Spin Transition in Strongly Correlated Bilayer Two Dimensional Electron Systems
arXiv:cond-mat/0410092 · doi:10.1103/PhysRevLett.94.076803
Abstract
Using a combination of heat pulse and nuclear magnetic resonance techniques we demonstrate that the phase boundary separating the interlayer phase coherent quantum Hall effect at in bilayer electron gases from the weakly coupled compressible phase depends upon the spin polarization of the nuclei in the host semiconductor crystal. Our results strongly suggest that, contrary to the usual assumption, the transition is attended by a change in the electronic spin polarization.
4 pages, 3 postscript figure
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- Quantum Hall to Insulator Transition in the Bilayer Quantum Hall Ferromagnet
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- Stability of the Excitonic Phase in Bilayer Quantum Hall Systems at Total Filling One -- Effects of Finite Well Width and Pseudopotentials --
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