-
1
-
-
0003414482
-
-
R. E. Prange
-
For a review, see The Quantum Hall Effect, edited by R. E. Prange and S. M. Girvin (Springer-Verlag, Berlin, 1987).
-
(1987)
The Quantum Hall Effect
-
-
-
4
-
-
16444385604
-
-
AIP Vipin Srivastava, Anil K. Bhatnagar, and Donald G. Naugle
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See, e.g., A. M. M. Pruisken and H. P. Wei, in Ordering Disorder: Prospect and Retrospect in Condensed Matter Physics, edited by Vipin Srivastava, Anil K. Bhatnagar, and Donald G. Naugle, AIP Conf. Proc. No. 159 (AIP, New York, 1999), p. 159.
-
(1999)
AIP Conf. Proc.
, pp. 159
-
-
Pruisken, A.M.M.1
Wei, H.P.2
-
7
-
-
0000783195
-
-
H. P. Wei, D. C. Tsui, M. A. Palaanen, and A. M. M. Pruisken, Phys. Rev. Lett. 61, 1294 (1988).
-
(1988)
Phys. Rev. Lett.
, vol.61
, pp. 1294
-
-
Wei, H.P.1
Tsui, D.C.2
Palaanen, M.A.3
Pruisken, A.M.M.4
-
9
-
-
0007134630
-
-
R. B. Laughlin, M. L. Cohen, J. M. Kosterlitz, H. Levine, S. B. Libby, and A. M. M. Pruisken, Phys. Rev. B 32, 1311 (1985).
-
(1985)
Phys. Rev. B
, vol.32
, pp. 1311
-
-
Laughlin, R.B.1
Cohen, M.L.2
Kosterlitz, J.M.3
Levine, H.4
Libby, S.B.5
Pruisken, A.M.M.6
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11
-
-
0001079771
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-
A. M. Finkelstein, Pis’ma Zh. Eksp. Teor. Fiz. 37, 436 (1983) [JETP Lett. 37, 517 (1983)];
-
(1983)
JETP Lett.
, vol.37
, pp. 517
-
-
Finkelstein, A.M.1
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24
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-
4243578372
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-
Phys. Rev. B 49, 4593 (1994).
-
(1994)
Phys. Rev. B
, vol.49
, pp. 4593
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27
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85037910735
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This was one of the main results of Lopez and Fradkin (Ref. 14), who discarded the edge states.
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This was one of the main results of Lopez and Fradkin (Ref. 14), who discarded the edge states.
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29
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0001670291
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A. M. M. Pruisken, B. Škorić, and M. A. Baranov, subsequent paper, Phys. Rev. B. 60, 16 838 (1999).
-
(1999)
Phys. Rev. B.
, vol.60
, pp. 16 838
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Pruisken, A.M.M.1
Škorić, B.2
Baranov, M.A.3
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30
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0000773070
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M. A. Baranov, A. M. M. Pruisken, and B. Škorić, following paper, Phys. Rev. B 60, 16 821 (1999).
-
(1999)
Phys. Rev. B
, vol.60
, pp. 16 821
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Baranov, M.A.1
Pruisken, A.M.M.2
Škorić, B.3
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31
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85037909969
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A similar phenomenon is well known to occur in ordinary Fermi liquid theory, where large frequency sums or non-Fermi level quantities contribute to the effective Landau parameters.
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A similar phenomenon is well known to occur in ordinary Fermi liquid theory, where large frequency sums or non-Fermi level quantities contribute to the effective Landau parameters.
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32
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85037896259
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(unpublished). A simplified version of this theory is given in Appendix B
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M. A. Baranov and A. M. M. Pruisken (unpublished). A simplified version of this theory is given in Appendix B.
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Baranov, M.A.1
Pruisken, A.M.M.2
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33
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85037893018
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The invariance of (Formula presented) can be easily understood by first writing (Formula presented)and then splitting (Formula presented)The second term on the right-hand side has nonzero matrix elements only in the upper-left-hand and lower-right-hand corners, i.e., in a small neighborhood of the extreme diagonal components (Formula presented) and (Formula presented) as can be seen by expanding the exponential form of (Formula presented) in powers of the (Formula presented) matrices. Therefore, this term commutes with (Formula presented) and we have (Formula presented)
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The invariance of (Formula presented) can be easily understood by first writing (Formula presented)and then splitting (Formula presented)The second term on the right-hand side has nonzero matrix elements only in the upper-left-hand and lower-right-hand corners, i.e., in a small neighborhood of the extreme diagonal components (Formula presented) and (Formula presented) as can be seen by expanding the exponential form of (Formula presented) in powers of the (Formula presented) matrices. Therefore, this term commutes with (Formula presented) and we have (Formula presented)
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