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Volumn 80, Issue 7, 2009, Pages

Curvature-enhanced spin-orbit coupling in a carbon nanotube

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EID: 70349114250     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.075409     Document Type: Article
Times cited : (99)

References (35)
  • 2
  • 11
    • 0034370218 scopus 로고    scopus 로고
    • 10.1143/JPSJ.69.1757;
    • T. Ando, J. Phys. Soc. Jpn. 69, 1757 (2000) 10.1143/JPSJ.69.1757
    • (2000) J. Phys. Soc. Jpn. , vol.69 , pp. 1757
    • Ando, T.1
  • 16
    • 67649225738 scopus 로고    scopus 로고
    • 10.1126/science.1158877
    • A. K. Geim, Science 324, 1530 (2009). 10.1126/science.1158877
    • (2009) Science , vol.324 , pp. 1530
    • Geim, A.K.1
  • 19
    • 70349099236 scopus 로고    scopus 로고
    • 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.
    • 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.
  • 23
    • 70349132275 scopus 로고    scopus 로고
    • Hc [PK / (E (0) - HK, (0))] Hc is spin independent and thus ignored [see Eq. 10].
    • Hc [PK / (E (0) - HK, (0))] Hc is spin independent and thus ignored [see Eq. 10].
  • 24
    • 70349144961 scopus 로고    scopus 로고
    • 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).
  • 25
    • 2442522754 scopus 로고
    • 10.1103/PhysRev.94.1498
    • J. C. Slater and G. F. Koster, Phys. Rev. 94, 1498 (1954). 10.1103/PhysRev.94.1498
    • (1954) Phys. Rev. , vol.94 , pp. 1498
    • Slater, J.C.1    Koster, G.F.2
  • 26
    • 70349158081 scopus 로고    scopus 로고
    • 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.
    • 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.
  • 27
    • 0029224192 scopus 로고
    • 10.1016/0008-6223(95)00018-9
    • J. W. Mintmire and C. T. White, Carbon 33, 893 (1995). 10.1016/0008-6223(95)00018-9
    • (1995) Carbon , vol.33 , pp. 893
    • Mintmire, J.W.1    White, C.T.2
  • 28
    • 11344253978 scopus 로고
    • Using other sets of tight-binding parameters 10.1103/PhysRevLett.67.2331;
    • Using other sets of tight-binding parameters [D. Tománek and M. A. Schluter, Phys. Rev. Lett. 67, 2331 (1991)] 10.1103/PhysRevLett.67.2331
    • (1991) Phys. Rev. Lett. , vol.67 , pp. 2331
    • Tománek, D.1    Schluter, M.A.2
  • 30
    • 6244247458 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.78.1932;
    • C. L. Kane and E. J. Mele, Phys. Rev. Lett. 78, 1932 (1997) 10.1103/PhysRevLett.78.1932
    • (1997) Phys. Rev. Lett. , vol.78 , pp. 1932
    • Kane, C.L.1    Mele, E.J.2
  • 31
    • 0034229826 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.85.154;
    • L. Yang and J. Han, Phys. Rev. Lett. 85, 154 (2000) 10.1103/PhysRevLett. 85.154
    • (2000) Phys. Rev. Lett. , vol.85 , pp. 154
    • Yang, L.1    Han, J.2
  • 32
    • 0035099199 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.63.073408;
    • A. Kleiner and S. Eggert, Phys. Rev. B 63, 073408 (2001) 10.1103/PhysRevB.63.073408
    • (2001) Phys. Rev. B , vol.63 , pp. 073408
    • Kleiner, A.1    Eggert, S.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.