]. This method is extremely advantageous for computing the electronic structure of magnetic multilayers, because it was designed to take into account the slab geometry and the interaction between the outermost monolayers of the trilayer system and vacuum.…”
Section: Self-consistent Calculationsmentioning
confidence: 99%