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Volumn 67, Issue 20, 2003, Pages

Exact diagonalization study of domain structure in integer filling factor quantum Hall ferromagnets

Author keywords

[No Author keywords available]

Indexed keywords

ACCELERATION; ARTICLE; CALCULATION; ENERGY; EXCITATION; MAGNETIC FIELD; MAGNETISM; MICROSCOPY; QUANTUM CHEMISTRY; QUANTUM MECHANICS;

EID: 0037489275     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.67.201305     Document Type: Article
Times cited : (13)

References (16)
  • 7
    • 0035138420 scopus 로고    scopus 로고
    • Magnetotransport anisotropy at integer filling factors and tilted fields has also been reported in Si/SiGe heterostructure samples
    • Magnetotransport anisotropy at integer filling factors and tilted fields has also been reported in Si/SiGe heterostructure samples: U. Zeitler, H.W. Schumacher, A.G.M. Jansen, and R.J. Haug, Phys. Rev. Lett. 86, 866 (2001).
    • (2001) Phys. Rev. Lett. , vol.86 , pp. 866
    • Zeitler, U.1    Schumacher, H.W.2    Jansen, A.G.M.3    Haug, R.J.4
  • 8
    • 0036684158 scopus 로고    scopus 로고
    • Stripe states at integer filling factors are, however, a possibility
    • Stripe states at integer filling factors are, however, a possibility. See E. Demler, Daw-Wei Wang, S. Das Sarma, and B.I. Halperin, Solid State Commun. 123, 243 (2002);
    • (2002) Solid State Commun. , vol.123 , pp. 243
    • Demler, E.1    Wang, D.-W.2    Das Sarma, S.3    Halperin, B.I.4
  • 13
    • 0003414482 scopus 로고
    • 2nd ed., edited by R.E. Prange and S.M. Girvin (Springer, New York
    • F.D.M. Haldane, in The Quantum Hall Effect, 2nd ed., edited by R.E. Prange and S.M. Girvin (Springer, New York, 1990).
    • (1990) The Quantum Hall Effect
    • Haldane, F.D.M.1
  • 16
    • 85039022405 scopus 로고    scopus 로고
    • z (along total B) is conserved, the domain walls have no dynamics and are localized. Indeed, the wall energy is essentially unchanged for fewer reversed spins (for 5, 4, and 3). It is somewhat reduced for very few reversed spins (for 1 and 2). The degree of quasidegeneracy is also denigrated for very small reversed spins. These differences are, however, very likely to be of finite-size origin
    • z (along total B) is conserved, the domain walls have no dynamics and are localized. Indeed, the wall energy is essentially unchanged for fewer reversed spins (for 5, 4, and 3). It is somewhat reduced for very few reversed spins (for 1 and 2). The degree of quasidegeneracy is also denigrated for very small reversed spins. These differences are, however, very likely to be of finite-size origin.


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