Magnetic Field Induced Insulating Phases at Large
arXiv:cond-mat/0408152 · doi:10.1103/PhysRevLett.94.226802
Abstract
Exploring a backgated low density two-dimensional hole sample in the large regime we found a surprisingly rich phase diagram. At the highest densities, beside the , 2/3, and 2/5 fractional quantum Hall states, we observe both of the previously reported high field insulating and reentrant insulating phases. As the density is lowered, the reentrant insulating phase initially strengthens, then it unexpectedly starts weakening until it completely dissapears. At the lowest densities the terminal quantum Hall state moves from to . The intricate behavior of the insulating phases can be explained by a non-monotonic melting line in the - phase space.
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- Connecting the Reentrant Insulating Phase and the Zero Field Metal-Insulator Transition in a 2D Hole System
- Wigner Crystallization in a Quasi-3D Electronic System
- Competition between fractional quantum Hall liquid and Wigner solid at small fillings: Role of layer thickness and Landau level mixing
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- Developing fractional quantum Hall states at = and in the presence of significant Landau level mixing
- Interaction-driven quantum phase transitions between topological and crystalline orders of electrons
- Coexistence of two hole phases in high-quality -GaAs/AlGaAs in the vicinity of Landau level filling factors =1 and =(1/3)
- Resistivity peak values at transition between fractional quantum Hall states