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Journal articles on the topic 'Quantum Hall regime'

Author: Grafiati

Published: 6 September 2023

Last updated: 31 July 2025

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1

Asano, Kenichi, and Tsuneya Ando. "Photoluminescence in quantum Hall regime:." Physica B: Condensed Matter 249-251 (June 1998): 549–52. http://dx.doi.org/10.1016/s0921-4526(98)00183-5.

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2

BUHMANN, HARTMUT. "SPIN HALL EFFECTS IN HgTe QUANTUM WELL STRUCTURES." International Journal of Modern Physics B 23, no. 12n13 (2009): 2551–55. http://dx.doi.org/10.1142/s0217979209061974.

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Due to a strong spin orbit interaction HgTe quantum well structures exhibit an unusual subband structure ordering which leads to some remarkable transport properties depending on the actual carrier density. Especially for quantum wells with an inverted band structure ordering, a strong Rashba-type spin orbit splitting gives rise to a strong spin Hall effect in the metallic regime and in the bulk insulating regime spin polarized edge channel transport leads to the formation of the quantum spin Hall effect. Gated quantum well structures have been used to explore these, the metallic and insulatin

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3

He, Mengyun, Yu Huang, Huimin Sun, et al. "Quantum anomalous Hall interferometer." Journal of Applied Physics 133, no. 8 (2023): 084401. http://dx.doi.org/10.1063/5.0140086.

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Electronic interferometries in integer and fractional quantum Hall regimes have unfolded the coherence, correlation, and statistical properties of interfering constituents. This is addressed by investigating the roles played by the Aharonov–Bohm effect and Coulomb interactions on the oscillations of transmission/reflection. Here, we construct magnetic interferometers using Cr-doped (Bi,Sb)2Te3 films and demonstrate the electronic interferometry using chiral edge states in the quantum anomalous Hall regime. By controlling the extent of edge coupling and the amount of threading magnetic flux, di

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4

Suzuki, Kenji, and Yoshiyuki Ono. "Orbital Magnetization in Quantum Hall Regime." Journal of the Physical Society of Japan 66, no. 11 (1997): 3536–42. http://dx.doi.org/10.1143/jpsj.66.3536.

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5

Amet, F., C. T. Ke, I. V. Borzenets, et al. "Supercurrent in the quantum Hall regime." Science 352, no. 6288 (2016): 966–69. http://dx.doi.org/10.1126/science.aad6203.

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6

Kramer, Bernhard, Stefan Kettemann, and Tomi Ohtsuki. "Localization in the quantum Hall regime." Physica E: Low-dimensional Systems and Nanostructures 20, no. 1-2 (2003): 172–87. http://dx.doi.org/10.1016/j.physe.2003.09.034.

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7

Aoki, Hideo. "Localisation in the quantum hall regime." Surface Science 196, no. 1-3 (1988): 107–19. http://dx.doi.org/10.1016/0039-6028(88)90672-3.

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8

Pruisken, A. M. M. "Delocalization in the quantum Hall regime." Physics Reports 184, no. 2-4 (1989): 213–17. http://dx.doi.org/10.1016/0370-1573(89)90040-9.

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9

Shikin, V. B. "Inhomogeneous Hall-geometry sample in the quantum Hall regime." Journal of Experimental and Theoretical Physics Letters 73, no. 5 (2001): 246–49. http://dx.doi.org/10.1134/1.1371063.

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10

ISHIKAWA, K., T. AOYAMA, Y. ISHIZUKA, and N. MAEDA. "FIELD THEORY OF ANISOTROPIC QUANTUM HALL GAS: METROLOGY AND A NOVEL QUANTUM HALL REGIME." International Journal of Modern Physics B 17, no. 27 (2003): 4765–818. http://dx.doi.org/10.1142/s0217979203023112.

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The von Neumann lattice representation is a convenient representation for studying several intriguing physics of quantum Hall systems. In this formalism, electrons are mapped to lattice fermions. A topological invariant expression of the Hall conductance is derived and is used for the proof of the integer quantum Hall effect in the realistic situation. Anisotropic quantum Hall gas is investigated based on the Hartree–Fock approximation in the same formalism. Thermodynamic properties, transport properties, and unusual response under external modulations are found. Implications for the integer q

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11

Nicopoulos, V. Nikos, and S. A. Trugman. "Complex quantum dynamics in the integer quantum Hall regime." Physical Review B 45, no. 19 (1992): 11004–15. http://dx.doi.org/10.1103/physrevb.45.11004.

