Одномерная электронная жидкость на краю двумерной электронной системы в режиме квантового эффекта Холла (1097785), страница 11
Текст из файла (страница 11)
Weis, K. v. Klitzing, K. Eberl, Hall Potential Distribution in the QuantumHall Regime in the Vicinity of a Potential Probe Contact // Physica E – 2002. vol.12, –pp.165-168.[12] Landauer R., Electrical resistance of disordered one-dimensional lattices // PhilosophicalMagazine. – 1970. vol. 21, pp. 863-867.[13] Haug R.J., Edge-state transport and its experimental consequences in high magnetic fields// Semicond. Sci. Technol. – 1993. vol.8, – pp.
131-153.[14] Xiao-Gang Wen, Gapless boundary excitations in the quantum Hall states and in the chiralspin states // Phys. Rev. B – 1991. vol.43, – pp. 11025-11036; Electrodynamical propertiesof gapless edge excitations in the fractional quantum Hall states // Phys. Rev. Lett. – 1990.vol.64 – pp. 2206-2209.[15] Fisher Matthew P.A., Glazman Leonid I., / chapter in "Mesoscopic ElectronTransport edited by L. Kowenhoven, G. Schoen and L.
Sohn, – NATO ASI Series E, KluwerAc. Publ., Dordrecht, 1996.; arXiv:cond-mat/9610037v1[16] Ando T. and Uemura Y., Theory of Oscillatory g Factor in an MOS Inversion Layerunder Strong Magnetic Fields // J. Phys. Soc. Jpn. – 1974. vol.37, – pp. 1044-1052;Бычков Ю.А., Иорданский С.В., Элиашберг Г.М. , Двумерные электроны в сильноммагнитном поле // Письма в ЖЭТФ – 1981. т.33, – C. 152-155; Kallin C. and HalperinB.
I., Excitations from a filled Landau level in the two-dimensional electron gas // Phys.Rev. B – 1984. vol.30, – pp. 5655-5668.[17] Usher A., Nicholas R. J., Harris J. J., and Foxon C. T., Observation of magnetic excitonsand spin waves in activation studies of a two-dimensional electron gas // Phys. Rev. B –1990. vol.41, – pp. 1129-1134.32[18] Dolgopolov V. T., Shashkin A. A., Aristov A. V., Schmerek D., Hansen W., Kotthaus J. P.,and Holland M., Direct Measurements of the Spin Gap in the Two-Dimensional ElectronGas of AlGaAs-GaAs Heterojunctions // Phys. Rev.
Lett. – 1997. vol. 79, – pp. 729-732.[19] Vankov A. B., Kulik L. V., Kukushkin I. V., Kirpichev V. E., Dickmann S., Zhilin V. M.,Smet J. H., von Klitzing K., and Wegscheider W., Low-Magnetic-Field Divergence of theElectronic g Factor Obtained from the Cyclotron Spin-Flip Mode of the ν = 1 QuantumHall Ferromagnet // Phys.
Rev. Lett. – 2006. vol.97, – pp. 246801.[20] Müller G., Weiss D., Khaetskii A. V., von Klitzing K., Koch S., Nickel H., Schlapp W.,and Lösch R., Equilibration length of electrons in spin-polarized edge channels // Phys.Rev. B – 1992. vol.45, – pp. 3932-3935.[21] Dixon David C., Wald Keith R., McEuen Paul L. and Melloch M. R., Dynamic nuclearpolarization at the edge of a two-dimensional electron gas // Phys. Rev.
B – 1997. vol.56,– pp. 4743-4750.[22] Machida T., Ishizuka S., Yamazaki T., Komiyama S., Muraki K. and Hirayama Y.,Spin polarization of fractional quantum Hall edge channels studied by dynamic nuclearpolarization, // Phys. Rev. B – 2002. vol.65, – pp. 233304.[23] Khrapai V. S., Deviatov E. V., Shashkin A. A., Dolgopolov V. T., Hastreiter F., WixforthA., Campman K. L., and Gossard A. C., Canted Antiferromagnetic Phase in a DoubleQuantum Well in a Tilted Quantizing Magnetic Field // Phys. Rev. Lett. – 2000. vol.84,– pp.
725-728.[24]Das Sarma S.,Sachdev S., andZheng L., Double-Layer Quantum HallAntiferromagnetism at Filling Fraction ν = 1 = 2/m where m is an Odd Integer //Phys. Rev. Lett. – 1997. vol.79, – pp. 917-920; Das Sarma S., Sachdev S., and Zheng L.,Canted antiferromagnetic and spin-singlet quantum Hall states in double-layer systems //Phys. Rev.
