Electron pairing in the quantum Hall regime due to neutralon exchange

被引:4
|
作者
Frigeri, Giovanni A. [1 ,2 ]
Rosenow, Bernd [2 ]
机构
[1] Max Planck Inst Math Sci, D-04103 Leipzig, Germany
[2] Univ Leipzig, Inst Theoret Phys, D-04103 Leipzig, Germany
来源
PHYSICAL REVIEW RESEARCH | 2020年 / 2卷 / 04期
关键词
SCATTERING-THEORY; SHOT-NOISE; INTERFEROMETER; STATISTICS; ANYONS;
D O I
10.1103/PhysRevResearch.2.043396
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The behavior of electrons in condensed matter systems is mostly determined by the repulsive Coulomb interaction. However, under special circumstances, the Coulomb interaction can be effectively attractive, giving rise to electron pairing in unconventional superconductors and specifically designed mesoscopic setups. In quantum Hall systems, electron interactions can play a particularly important role due to the huge degeneracy of Landau levels, leading, for instance, to the emergence of quasiparticles with fractional charge and anyonic statistics. Quantum Hall Fabry-Perot interferometers (FPI) have attracted increasing attention due to their ability to probe such exotic physics. In addition, such interferometers are affected by electron interactions themselves in interesting ways. Recently, experimental evidence for electron pairing in a quantum Hall FPI was found [Choi et al., Nat. Commun. 6, 7435 (2015)]. Theoretically describing an FPI in the limit of strong backscattering and under the influence of a screened Coulomb interaction, we compute electron shot noise and indeed find a two-fold enhanced Fano factor for some parameters, indicative of electron pairing. This result is explained in terms of an electron interaction due to exchange of neutral interedge plasmons, so-called neutralons.
引用
收藏
页数:17
相关论文
共 50 条
  • [31] LOCALIZATION IN THE QUANTUM HALL REGIME
    AOKI, H
    [J]. SURFACE SCIENCE, 1988, 196 (1-3) : 107 - 119
  • [32] Localization in the quantum Hall regime
    Kramer, B
    Kettemann, S
    Ohtsuki, T
    [J]. PHYSICA E-LOW-DIMENSIONAL SYSTEMS & NANOSTRUCTURES, 2003, 20 (1-2): : 172 - 187
  • [33] Correlation and exchange energies of a quantum Hall ferromagnet with ν= 13 in the strong interaction regime
    Institute of Solid State Physics, RAS, Chernogolovka
    142432, Russia
    不详
    101000, Russia
    [J]. Phys. Rev. B, 2024, 23
  • [34] BREAKDOWN OF THE QUANTUM HALL-EFFECT DUE TO ELECTRON HEATING
    KOMIYAMA, S
    TAKAMASU, T
    HIYAMIZU, S
    SASA, S
    [J]. SOLID STATE COMMUNICATIONS, 1985, 54 (06) : 479 - 484
  • [35] Exchange-mediated dynamic screening in the integer quantum Hall effect regime
    Oswald, Josef
    Romer, Rudolf A.
    [J]. EPL, 2017, 117 (05)
  • [36] ANOMALOUS RXX IN THE QUANTUM HALL REGIME DUE TO IMPURITY-BOUND STATES
    LEE, Y
    MCLENNAN, MJ
    DATTA, S
    [J]. PHYSICAL REVIEW B, 1991, 43 (17): : 14333 - 14336
  • [37] Imaging quantum-dot-confined electron density in transition to fractional quantum Hall regime
    Wach, E.
    Zebrowski, D. P.
    Szafran, B.
    [J]. SEMICONDUCTOR SCIENCE AND TECHNOLOGY, 2015, 30 (01)
  • [38] Edge strips in the quantum Hall regime imaged by a single-electron transistor
    Wei, YY
    Weis, J
    von Klitzing, K
    Eberl, K
    [J]. PHYSICAL REVIEW LETTERS, 1998, 81 (08) : 1674 - 1677
  • [39] Longitudinal impedance of a two-dimensional electron in the quantum Hall effect regime
    Hernandez, C.
    Chaubet, C.
    [J]. REVISTA MEXICANA DE FISICA, 2009, 55 (06) : 432 - 436
  • [40] SINGLE-ELECTRON TUNNELING IN THE FRACTIONAL QUANTUM HALL-EFFECT REGIME
    BEENAKKER, CWJ
    REJAEI, B
    [J]. PHYSICA B, 1993, 189 (1-4): : 147 - 156