Suppression of backward scattering of Dirac fermions in iron pnictides Ba(FeRuAs)
arXiv:1208.2328 · doi:10.1103/PhysRevB.86.094510
Abstract
We report electronic transport of Dirac cones when Fe is replaced by Ru, which has an isoelectronic electron configuration to Fe, using single crystals of Ba(FeRuAs). The electronic transport of parabolic bands is shown to be suppressed by scattering due to the crystal lattice distortion and the impurity effect of Ru, while that of the Dirac cone is not significantly reduced due to the intrinsic character of Dirac cones. It is clearly shown from magnetoresistance and Hall coefficient measurements that the inverse of average mobility, proportional to cyclotron effective mass, develops as the square root of the carrier number (n) of the Dirac cones. This is the unique character of the Dirac cone linear dispersion relationship. Scattering of Ru on the Dirac cones is discussed in terms of the estimated mean free path using experimental parameters.
6 pages, 3 figures, To be published in Phys. Rev. B
References in corpus (7)
- The electronic properties of graphene
- Magnetism and Charge Dynamics in Iron Pnictides
- Nodal Spin Density Wave and band topology of the FeAs based materials
- Unconventional electronic reconstruction in undoped (Ba,Sr)FeAs across the spin density wave transition
- Electron and hole Dirac cone states in-pairs in Ba(FeAs) confirmed by magnetoresistance
- Effects of the Zero-Mode Landau Level on Inter-Layer Magnetoresistance in Multilayer Massless Dirac Fermion Systems
- Topological and Transport Properties of Dirac Fermions in Antiferromagnetic Metallic Phase of Iron-Based Superconductors
Cited by in corpus (4)
- Multiband Effect and Possible Dirac Fermions in FeTeSe
- Mobility spectrum analytical approach for intrinsic band picture of Ba(FeAs)
- Emergence of the minority hole with high mobility on the electrical transport in the Fe-pnictides Ba(FeMnAs)
- Effect of controlled point-like disorder induced by 2.5 MeV electron irradiation on nematic resistivity anisotropy of hole-doped (Ba,K)FeAs