On the self-energy of 2D electron gas under random magnetic field

2011 ◽  
Vol 44 (2) ◽  
pp. 483-486
Author(s):  
B. Ünal ◽  
D. Ketenoğlu
2000 ◽  
Vol 85 (5) ◽  
pp. 1060-1063 ◽  
Author(s):  
D. Taras-Semchuk ◽  
K. B. Efetov

1995 ◽  
Vol 18 (1) ◽  
pp. 67-73 ◽  
Author(s):  
G.M. Gusev ◽  
U. Gennser ◽  
X. Kleber ◽  
D.K. Maude ◽  
J.C. Portal ◽  
...  

2007 ◽  
Vol 06 (03n04) ◽  
pp. 173-177
Author(s):  
YU. G. ARAPOV ◽  
S. V. GUDINA ◽  
G. I. HARUS ◽  
V. N. NEVEROV ◽  
N. G. SHELUSHININA ◽  
...  

The resistivity (ρ) of low mobility dilute 2D electron gas in an n- InGaAs / GaAs double quantum well (DQW) exhibits the monotonic "insulating-like" temperature dependence (dρ/dT < 0) at T = 1.8–70 K in zero magnetic field. This temperature interval corresponds to a ballistic regime (kBTτ/ħ > 0.1–3.5) for our samples, and the electron density is on an "insulating" side of the so-called B = 0 2D metal–insulator transition. We show that the observed features of localization and Landau quantization in a vicinity of the low magnetic-field-induced insulator–quantum Hall liquid transition is due to the σxy(T) anomalous T-dependence.


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