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The corresponding expression in Ref. is slightly different from Eq. 2 since the σ band is treated in different ways. When a few minor mistakes in Ref. are corrected, the two expressions result in similar numerical values.
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The corresponding expression in Ref. is slightly different from Eq. 2 since the σ band is treated in different ways. When a few minor mistakes in Ref. are corrected, the two expressions result in similar numerical values.
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70349132275
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Hc [PK / (E (0) - HK, (0))] Hc is spin independent and thus ignored [see Eq. 10].
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Hc [PK / (E (0) - HK, (0))] Hc is spin independent and thus ignored [see Eq. 10].
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24
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70349144961
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For the K′ point, E↑ K′, (2) = ψA K′ |H K′,(2)| ψA K′ ±νRe [ ψA K′ |H K′,(2)| ψB K′ e-iθ], E↑ K′, (2) =- E↑ K′, (2) with upper (lower) sign for the conduction-band bottom (valence-band top).
-
For the K′ point, E↑ K′, (2) = ψA K′ | H K′, (2) | ψA K′ ±νRe [ ψA K′ | H K′, (2) | ψB K′ e-iθ], E↑ K′, (2) =- E↑ K′, (2) with upper (lower) sign for the conduction-band bottom (valence-band top).
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The last four terms of Hso in Eq. 9, which do not commute with σy, do not contribute to the effective SOC near the Fermi energy due to the factor e±iφ8.
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The last four terms of Hso in Eq. 9, which do not commute with σy, do not contribute to the effective SOC near the Fermi energy due to the factor e±iφ8.
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