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Volumn 78, Issue 11, 2008, Pages

Conductance properties of rough quantum wires with colored surface disorder

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EID: 52949092786     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.78.115317     Document Type: Article
Times cited : (10)

References (26)
  • 1
    • 24244444170 scopus 로고
    • PHRVAO 0031-899X 10.1103/PhysRev.109.1492
    • P. W. Anderson, Phys. Rev. PHRVAO 0031-899X 10.1103/PhysRev.109.1492 109, 1492 (1958).
    • (1958) Phys. Rev. , vol.109 , pp. 1492
    • Anderson, P.W.1
  • 4
    • 6644226380 scopus 로고    scopus 로고
    • PRLTAO 0031-9007 10.1103/PhysRevLett.82.4062
    • F. M. Izrailev and A. A. Krokhin, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.82.4062 82, 4062 (1999).
    • (1999) Phys. Rev. Lett. , vol.82 , pp. 4062
    • Izrailev, F.M.1    Krokhin, A.A.2
  • 10
  • 11
    • 33748305547 scopus 로고    scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.74.104201
    • A. Rodriguez and J. M. Cervero, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.74.104201 74, 104201 (2006).
    • (2006) Phys. Rev. B , vol.74 , pp. 104201
    • Rodriguez, A.1    Cervero, J.M.2
  • 12
    • 35148900763 scopus 로고    scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.76.134202
    • V. M. K. Bagci and A. A. Krokhin, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.76.134202 76, 134202 (2007).
    • (2007) Phys. Rev. B , vol.76 , pp. 134202
    • Bagci, V.M.K.1    Krokhin, A.A.2
  • 14
    • 41549127013 scopus 로고    scopus 로고
    • PRLTAO 0031-9007 10.1103/PhysRevLett.100.126402
    • U. Kuhl, F. M. Izrailev, and A. A. Krokhin, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.100.126402 100, 126402 (2008).
    • (2008) Phys. Rev. Lett. , vol.100 , pp. 126402
    • Kuhl, U.1    Izrailev, F.M.2    Krokhin, A.A.3
  • 15
    • 33646018662 scopus 로고    scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.73.155421
    • F. M. Izrailev, N. M. Makarov, and M. Rendon, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.73.155421 73, 155421 (2006)
    • (2006) Phys. Rev. B , vol.73 , pp. 155421
    • Izrailev, F.M.1    Makarov, N.M.2    Rendon, M.3
  • 16
    • 33646337699 scopus 로고    scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.73.205404
    • U. Harbola, J. Maddox, and S. Mukamel, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.73.205404 73, 205404 (2006).
    • (2006) Phys. Rev. B , vol.73 , pp. 205404
    • Harbola, U.1    Maddox, J.2    Mukamel, S.3
  • 17
    • 33845660835 scopus 로고    scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.74.245317
    • G. B. Akguc and T. H. Seligman, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.74.245317 74, 245317 (2006).
    • (2006) Phys. Rev. B , vol.74 , pp. 245317
    • Akguc, G.B.1    Seligman, T.H.2
  • 18
    • 43049134789 scopus 로고    scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.77.205302
    • G. B. Akguc and J. B. Gong, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.77.205302 77, 205302 (2008).
    • (2008) Phys. Rev. B , vol.77 , pp. 205302
    • Akguc, G.B.1    Gong, J.B.2
  • 21
    • 52949107920 scopus 로고    scopus 로고
    • Note that to be more precise, one should compensate for the discretized correlation function defined in Eq. 2 by a factor of 1/ (N-m-1). However, this compensation has little effect here because N, i.e., the total number of grid points, is large enough and the correlation function itself decays fast (correlation radius much smaller than the waveguide length).
    • Note that to be more precise, one should compensate for the discretized correlation function defined in Eq. 2 by a factor of 1/ (N-m-1). However, this compensation has little effect here because N, i.e., the total number of grid points, is large enough and the correlation function itself decays fast (correlation radius much smaller than the waveguide length).
  • 22
    • 52949091875 scopus 로고    scopus 로고
    • After the convolution, we will rescale the new surface roughness function η̃(x) such as its maximal value is still given by |ηmax |.
    • After the convolution, we will rescale the new surface roughness function η̃(x) such as its maximal value is still given by | ηmax |.
  • 23
    • 0000061057 scopus 로고    scopus 로고
    • See, for example, PLEEE8 1063-651X 10.1103/PhysRevE.53.3271
    • See, for example, G. A. Luna-Acosta, Kyungsun Na, L. E. Reichl, and A. Krokhin, Phys. Rev. E PLEEE8 1063-651X 10.1103/PhysRevE.53.3271 53, 3271 (1996).
    • (1996) Phys. Rev. e , vol.53 , pp. 3271
    • Luna-Acosta, G.A.1    Na, K.2    Reichl, L.E.3    Krokhin, A.4
  • 24
    • 52949125569 scopus 로고    scopus 로고
    • Interestingly, for |ηmax| =0.01, if the location of the peak of χ η̃(2k) is too close to the channel opening energy, e.g., ∼kw/π=0.25, then it becomes harder to identify a conductance window similar to that shown in Fig. 4.
    • Interestingly, for |ηmax| =0.01, if the location of the peak of χ η̃(2k) is too close to the channel opening energy, e.g., ∼kw/π=0.25, then it becomes harder to identify a conductance window similar to that shown in Fig. 4.
  • 25
    • 35448989286 scopus 로고    scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.76.155313
    • P. G. Murphy and J. E. Moore, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.76.155313 76, 155313 (2007).
    • (2007) Phys. Rev. B , vol.76 , pp. 155313
    • Murphy, P.G.1    Moore, J.E.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.