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Volumn 82, Issue 7, 2010, Pages

Tunneling-driven breakdown of the 331 state and the emergent Pfaffian and composite Fermi liquid phases

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EID: 77957564021     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.82.075302     Document Type: Article
Times cited : (40)

References (47)
  • 1
    • 22244440948 scopus 로고
    • 10.1103/PhysRevLett.50.1395
    • R. B. Laughlin, Phys. Rev. Lett. 50, 1395 (1983). 10.1103/PhysRevLett.50. 1395
    • (1983) Phys. Rev. Lett. , vol.50 , pp. 1395
    • Laughlin, R.B.1
  • 3
    • 84926087383 scopus 로고    scopus 로고
    • Cambridge University Press, Cambridge, England, 10.1017/CBO9780511607561
    • J. Jain, Composite Fermions (Cambridge University Press, Cambridge, England, 2007). 10.1017/CBO9780511607561
    • (2007) Composite Fermions
    • Jain, J.1
  • 4
    • 4143100806 scopus 로고
    • 10.1103/PhysRevLett.72.900
    • E. H. Rezayi and N. Read, Phys. Rev. Lett. 72, 900 (1994). 10.1103/PhysRevLett.72.900
    • (1994) Phys. Rev. Lett. , vol.72 , pp. 900
    • Rezayi, E.H.1    Read, N.2
  • 9
    • 1842460762 scopus 로고
    • 10.1016/0550-3213(91)90407-O
    • G. Moore and N. Read, Nucl. Phys. B 360, 362 (1991). 10.1016/0550- 3213(91)90407-O
    • (1991) Nucl. Phys. B , vol.360 , pp. 362
    • Moore, G.1    Read, N.2
  • 10
    • 0000434548 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.54.16864
    • N. Read and E. Rezayi, Phys. Rev. B 54, 16864 (1996). 10.1103/PhysRevB.54.16864
    • (1996) Phys. Rev. B , vol.54 , pp. 16864
    • Read, N.1    Rezayi, E.2
  • 18
    • 77955385299 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.81.165304
    • Michael R. Peterson and S. Das Sarma, Phys. Rev. B 81, 165304 (2010). 10.1103/PhysRevB.81.165304
    • (2010) Phys. Rev. B , vol.81 , pp. 165304
    • Peterson, M.R.1    Das Sarma, S.2
  • 27
    • 0000049832 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.61.10267
    • N. Read and D. Green, Phys. Rev. B 61, 10267 (2000). 10.1103/PhysRevB.61. 10267
    • (2000) Phys. Rev. B , vol.61 , pp. 10267
    • Read, N.1    Green, D.2
  • 28
    • 0000224186 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.82.984
    • N. E. Bonesteel, Phys. Rev. Lett. 82, 984 (1999). 10.1103/PhysRevLett.82. 984
    • (1999) Phys. Rev. Lett. , vol.82 , pp. 984
    • Bonesteel, N.E.1
  • 29
    • 33744723980 scopus 로고
    • 10.1103/PhysRevLett.51.605;
    • F. D. M. Haldane, Phys. Rev. Lett. 51, 605 (1983) 10.1103/PhysRevLett.51. 605
    • (1983) Phys. Rev. Lett. , vol.51 , pp. 605
    • Haldane, F.D.M.1
  • 30
    • 0003414482 scopus 로고
    • see also 2nd ed., edited by R. E. Prange and S. M. Girvin (Springer-Verlag, New York
    • see also The Quantum Hall Effect, 2nd ed., edited by, R. E. Prange, and, S. M. Girvin, (Springer-Verlag, New York, 1990).
    • (1990) The Quantum Hall Effect
  • 31
    • 4243683825 scopus 로고
    • 10.1103/PhysRevLett.55.2095
    • F. D. Haldane, Phys. Rev. Lett. 55, 2095 (1985). 10.1103/PhysRevLett.55. 2095
    • (1985) Phys. Rev. Lett. , vol.55 , pp. 2095
    • Haldane, F.D.1
  • 34
    • 0000055697 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.58.15717
    • X.-G. Wen and A. Zee, Phys. Rev. B 58, 15717 (1998). 10.1103/PhysRevB.58. 15717
    • (1998) Phys. Rev. B , vol.58 , pp. 15717
    • Wen, X.-G.1    Zee, A.2
  • 35
    • 0001549186 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.53.13559
    • M. Milovanović and N. Read, Phys. Rev. B 53, 13559 (1996). 10.1103/PhysRevB.53.13559
    • (1996) Phys. Rev. B , vol.53 , pp. 13559
    • Milovanović, M.1    Read, N.2
  • 38
    • 0001343202 scopus 로고
    • 10.1103/PhysRevB.29.6833
    • D. Yoshioka, Phys. Rev. B 29, 6833 (1984). 10.1103/PhysRevB.29.6833
    • (1984) Phys. Rev. B , vol.29 , pp. 6833
    • Yoshioka, D.1
  • 43
    • 85083149129 scopus 로고    scopus 로고
    • This is equivalent to imposing the following constraint for the BCS Hamiltonian with only a tunneling term ΔSAS: the increase of the tunneling ΔSAS is followed by the decrease in the chemical potential μ by twice the same amount, δμ+δ ΔSAS /2=0, in our simplified model to maintain the chemical potential of the even channel, μe =μ+ ΔSAS /2, stay constant.
    • This is equivalent to imposing the following constraint for the BCS Hamiltonian with only a tunneling term Δ S A S: the increase of the tunneling Δ S A S is followed by the decrease in the chemical potential μ by twice the same amount, δ μ + δ Δ S A S / 2 = 0, in our simplified model to maintain the chemical potential of the even channel, μ e = μ + Δ S A S / 2, stay constant.
  • 46
    • 85083146295 scopus 로고    scopus 로고
    • arXiv:0912.0109 (unpublished).
    • Edward H. Rezayi and Steven H. Simon, arXiv:0912.0109 (unpublished).
    • Rezayi, E.H.1    Simon, S.H.2
  • 47
    • 70350629009 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.80.121302
    • W. Bishara and C. Nayak, Phys. Rev. B 80, 121302 (2009). 10.1103/PhysRevB.80.121302
    • (2009) Phys. Rev. B , vol.80 , pp. 121302
    • Bishara, W.1    Nayak, C.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.