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3
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0003414482
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Springer, NY
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For reviews see: The Quantum Hall Effect, 2nd Ed. Edited by R. E. Prange and S. M. Girvin (Springer, NY, 1990); Perspectives in Quantum Hall Effects, Edited by S. Das Sarma and A. Pinczuk (Wiley, NY, 1997); S. M. Girvin, The Quantum Hall Effect, Les Houches Lecture Notes (1998); V. J. Goldman, Physica B 280, 372 (2000).
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(1990)
The Quantum Hall Effect, 2nd Ed.
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Prange, R.E.1
Girvin, S.M.2
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4
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0003490204
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Wiley, NY
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For reviews see: The Quantum Hall Effect, 2nd Ed. Edited by R. E. Prange and S. M. Girvin (Springer, NY, 1990); Perspectives in Quantum Hall Effects, Edited by S. Das Sarma and A. Pinczuk (Wiley, NY, 1997); S. M. Girvin, The Quantum Hall Effect, Les Houches Lecture Notes (1998); V. J. Goldman, Physica B 280, 372 (2000).
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(1997)
Perspectives in Quantum Hall Effects
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Das Sarma, S.1
Pinczuk, A.2
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5
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0003414482
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Les Houches Lecture Notes
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For reviews see: The Quantum Hall Effect, 2nd Ed. Edited by R. E. Prange and S. M. Girvin (Springer, NY, 1990); Perspectives in Quantum Hall Effects, Edited by S. Das Sarma and A. Pinczuk (Wiley, NY, 1997); S. M. Girvin, The Quantum Hall Effect, Les Houches Lecture Notes (1998); V. J. Goldman, Physica B 280, 372 (2000).
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(1998)
The Quantum Hall Effect
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Girvin, S.M.1
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6
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0033885835
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For reviews see: The Quantum Hall Effect, 2nd Ed. Edited by R. E. Prange and S. M. Girvin (Springer, NY, 1990); Perspectives in Quantum Hall Effects, Edited by S. Das Sarma and A. Pinczuk (Wiley, NY, 1997); S. M. Girvin, The Quantum Hall Effect, Les Houches Lecture Notes (1998); V. J. Goldman, Physica B 280, 372 (2000).
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(2000)
Physica B
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Goldman, V.J.1
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7
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0007324787
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http://www.nobel.se/prize/index.html
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15
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0030193668
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V. J. Goldman, Surf. Sci. 361/362, 1 (1996); Physica E 1, 15 (1997).
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(1996)
Surf. Sci.
, vol.361-362
, pp. 1
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Goldman, V.J.1
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16
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0030193668
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V. J. Goldman, Surf. Sci. 361/362, 1 (1996); Physica E 1, 15 (1997).
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(1997)
Physica E
, vol.1
, pp. 15
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18
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0001080950
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The excitation spectrum of QH edge channels is gapless, thus excitations of arbitrary charge can be created; e.g., X.-G. Wen, Intl. J. Mod. Phys. B 6, 1711 (1992). These edge excitations are a sort of ID charge density fluctuations in the direction perpendicular to the edge and generally are not Laughlin quasiparticles. A weakly coupled QAD serves as a "charge filter" that selects bulk Laughlin quasiparticles for interedge resonant tunneling.
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(1992)
Intl. J. Mod. Phys. B
, vol.6
, pp. 1711
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20
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0007258869
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note
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2 /(dσcursive Greek chicursive Greek chi), where L is the size of 2DES, because of finite diagonal conductivity σcursive Greek chicursive Greek chi at a finite temperature.
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22
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0005066202
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A small front gate that defines the antidot (as in J. Franklin et al., Surf. Sci. 361/362, 17 (1996)) clearly does not produce a uniform E⊥.
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(1996)
Surf. Sci.
, vol.361-362
, pp. 17
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Franklin, J.1
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26
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0007255073
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to be published
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I. Karakurt et al., to be published.
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Karakurt, I.1
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29
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0007324788
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note
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T peaks; we exclude such data from the charge analysis.
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31
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0034138847
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These our results are in stark disagreement with recent reports of shot noise power experiments in constrictions without antidots, which, interpreted as a measurement of fractional charge, show variations of q by factors of up to three and even six depending on all: v, It, and T. See, e.g., D. Glattli et al., Physica E 6, 22 (2000); T. Griffiths et al., cond-mat/00072664.
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(2000)
Physica E
, vol.6
, pp. 22
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Glattli, D.1
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32
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0007192228
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cond-mat/00072664
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These our results are in stark disagreement with recent reports of shot noise power experiments in constrictions without antidots, which, interpreted as a measurement of fractional charge, show variations of q by factors of up to three and even six depending on all: v, It, and T. See, e.g., D. Glattli et al., Physica E 6, 22 (2000); T. Griffiths et al., cond-mat/00072664.
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Glattli, D.1
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