Unconventional Fractional Quantum Hall States in a Wide Quantum Well

被引:0
|
作者
Dorozhkin, S. I. [1 ]
Kapustin, A. A. [1 ]
Fedorov, I. B. [1 ]
Umansky, V. [2 ]
Smet, J. H. [3 ]
机构
[1] Russian Acad Sci, Osipyan Inst Solid State Phys, Chernogolovka 142432, Moscow, Russia
[2] Weizmann Inst Sci, Dept Phys, IL-76100 Rehovot, Israel
[3] Max Planck Inst Festkorperforsch, D-70569 Stuttgart, Germany
基金
俄罗斯科学基金会;
关键词
FUNCTIONAL-INTEGRAL APPROACH; CORRELATED FERMI SYSTEMS; PHASE-TRANSITIONS; GAUGE-THEORY; INSULATOR; LATTICE; CONDENSATION; CONFINEMENT; EXCITATIONS; PHYSICS;
D O I
10.1134/S0021364022602974
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
A bilayer electron system that is formed in a 60-nm-wide GaAs quantum well and has a large difference of the electron densities in the layers has been studied. It has been found that, when a magnetic field is tilted from the normal to the plane of the system, integer quantum Hall effect states at the filling factors of Landau levels of 1 and 2 disappear; instead, fractional quantum Hall effect states in the interval between these filling factors appear at the filling factors nu(F) = 4/3, 10/7, and 6/5 with odd denominators and at the filling factor nu(F) = 5/4. Several different states can be observed under the variation of the magnetic field. The detected fractional quantum Hall effect states are interpreted as combined states with the same filling factor 1 in the layer with the higher density and with the filling factors nu(F) - 1 in the layer with the lower density. These states are formed because of the redistribution of electrons between the layers, which occurs under the variation of the magnetic field. The appearance of the state with the filling factor nu(F) = 5/4 with the even denominator is presumably attributed to the dominance of the interlayer electron-electron interaction over the intralayer one for electrons in the layer with the lower density.
引用
收藏
页码:68 / 74
页数:7
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