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12

Kinaret, Jari M. "A quantum dot in the fractional quantum Hall regime." Physica B: Condensed Matter 189, no. 1-4 (1993): 142–46. http://dx.doi.org/10.1016/0921-4526(93)90155-y.

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13

Aoki, Hideo. "Double quantum dots in the fractional quantum Hall regime." Physica E: Low-dimensional Systems and Nanostructures 1, no. 1-4 (1997): 198–203. http://dx.doi.org/10.1016/s1386-9477(97)00043-x.

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14

Kasner, Marcus. "Electronic correlation in the quantum Hall regime." Annalen der Physik 514, no. 3 (2002): 175–252. http://dx.doi.org/10.1002/andp.20025140301.

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15

MacDonald, A. H., E. H. Rezayi, and David Keller. "Photoluminescence in the fractional quantum Hall regime." Physical Review Letters 68, no. 12 (1992): 1939–42. http://dx.doi.org/10.1103/physrevlett.68.1939.

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16

Schüller, C., K. B. Broocks, P. Schröter, et al. "Charged Excitons in the Quantum Hall Regime." Acta Physica Polonica A 106, no. 3 (2004): 341–53. http://dx.doi.org/10.12693/aphyspola.106.341.

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17

MacDonald, A. H. "Spin Bottlenecks in the Quantum Hall Regime." Physical Review Letters 83, no. 16 (1999): 3262–65. http://dx.doi.org/10.1103/physrevlett.83.3262.

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18

Fromer, N. A., C. Schüller, D. S. Chemla, et al. "Electronic Dephasing in the Quantum Hall Regime." Physical Review Letters 83, no. 22 (1999): 4646–49. http://dx.doi.org/10.1103/physrevlett.83.4646.

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19

Okulov, V. I., E. A. Pamyatnykh, and A. T. Lonchakov. "Thermodynamic anomalous Hall effect: The quantum regime." Low Temperature Physics 40, no. 11 (2014): 1032–34. http://dx.doi.org/10.1063/1.4901991.

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20

Main, P. C., A. K. Geim, H. A. Carmona, et al. "Resistance fluctuations in the quantum Hall regime." Physical Review B 50, no. 7 (1994): 4450–55. http://dx.doi.org/10.1103/physrevb.50.4450.

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21

Jain, J. K. "Composite Fermions in the Quantum Hall Regime." Science 266, no. 5188 (1994): 1199–202. http://dx.doi.org/10.1126/science.266.5188.1199.

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22

Russell, P. A., F. F. Ouali, N. P. Hewett, and L. J. Challis. "Power dissipation in the quantum Hall regime." Surface Science 229, no. 1-3 (1990): 54–56. http://dx.doi.org/10.1016/0039-6028(90)90831-r.

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23

Zheng, H. Z., K. K. Choi, D. C. Tsui, and G. Weimann. "Size effect in the quantum Hall regime." Surface Science Letters 170, no. 1-2 (1986): A229. http://dx.doi.org/10.1016/0167-2584(86)90553-0.

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24

Nielsen, Hans. "Magnetoresistance oscillations in the quantum Hall regime." Physica B: Condensed Matter 175, no. 1-3 (1991): 231–34. http://dx.doi.org/10.1016/0921-4526(91)90718-t.

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25

Bhatt, R. N., and Wan Xin. "Mesoscopic effects in the quantum Hall regime." Pramana 58, no. 2 (2002): 271–83. http://dx.doi.org/10.1007/s12043-002-0013-1.

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26

Ma, M., and A. Yu Zyuzin. "Josephson Effect in the Quantum Hall Regime." Europhysics Letters (EPL) 21, no. 9 (1993): 941–45. http://dx.doi.org/10.1209/0295-5075/21/9/011.

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27

Zheng, H. Z., K. K. Choi, D. C. Tsui, and G. Weimann. "Size effect in the quantum Hall regime." Surface Science 170, no. 1-2 (1986): 209–13. http://dx.doi.org/10.1016/0039-6028(86)90963-5.

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28

Yusa, G., H. Shtrikman, and I. Bar-Joseph. "Photoluminescence in the fractional quantum Hall regime." Physica E: Low-dimensional Systems and Nanostructures 12, no. 1-4 (2002): 49–54. http://dx.doi.org/10.1016/s1386-9477(01)00259-4.

