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Published on: January 21, 2016
Randomness-induced XY ordering in a graphene quantum hall ferromagnet.
Dmitry A Abanin1, Patrick A Lee, Leonid S Levitov
1Department of Physics, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, Massachusetts 02139, USA.
Valley-polarized quantum Hall states in graphene are stabilized by a random magnetic field, leading to an XY ferromagnet state. This results in unique Berezinskii-Kosterlitz-Thouless transitions and topological defects with half-integer charge.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Quantum Mechanics
Background:
- Valley-polarized quantum Hall states in graphene exhibit complex ordering behaviors.
- The Heisenberg O(3) ferromagnet model describes these states, influenced by valley anisotropy.
- Electron coupling to strain-induced gauge fields is a key factor in anisotropy.
Purpose of the Study:
- To investigate the role of strain-induced gauge fields in stabilizing quantum Hall states in graphene.
- To elucidate the mechanism of valley anisotropy and its effect on magnetic ordering.
- To explore the implications for topological transitions and defect properties.
Main Methods:
- Theoretical modeling using an effective random magnetic field approach.
- Analysis based on the Heisenberg O(3) ferromagnet model.
- Discussion of Berezinskii-Kosterlitz-Thouless theory and topological defect characteristics.
Main Results:
- A random magnetic field, arising from electron-strain coupling, stabilizes the XY ferromagnet state.
- The XY ferromagnet state represents a coherent mixture of K and K' valley states.
- The model predicts Berezinskii-Kosterlitz-Thouless ordering transitions and half-integer charged topological defects.
Conclusions:
- Strain-induced gauge fields play a crucial role in the physics of valley-polarized quantum Hall states.
- The random magnetic field mechanism provides a new perspective on ordering and stability in these systems.
- The findings offer insights into exotic phenomena like topological defects with fractional charge.
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