Spin Polarization Curve of Fractional Quantum Hall States with Filling Factor Smaller than 2
Author(s) -
Shosuke Sasaki
Publication year - 2013
Publication title -
isrn condensed matter physics
Language(s) - English
Resource type - Journals
eISSN - 2090-7400
pISSN - 2090-7397
DOI - 10.1155/2013/489519
Subject(s) - physics , condensed matter physics , quantum hall effect , landau quantization , spin polarization , fractional quantum hall effect , hamiltonian (control theory) , coulomb , degenerate energy levels , electron , quantum mechanics , spins , quantum spin hall effect , mathematical optimization , mathematics
Kukushkin et al. have measured the electron spin polarization versus magnetic field in the fractional quantum Hall states. The polarization curves show wide plateaus and small shoulders. The 2D electron system is described by the total Hamiltonian (). Therein, is the sum of the Landau energies and classical Coulomb energies. is the residual interaction yielding Coulomb transitions. It is proven for any filling factor that the most uniform electron configuration in the Landau states is only one. The configuration has the minimum energy of . When the magnetic field is weak, some electrons have up-spins and the others down-spins. Then, there are many spin arrangements. These spin arrangements give the degenerate ground states of . We consider the partial Hamiltonian only between the ground states. The partial Hamiltonian yields the Peierls instability and is diagonalized exactly. The sum of the classical Coulomb and spin exchange energies has minimum for an interval modulation between Landau orbitals. Using the solution with the minimum energy, the spin polarization is calculated which reproduces the wide plateaus and small shoulders. The theoretical result is in good agreement with the experimental data.
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