scholarly journals Marginal metallic state at a fractional filling of ’8/5’ and ’4/3’ of Landau levels in the GaAs/AlGaAs 2D electron system

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
R. G. Mani ◽  
U. K. Wijewardena ◽  
T. R. Nanayakkara ◽  
Annika Kriisa ◽  
C. Reichl ◽  
...  

AbstractA metallic state with a vanishing activation gap, at a filling factor $$\nu = 8/5$$ ν = 8 / 5 in the untilted specimen with $$n= 2 \times 10^{11} cm^{-2}$$ n = 2 × 10 11 c m - 2 , and at $$\nu = 4/3$$ ν = 4 / 3 at $$n=1.2 \times 10^{11} cm^{-2}$$ n = 1.2 × 10 11 c m - 2 under a $$\theta = 66^{0}$$ θ = 66 0 tilted magnetic field, is examined through a microwave photo-excited transport study of the GaAs/AlGaAs 2 dimensional electron system (2DES). The results presented here suggest, remarkably, that at the possible degeneracy point of states with different spin polarization, where the 8/5 or 4/3 FQHE vanish, there occurs a peculiar marginal metallic state that differs qualitatively from a quantum Hall insulating state and the usual quantum Hall metallic state. Such a marginal metallic state occurs most prominently at $$\nu =8/5$$ ν = 8 / 5 , and at $$\nu =4/3$$ ν = 4 / 3 under tilt as mentioned above, over the interval $$1 \le \nu \le 2$$ 1 ≤ ν ≤ 2 , that also includes the $$\nu = 3/2$$ ν = 3 / 2 state, which appears perceptibly gapped in the first instance.

2014 ◽  
Vol 112 (18) ◽  
Author(s):  
A. A. Shashkin ◽  
V. T. Dolgopolov ◽  
J. W. Clark ◽  
V. R. Shaginyan ◽  
M. V. Zverev ◽  
...  

2004 ◽  
Vol 22 (1-3) ◽  
pp. 181-184 ◽  
Author(s):  
M. Grayson ◽  
D. Schuh ◽  
M. Bichler ◽  
M. Huber ◽  
G. Abstreiter ◽  
...  

SPIN ◽  
2015 ◽  
Vol 05 (03) ◽  
pp. 1530003
Author(s):  
R. Cangas ◽  
M. A. Hidalgo

In this paper, we review the contribution of the Rashba spin–orbit coupling to the magnetoconduction of a two-dimensional electron system (2DES) confined in an inversion layer under quantum Hall regime (low temperature and low defects and impurities). The study is based on a semi-classical model for the magnetoconductivities of the 2DES. This model reproduces the measurements of the Shubnikov-de Haas (SdH) oscillations obtained in systems confined in III–V heterostructures, and also the quantum Hall magnetoconductivity (magnetoresistivity). We also discuss the Rashba and Zeeman competition and its effect on the magnetoconductivity.


2002 ◽  
Vol 16 (20n22) ◽  
pp. 2924-2929 ◽  
Author(s):  
M. M. FOGLER

The stripe phase of a two-dimensional electron system in a weak magnetic field bears a close analogy to liquid crystals. However, reduced dimensionality and unusual dynamics give rise to important differences. At finite temperature they cause divergent fluctuations and nonperturbative renormalization of hydrodynamic parameters. Such effects can be verified in microwave experiments. At low temperatures the physics is dominated by quantum fluctuations. When they are large, the transition to a novel quantum nematic phase may occur, driven by quantum proliferation of dislocations. It will be signaled by an additional low-frequency resonance in the microwave response.


Sign in / Sign up

Export Citation Format

Share Document