Effects of In-plane Magnetic Fields on the Canted Antiferromagnetic Phase in the Bilayer ν = 2 Quantum Hall State

2007 ◽  
Author(s):  
Akira Fukuda ◽  
Shinsuke Kozumi ◽  
Daiju Terasawa ◽  
Norio Kumada ◽  
Yoshiro Hirayama ◽  
...  
2006 ◽  
Vol 34 (1-2) ◽  
pp. 81-84 ◽  
Author(s):  
D. Terasawa ◽  
A. Fukuda ◽  
S. Kozumi ◽  
A. Sawada ◽  
Z.F. Ezawa ◽  
...  

2007 ◽  
Vol 39 (2) ◽  
pp. 277
Author(s):  
Akira Fukuda ◽  
Shinsuke Kozumi ◽  
Daiju Terasawa ◽  
Yuichi Shimoda ◽  
Norio Kumada ◽  
...  

2006 ◽  
Vol 34 (1-2) ◽  
pp. 77-80
Author(s):  
Akira Fukuda ◽  
Shinsuke Kozumi ◽  
Daiju Terasawa ◽  
Yuichi Shimoda ◽  
Norio Kumada ◽  
...  

2004 ◽  
Vol 18 (27n29) ◽  
pp. 3693-3698 ◽  
Author(s):  
U. ZEITLER ◽  
J. DE JONGE ◽  
J. W. W. VAN TILBURG ◽  
J. C. MAAN ◽  
D. REUTER ◽  
...  

We use tilted magnetic fields to effectively decouple a strongly coupled bilayer two-dimensional electron system into two separate layers. For our specific sample (tunnelling gap ΔSAS=2.5 meV ) the inter-layer coupling is quenched by an in-plane field B≈14 T , leading to the successive disappearance of all odd-integer states visible in the quantum Hall effect. Such a transition from a bilayer into two single layers is also observed in a solely parallel magnetic field. Surprisingly, the ν=1 the quantum Hall state remains present even for in-plane fields exceeding 20 T. Only when decreasing the total Landau level filling slightly below ν=1 the system undergoes an abrupt transition from a ν=1 quantum Hall state into two (insulating) systems with a half filled Landau level.


Science ◽  
2014 ◽  
Vol 345 (6192) ◽  
pp. 58-61 ◽  
Author(s):  
Kayoung Lee ◽  
Babak Fallahazad ◽  
Jiamin Xue ◽  
David C. Dillen ◽  
Kyounghwan Kim ◽  
...  

Bilayer graphene has a distinctive electronic structure influenced by a complex interplay between various degrees of freedom. We probed its chemical potential using double bilayer graphene heterostructures, separated by a hexagonal boron nitride dielectric. The chemical potential has a nonlinear carrier density dependence and bears signatures of electron-electron interactions. The data allowed a direct measurement of the electric field–induced bandgap at zero magnetic field, the orbital Landau level (LL) energies, and the broken-symmetry quantum Hall state gaps at high magnetic fields. We observe spin-to-valley polarized transitions for all half-filled LLs, as well as emerging phases at filling factors ν = 0 and ν = ±2. Furthermore, the data reveal interaction-driven negative compressibility and electron-hole asymmetry in N = 0, 1 LLs.


2013 ◽  
Vol 456 ◽  
pp. 012030 ◽  
Author(s):  
M E Msall ◽  
W Dietsche ◽  
S Schmult ◽  
K von Klitzing

1998 ◽  
Vol 516 (3) ◽  
pp. 704-718 ◽  
Author(s):  
Eduardo Fradkin ◽  
Chetan Nayak ◽  
Alexei Tsvelik ◽  
Frank Wilczek

Sign in / Sign up

Export Citation Format

Share Document