메뉴 건너뛰기




Volumn 79, Issue 3, 2009, Pages

Spin Hall effect on the kagome lattice with Rashba spin-orbit interaction

Author keywords

[No Author keywords available]

Indexed keywords


EID: 60349120561     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.035323     Document Type: Article
Times cited : (45)

References (55)
  • 1
    • 0032573499 scopus 로고    scopus 로고
    • 10.1126/science.282.5394.1660;
    • G. A. Prinz, Science 282, 1660 (1998) 10.1126/science.282.5394.1660
    • (1998) Science , vol.282 , pp. 1660
    • Prinz, G.A.1
  • 3
    • 0003562493 scopus 로고    scopus 로고
    • edited by D. D. Awschalom, N. Sarmarth, and D. Loss (Springer-Verlag, Berlin
    • Semiconductor Spintronics and Quantum Computation, edited by, D. D. Awschalom,,, N. Sarmarth,, and, D. Loss, (Springer-Verlag, Berlin, 2002).
    • (2002) Semiconductor Spintronics and Quantum Computation
  • 8
    • 19544377969 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.70.081311
    • S.-Q. Shen, Phys. Rev. B 70, 081311 (R) (2004). 10.1103/PhysRevB.70. 081311
    • (2004) Phys. Rev. B , vol.70 , pp. 081311
    • Shen, S.-Q.1
  • 11
    • 11244249594 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.70.161201
    • E. I. Rashba, Phys. Rev. B 70, 161201 (R) (2004). 10.1103/PhysRevB.70. 161201
    • (2004) Phys. Rev. B , vol.70 , pp. 161201
    • Rashba, E.I.1
  • 13
    • 16444381421 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.71.085308
    • J. Schliemann and D. Loss, Phys. Rev. B 71, 085308 (2005). 10.1103/PhysRevB.71.085308
    • (2005) Phys. Rev. B , vol.71 , pp. 085308
    • Schliemann, J.1    Loss, D.2
  • 14
    • 27744608898 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.94.226601
    • G. Y. Guo, Y. Yao, and Q. Niu, Phys. Rev. Lett. 94, 226601 (2005). 10.1103/PhysRevLett.94.226601
    • (2005) Phys. Rev. Lett. , vol.94 , pp. 226601
    • Guo, G.Y.1    Yao, Y.2    Niu, Q.3
  • 15
  • 17
    • 29644433329 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.72.245305
    • Q.-F. Sun and X. C. Xie, Phys. Rev. B 72, 245305 (2005). 10.1103/PhysRevB.72.245305
    • (2005) Phys. Rev. B , vol.72 , pp. 245305
    • Sun, Q.-F.1    Xie, X.C.2
  • 23
    • 28844477796 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.95.226801
    • C. L. Kane and E. J. Mele, Phys. Rev. Lett. 95, 226801 (2005). 10.1103/PhysRevLett.95.226801
    • (2005) Phys. Rev. Lett. , vol.95 , pp. 226801
    • Kane, C.L.1    Mele, E.J.2
  • 24
    • 28844477210 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.95.146802
    • C. L. Kane and E. J. Mele, Phys. Rev. Lett. 95, 146802 (2005). 10.1103/PhysRevLett.95.146802
    • (2005) Phys. Rev. Lett. , vol.95 , pp. 146802
    • Kane, C.L.1    Mele, E.J.2
  • 25
    • 27144509118 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.95.106601
    • M. Onoda and N. Nagaosa, Phys. Rev. Lett. 95, 106601 (2005). 10.1103/PhysRevLett.95.106601
    • (2005) Phys. Rev. Lett. , vol.95 , pp. 106601
    • Onoda, M.1    Nagaosa, N.2
  • 26
  • 29
    • 33947198126 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.75.121403
    • T. Fukui and Y. Hatsugai, Phys. Rev. B 75, 121403 (R) (2007). 10.1103/PhysRevB.75.121403
    • (2007) Phys. Rev. B , vol.75 , pp. 121403
    • Fukui, T.1    Hatsugai, Y.2
  • 30
    • 33750926079 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.74.195312
    • L. Fu and C. L. Kane, Phys. Rev. B 74, 195312 (2006). 10.1103/PhysRevB.74.195312
