Conductivity Tensor in a Holographic Quantum Hall Ferromagnet
arXiv:1408.3320 · doi:10.1016/j.physletb.2014.10.004
Abstract
The Hall and longitudinal conductivities of a recently studied holographic model of a quantum Hall ferromagnet are computed using the Karch-O'Bannon technique. In addition, the low temperature entropy of the model is determined. The holographic model has a phase transition as the Landau level filling fraction is increased from zero to one. We argue that this phase transition allows the longitudinal conductivity to have features qualitatively similar to those of two dimensional electron gases in the integer quantum Hall regime. The argument also applies to the low temperature limit of the entropy. The Hall conductivity is found to have an interesting structure. Even though it does not exhibit Hall plateaux, it has a flattened dependence on the filling fraction with a jump, analogous to the interpolation between Hall plateaux, at the phase transition.
7 pages, double column format, 4 figures
References in corpus (8)
- Landau Level Splitting in Graphene in High Magnetic Fields
- Metallic AdS/CFT
- The zero-energy state in graphene in a high magnetic field
- Dissipative Quantum Hall Effect in Graphene near the Dirac Point
- Divergent resistance at the Dirac point in graphene: Evidence for a transition in a high magnetic field
- The Stress-Energy Tensor of Flavor Fields from AdS/CFT
- Fluctuations and instabilities of a holographic metal
- A Holographic Quantum Hall Ferromagnet
Cited by in corpus (7)
- One-Point Functions of Non-protected Operators in the SO(5) symmetric D3-D7 dCFT
- Holographic sliding stripes
- A Quantum Check of Non-Supersymmetric AdS/dCFT
- A Quantum Framework for AdS/dCFT through Fuzzy Spherical Harmonics on
- Striped anyonic fluids
- The D3-probe-D7 brane holographic fractional topological insulator
- Fundamental Landau Levels in a Strongly Coupled Plasma