B – 1998. vol.58, – pp. 4672-4693.[25] Eisenstein J. P., Stormer H. L., Pfeiffer L. N., and West K. W., Evidence for a spintransition in the ν=2/3 fractional quantum Hall effect // Phys Rev. B – 1990. vol. 41– pp. 7910-7913; Engel L. W., Hwang S. W., Sajoto T., Tsui D. C., and Shayegan M.,Fractional quantum Hall effect at ν=2/3 and 3/5 in tilted magnetic fields // Phys Rev. B– 1992.
vol. 45, – pp. 3418-3425 (1992).[26] Smet J. H., Deutschmann R. A., Wegscheider W., Abstreiter G., and von Klitzing K. ,Ising Ferromagnetism and Domain Morphology in the Fractional Quantum Hall Regime// Phys. Rev. Lett., – 2001. vol. 86, – pp. 2412-2415.[27] Dempsey Jed, Gelfand B. Y., and Halperin B. I. Electron-electron interactions andspontaneous spin polarization in quantum Hall edge states // Phys. Rev. Lett.
– 1993.vol.70, – pp. 3639-3642.[28] Rijkels Lex and Bauer Gerrit E. W., Hysteresis and defects of spin-polarized edge statesin the integer quantum Hall regime // Phys. Rev. B – 1994. vol.50, – pp. 8629-8635.[29] Бычков Ю.А., Рашба Э.И. , Свойства двумерного электронного газа со снятым вырождением спектра // Письма в ЖЭТФ, – 1984. т. 39, – С. 66-69.33[30] Chamon C. d. C. and Wen X. G., Sharp and smooth boundaries of quantum Hall liquids//Phys. Rev.
B – 1984. vol. 49, – pp. 8227-8241.[31] Kane C.L. and Fisher M.P.A., Transmission through barriers and resonant tunneling inan interacting one-dimensional electron gas // Phys. Rev. B – 1992. vol. 46, – pp. 1523315262; Kane C.L. and Fisher M.P.A., Transport in a one-channel Luttinger liquid // Phys.Rev. Lett.
– 1992. vol. 68, – pp. 1220-1223.[32] Conti S. and Vignale G., Collective modes and electronic spectral function in smooth edgesof quantum hall systems // Phys. Rev. B – 1996. vol. 54, – pp. 14309-14312.[33] Zulicke U. and Shimshoni E., Conductance oscillations in strongly correlated fractionalquantum Hall line junctions // Phys. Rev. B – 2004. vol. 69, – pp. 085307; Zulicke U. andShimshoni E., Strongly Correlated Fractional Quantum Hall Line Junctions // Phys. Rev.Lett. – 2003. vol. 90, – pp. 026802.[34] Ponomarenko V. V.
and Averin D. V., Strong-coupling branching between edges offractional quantum Hall liquids // Phys. Rev. B – 2004. vol. 70, – pp. 195316.[35] Feldman D. E. and Feifei Li, Charge-statistics separation and probing non-Abelian states,// Phys. Rev.
B – 2008. vol 78, – pp. 161304.[36] Волков В.А. и Михайлов С.А., Краевые магнетоплазмоны: низкочастотные слабозатухающие возбуждения в неоднородных двумерных электронных системах // ЖЭТФ,– 1988. т. 94, – С. 217-241.[37] Kane C. L., Fisher M. P. A., and Polchinski J., Randomness at the edge: Theory of quantumHall transport at filling ν=2/3 // Phys. Rev. Lett.
– 1994. vol. 72, – pp. 4129-4132;Grosfeld E. , Das S., Probing the Neutral Edge Modes in Transport across a Point Contactvia Thermal Effects in the Read-Rezayi Non-Abelian Quantum Hall States // Phys. Rev.Lett. – 2009. vol. 102, – pp. 106403; Rosenow B. and Halperin B. I., Signatures of neutralquantum Hall modes in transport through low-density constrictions // Phys. Rev. B 2010. vol. 81, – pp. 165313.[38] Stern A., Anyons and the quantum Hall effect—A pedagogical review // Annals of Physics,– 2008.
vol. 323, – pp. 204-249.[39] van Wees B. J., Kouwenhoven L. P., Harmans C. J. P. M., Williamson J. G., TimmeringC. E., Broekaart M. E. I., Foxon C. T. and Harris J. J., Observation of zero-dimensionalstates in a one-dimensional electron interferometer // Phys. Rev. Lett. – 1989. vol. 62, –pp. 2523–2526.[40] Byers N. and Yang C.N., Theoretical Considerations Concerning Quantized Magnetic Fluxin Superconducting Cylinders // Phys.
Rev. Lett., – 1961. vol. 7, – pp. 46-49.34.
![](https://s.studizba.com/z.php?f=/templates/si/i/noavatar.png&w=100&h=100&t=1"){kind=avatar}