    • (2006) Phys. Rev. B , vol.74 , pp. 195312
    • Fu, L.1    Kane, C.L.2
  • 31
    • 33847795859 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.98.106803
    • L. Fu, C. L. Kane, and E. J. Mele, Phys. Rev. Lett. 98, 106803 (2007). 10.1103/PhysRevLett.98.106803
    • (2007) Phys. Rev. Lett. , vol.98 , pp. 106803
    • Fu, L.1    Kane, C.L.2    Mele, E.J.3
  • 32
    • 34347373900 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.76.045302
    • L. Fu and C. L. Kane, Phys. Rev. B 76, 045302 (2007). 10.1103/PhysRevB.76.045302
    • (2007) Phys. Rev. B , vol.76 , pp. 045302
    • Fu, L.1    Kane, C.L.2
  • 35
    • 33144489555 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.73.045322
    • C. Xu and J. E. Moore, Phys. Rev. B 73, 045322 (2006). 10.1103/PhysRevB.73.045322
    • (2006) Phys. Rev. B , vol.73 , pp. 045322
    • Xu, C.1    Moore, J.E.2
  • 37
    • 33947696243 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.75.121306
    • J. E. Moore and L. Balents, Phys. Rev. B 75, 121306 (R) (2007). 10.1103/PhysRevB.75.121306
    • (2007) Phys. Rev. B , vol.75 , pp. 121306
    • Moore, J.E.1    Balents, L.2
  • 45
    • 60349092104 scopus 로고    scopus 로고
    • arXiv:cond-mat/0406436 (unpublished).
    • P. Zhang and Q. Niu, arXiv:cond-mat/0406436 (unpublished).
    • Zhang, P.1    Niu, Q.2
  • 47
    • 0002857806 scopus 로고
    • 10.1088/0305-4470/24/2/005;
    • A. Mielke, J. Phys. A 24, L73 (1991) 10.1088/0305-4470/24/2/005
    • (1991) J. Phys. a , vol.24 , pp. 73
    • Mielke, A.1
  • 48
    • 0041046391 scopus 로고
    • 10.1088/0305-4470/24/14/018;
    • A. Mielke, J. Phys. A 24, 3311 (1991) 10.1088/0305-4470/24/14/018
    • (1991) J. Phys. a , vol.24 , pp. 3311
    • Mielke, A.1
  • 49
    • 0039267801 scopus 로고
    • 10.1088/0305-4470/25/16/011
    • A. Mielke, J. Phys. A 25, 4335 (1992). 10.1088/0305-4470/25/16/011
    • (1992) J. Phys. a , vol.25 , pp. 4335
    • Mielke, A.1
  • 50
    • 60349115602 scopus 로고    scopus 로고
    • To simply clarify this feature, let us consider a usual Anderson insulator, in which the eigenenergy states are localized and thus the spin displacement operator sz r is well defined. Since the conserved spin current Js is given as a time derivative of the spin displacement operator, then it is straightforward to see that the response coefficient σ xy s of Js to a weak electric field is zero although both of the two components σ xy s0 and σ xy sτ in σ xy s can be nonzero. This subsequently results in the conclusion that these two components have different signs.
    • To simply clarify this feature, let us consider a usual Anderson insulator, in which the eigenenergy states are localized and thus the spin displacement operator sz r is well defined. Since the conserved spin current Js is given as a time derivative of the spin displacement operator, then it is straightforward to see that the response coefficient σ xy s of Js to a weak electric field is zero although both of the two components σ xy s0 and σ xy sτ in σ xy s can be nonzero. This subsequently results in the conclusion that these two components have different signs.
  • 54
    • 19744366974 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.93.206602
    • F. D. M. Haldane, Phys. Rev. Lett. 93, 206602 (2004). 10.1103/PhysRevLett.93.206602
    • (2004) Phys. Rev. Lett. , vol.93 , pp. 206602
    • Haldane, F.D.M.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.