Magnetotransport Study of the Canted Antiferromagnetic Phase in Bilayer Quantum Hall State
arXiv:cond-mat/0601654 · doi:10.1103/PhysRevB.73.165304
Abstract
Magnetotransport properties are investigated in the bilayer quantum Hall state at the total filling factor . We measured the activation energy elaborately as a function of the total electron density and the density difference between the two layers. Our experimental data demonstrate clearly the emergence of the canted antiferromagnetic (CAF) phase between the ferromagnetic phase and the spin-singlet phase. The stability of the CAF phase is discussed by the comparison between experimental results and theoretical calculations using a Hartree-Fock approximation and an exact diagonalization study. The data reveal also an intrinsic structure of the CAF phase divided into two regions according to the dominancy between the intralayer and interlayer correlations.
6 pages, 7 figures
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Cited by in corpus (13)
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- Hilbert space and ground state structure of bilayer quantum Hall systems at
- The Study of Goldstone Modes in =2 Bilayer Quantum Hall Systems
- Hilbert space structure of the low energy sector of U(N) quantum Hall ferromagnets and their classical limit
- Husimi function and phase-space analysis of bilayer quantum Hall systems at
- Spin Supercurrent in the Canted Antiferromagnetic Phase
- Double Nuclear Spin Relaxation in Hybrid Quantum Hall Systems
- Dicke Model for Quantum Hall Systems
- Nambu-Goldstone modes and the Josephson supercurrent in the bilayer quantum Hall system
- Microwave Imaging of Edge Conductivity in Graphene at Charge Neutrality and Quantum Hall States