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29

Ando, Tsuneya. "Local Current Distribution in Quantum Hall Regime." Journal of the Physical Society of Japan 58, no. 10 (1989): 3711–17. http://dx.doi.org/10.1143/jpsj.58.3711.

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30

Nurmikko, Arto, and Aron Pinczuk. "Optical Probes in the Quantum Hall Regime." Physics Today 46, no. 6 (1993): 24–32. http://dx.doi.org/10.1063/1.881352.

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31

Grunwald, A., and J. Hajdu. "Thermoelectric effects in the quantum Hall regime." Solid State Communications 63, no. 4 (1987): 289–92. http://dx.doi.org/10.1016/0038-1098(87)90910-0.

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32

Łydżba, Patrycja, and Janusz Jacak. "Identifying Particle Correlations in Quantum Hall Regime." Annalen der Physik 530, no. 3 (2017): 1700221. http://dx.doi.org/10.1002/andp.201700221.

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33

Page, D. A., and E. Brown. "Nonadiabatic Effects in the Quantum Hall Regime." Annals of Physics 223, no. 1 (1993): 75–128. http://dx.doi.org/10.1006/aphy.1993.1027.

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34

Kasner, Marcus. "Electronic correlation in the quantum Hall regime." Annalen der Physik 11, no. 3 (2002): 175–252. http://dx.doi.org/10.1002/1521-3889(200203)11:3<175::aid-andp175>3.0.co;2-a.

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35

Huang, Yu, Yu Fu, Peng Zhang, Kang L. Wang, and Qing Lin He. "Inducing superconductivity in quantum anomalous Hall regime." Journal of Physics: Condensed Matter 36, no. 37 (2024): 37LT01. http://dx.doi.org/10.1088/1361-648x/ad550a.

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Abstract Interfacing the quantum anomalous Hall insulator with a conventional superconductor is known to be a promising manner for realizing a topological superconductor, which has been continuously pursued for years. Such a proximity route depends to a great extent on the control of the delicate interfacial coupling of the two constituents. However, a recent experiment reported the failure to reproduce such a topological superconductor, which is ascribed to the negligence of the electrical short by the superconductor in the theoretical proposal. Here, we reproduce this topological superconduc

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36

CHENAUD, B., C. CHAUBET, B. JOUAULT, et al. "ARE AHARONOV–BOHM EFFECT AND QUANTIZED HALL REGIME COMPATIBLE?" International Journal of Nanoscience 02, no. 06 (2003): 535–41. http://dx.doi.org/10.1142/s0219581x03001656.

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We present calculations of the quantum oscillations appearing in the transmission of a mesoscopic GaAs / GaAlAs ring isolated by quantum point contacts. We show that the device acts as an electronic Fabry–Perot spectrometer in the quantum Hall effect regime, and discuss the effect of the coherence length of edge states.

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37

GIESBERS, A. J. M., U. ZEITLER, J. C. MAAN, D. REUTER, and A. D. WIECK. "AHARONOV-BOHM EFFECT IN THE QUANTUM HALL REGIME." International Journal of Modern Physics B 21, no. 08n09 (2007): 1404–8. http://dx.doi.org/10.1142/s0217979207042902.

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We have fabricated quantum rings in a GaAs/GaAlAs heterostructure 2DEG by local anodic oxidation with an atomic force microscope. In low magnetic fields we observe Aharonov-Bohm oscillations with a period of 60 mT corresponding to an effective ring diameter of 300 nm. In the high field regime, between filling factors ν = 2/3 and ν = 3, we observe Aharonov-Bohm oscillations of quantum Hall edge channels with a surprisingly large period, Δ B = 163 mT , corresponding to an edge channel around the inner diameter of the ring.

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38

PELED, E., D. SHAHAR, Y. CHEN, E. DIEZ, D. L. SIVCO, and A. Y. CHO. "QUANTUM HALL TRANSITIONS IN MESOSCOPIC SAMPLES." International Journal of Modern Physics B 18, no. 27n29 (2004): 3575–80. http://dx.doi.org/10.1142/s0217979204027049.

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We present an experimental study of four-terminal resistance fluctuations of mesoscopic samples in the quantum Hall regime. We show that in the vicinity of integer quantum Hall transitions there exist two kinds of correlations between the longitudinal and Hall resistances of the samples, one on either side of the transition region.

