The evaluation of non-topological components in Berry phase and momentum relaxation time in a gapped 3D topological insulator
- 1. Department of Electrical and Computer Engineering and Material Science Division, Boston University, Boston, MA 02215 (United States)
- 2. Department of Electrical and Computer Engineering, Purdue University, West Lafayette, IN 47907 (United States)
Description
The zero gap surface states of a 3D-topological insulator host Dirac fermions with spin locked to the momentum. The gap-less Dirac fermions exhibit electronic behaviour different from those predicted in conventional materials. While calculations based on a simple linear dispersion can account for observed experimental patterns, a more accurate description of the physics of these systems and a better agreement between experimental data theoretical results can be obtained by including higher order terms in the Hamiltonian. In this work, in presence of a time reversal symmetry breaking external magnetic field and higher order warping term, alteration to the topologically ordained Berry phase of , momentum relaxation time, and the magneto-conductivity tensors is established. The relation between scattering times and the deviations to topological Berry phase of is also emphasized. (paper)
Availability note (English)
Available from http://dx.doi.org/10.1088/0953-8984/27/33/335505Additional details
Identifiers
Publishing Information
- Journal Title
- Journal of Physics. Condensed Matter
- Journal Volume
- 27
- Journal Issue
- 33
- Journal Page Range
- [8 p.]
- ISSN
- 0953-8984
- CODEN
- JCOMEL
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 51042969
- Subject category
- S75: CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY;
- Descriptors DEI
- FERMIONS; HAMILTONIANS; MAGNETIC FIELDS; RELAXATION TIME; SPIN; SYMMETRY BREAKING; TOPOLOGY
- Descriptors DEC
- ANGULAR MOMENTUM; MATHEMATICAL OPERATORS; MATHEMATICS; PARTICLE PROPERTIES; QUANTUM OPERATORS