Bismuth in strong magnetic fields: unconventional Zeeman coupling and correlation effects
arXiv:0810.3261 · doi:10.1103/PhysRevB.79.241101
Abstract
Recent experiments on bismuth have uncovered remarkably rich magnetization structure at fields well beyond the regime in which all carriers are expected to reside in the lowest Landau level. Motivated by these findings, we start from a microscopic tight-binding model and derive a low-energy Hamiltonian for the holes and three Dirac electrons pockets in bismuth. We find that an unconventional electron Zeeman effect, overlooked previously, suppresses the quantum limit for the electrons dramatically, giving rise to the observed anomalous magnetization structure. We further study interaction effects near fields at which the 2nd Landau level for one electron pocket empties, where magnetization hysteresis was observed. Here we find instabilities towards both charge density wave and Wigner crystal phases, and propose that hysteresis arises from a first-order transition out of the latter.
4 pages, 1 figure
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Cited by in corpus (24)
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- Phase diagram of bismuth in the extreme quantum limit
- Landau spectrum and twin boundaries of bismuth in the extreme quantum limit
- Signatures of surface states in bismuth at high magnetic fields
- Thermodynamic signatures of the field-induced states of graphite
- Theory of transport property of density wave phases in three-dimensional metals and semimetals under high magnetic field
- Hall plateaus at magic angles in bismuth beyond the quantum limit
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- Nernst quantum oscillations in bulk semi-metals
- Electron-phonon coupling in semimetals in a high magnetic field
- Competing phases and critical behavior in three coupled spinless Luttinger liquids
- Theory of phonon instabilities in Weyl semimetals at high magnetic fields
- High-field immiscibility of electrons belonging to adjacent twinned bismuth crystals