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39

GRANGER, GHISLAIN, J. P. EISENSTEIN, and J. L. RENO. "EDGE HEAT TRANSPORT IN THE QUANTUM HALL REGIME." International Journal of Modern Physics B 23, no. 12n13 (2009): 2616–17. http://dx.doi.org/10.1142/s0217979209062074.

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We investigate the transport of heat in the integer quantized Hall regime. We make use of quantum point contacts (QPC's) positioned along the edge of a large quantum Hall droplet to both locally heat and locally detect temperature rises at the edge of the droplet. The detection scheme is thermoelectric, in essence identical to one introduced by Molenkamp, et al.1 in the early 1990's for heat transport experiments at zero magnetic field. At zero magnetic field we find that heat moves away from the heater QPC more or less isotropically. As expected from the Mott formula, we find a close connecti

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40

Maasilta, I. J., and V. J. Goldman. "Energetics of quantum antidot states in the quantum Hall regime." Physical Review B 57, no. 8 (1998): R4273—R4276. http://dx.doi.org/10.1103/physrevb.57.r4273.

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41

Huber, M., M. Grayson, M. Rother, et al. "Tunneling in the quantum Hall regime between orthogonal quantum wells." Physica E: Low-dimensional Systems and Nanostructures 12, no. 1-4 (2002): 125–28. http://dx.doi.org/10.1016/s1386-9477(01)00283-1.

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42

Pashitskii, E. A. "New quantum states in the fractional quantum Hall effect regime." Low Temperature Physics 31, no. 2 (2005): 171–78. http://dx.doi.org/10.1063/1.1867312.

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43

Kettemann, Stefan. "Persistent Hall voltage and current in the fractional quantum Hall regime." Physical Review B 55, no. 4 (1997): 2512–22. http://dx.doi.org/10.1103/physrevb.55.2512.

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44

GOLDMAN, V. J., J. K. JAIN, and M. SHAYEGAN. "TRANSITIONS BETWEEN FRACTIONAL QUANTUM HALL STATES." Modern Physics Letters B 05, no. 07 (1991): 479–90. http://dx.doi.org/10.1142/s0217984991000563.

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We have studied transitions between adjacent incompressible states by measuring the positions of the longitudinal resistance peaks in the fractional quantum Hall regime and comparing results with the theoretical predictions. We have found that the peak positions agree well with those predicted by theory in which quantum effects are crucial to the existence of extended states.

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45

Vankov, A. B. "The Migdal jump under the quantum Hall regime." Izvestiâ Akademii nauk SSSR. Seriâ fizičeskaâ 88, no. 2 (2024): 190–95. http://dx.doi.org/10.31857/s0367676524020048.

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In two-dimensional electron systems at large values of the Wigner-Seits parameter rs and in the quantum Hall effect mode, the distribution function of particles over Landau levels was calculated. It turned out that at small filling factors, the tail of the distribution function and the magnitude of the Migdal jump are qualitatively different from the case of a Fermi liquid in a zero magnetic field. Due to the presence of the cyclotron energy gap, the Fermi-liquid distortion of the distribution function is significantly suppressed.

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46

Polyakov, D. G., and B. I. Shklovskii. "Conductivity-peak broadening in the quantum Hall regime." Physical Review B 48, no. 15 (1993): 11167–75. http://dx.doi.org/10.1103/physrevb.48.11167.

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47

Knüppel, Patrick, Sylvain Ravets, Martin Kroner, Stefan Fält, Werner Wegscheider, and Atac Imamoglu. "Nonlinear optics in the fractional quantum Hall regime." Nature 572, no. 7767 (2019): 91–94. http://dx.doi.org/10.1038/s41586-019-1356-3.

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48

Hohls, F., U. Zeitler, and R. J. Haug. "High Frequency Conductivity in the Quantum Hall Regime." Physical Review Letters 86, no. 22 (2001): 5124–27. http://dx.doi.org/10.1103/physrevlett.86.5124.

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49

Pruisken, A. M. M., and M. A. Baranov. "Cracking Coulomb Interactions in the Quantum Hall Regime." Europhysics Letters (EPL) 31, no. 9 (1995): 543–48. http://dx.doi.org/10.1209/0295-5075/31/9/007.

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50

de C. Chamon, C., and X. G. Wen. "Resonant tunneling in the fractional quantum Hall regime." Physical Review Letters 70, no. 17 (1993): 2605–8. http://dx.doi.org/10.1103/physrevlett.70.2605.

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