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W. Pan, T. Jungwirth, H.L. Stormer, D.C. Tsui, A.H. MacDonald, S.M. Girvin, L. Smrc̆ka, L.N. Pfeiffer, K.W. Baldwin, and K.W. West, Phys. Rev. Lett. 85, 3257 (2000).
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T. Jungwirth, A.H. MacDonald, L. Smrc̆ka, and S.M. Girvin, Phys. Rev. B 60, 15574 (1999).
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W. Pan, H.L. Stormer, D.C. Tsui, L.N. Pfeiffer, K.W. Baldwin, and K.W. West, Phys. Rev. B 64, 121305 (2001).
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7
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0035138420
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Magnetotransport anisotropy at integer filling factors and tilted fields has also been reported in Si/SiGe heterostructure samples
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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).
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Zeitler, U.1
Schumacher, H.W.2
Jansen, A.G.M.3
Haug, R.J.4
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8
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0036684158
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Stripe states at integer filling factors are, however, a possibility
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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);
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Solid State Commun.
, vol.123
, pp. 243
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Demler, E.1
Wang, D.-W.2
Das Sarma, S.3
Halperin, B.I.4
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9
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Daw-Wei Wang, S. Das Sarma, E. Demler, and B.I. Halperin, Phys. Rev. B 66, 195334 (2002).
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Phys. Rev. B
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Wang, D.-W.1
Das Sarma, S.2
Demler, E.3
Halperin, B.I.4
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12
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J.T. Chalker, D.G. Polyakov, F. Evers, A.D. Mirlin, and P. Wölfle, Phys. Rev. B 66, 161317 (2002).
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Chalker, J.T.1
Polyakov, D.G.2
Evers, F.3
Mirlin, A.D.4
Wölfle, P.5
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13
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0003414482
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2nd ed., edited by R.E. Prange and S.M. Girvin (Springer, New York
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F.D.M. Haldane, in The Quantum Hall Effect, 2nd ed., edited by R.E. Prange and S.M. Girvin (Springer, New York, 1990).
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The Quantum Hall Effect
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Haldane, F.D.M.1
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16
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85039022405
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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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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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