Phase Transitions of Dirac Electrons in Bismuth
The Dirac Hamiltonian, which successfully describes relativistic fermions, applies equally well to electrons in solids with linear energy dispersion, for example, in bismuth and graphene. A characteristic of these materials is that a magnetic field less than 10 tesla suffices to force the Dirac electrons into the lowest Landau level, with resultant strong enhancement of the Coulomb interaction energy. Moreover, the Dirac electrons usually come with multiple flavors or valley degeneracy. These ingredients favor transitions to a collective state with novel quantum properties in large field. By using torque magnetometry, we have investigated the magnetization of bismuth to fields of 31 tesla. We report the observation of sharp field-induced phase transitions into a state with striking magnetic anisotropy, consistent with the breaking of the threefold valley degeneracy.
L. Li et al., "Phase Transitions of Dirac Electrons in Bismuth," Science, vol. 321, no. 5888, pp. 547-550, American Association for the Advancement of Science (AAAS), Jul 2008.
The definitive version is available at https://doi.org/10.1126/science.1158908
Keywords and Phrases
Bismuth; Oxygen; Electron; Magnetic Anisotropy; Magnetic Field; Anisotropy; Electron Beam; Mathematical Model; Phase Transition; Quantum Chemistry
International Standard Serial Number (ISSN)
Article - Journal
© 2008 American Association for the Advancement of Science (AAAS), All rights reserved.
01 Jul 2008