Weyl semimetals are three dimensional analogs of graphene where the energy of the excitations are a linear function of their momentum. Pyrochlore Iridates (A2Ir2O7) with A =yttrium or lanthanide element) are conjectured to be examples of such a system, with the low energy physics described by twenty four Weyl nodes. An intriguing possibility is that these materials provide a physical realization of the Adler-Bell-Jackiw anomaly. In this letter we investigate the properties of pyrochlore iridates in an applied magnetic field. We find that the dispersion of the lowest landau level depends on the direction of the applied magnetic field. Consequently the velocity at low energies can be manipulated by changing the direction of the applied field. The resulting anisotropy in longitudinal conductivity is investigated. [7], and Majorana modes [7,8] are a few examples. A common feature of these systems is that the low energy physics is described by a two component Dirac Hamiltonian with the fermionic momentum is confined to two dimensions. Recently pyrochlore iridates have been conjectured to realize the Adler-Bell-Jackiw (ABJ)[9, 10] chiral anomaly, adding another example to the growing list.
GrapheneWan et al.[11] explored the possibility of the three dimensional analog of graphene being realized in the pyrochlore iridates. These materials have a large spin orbit couplings and are in a regime of intermediate correlations, making them promising candidates to realize topological insulators [12,13]. They have a magnetic ground state [14,15] and, within a LSDA+U+SO calculations, conjectured to be semi-metals. Most strikingly the low energy physics is described by the Weyl equation, which is the two component version of the Dirac equation. There are 24 Weyl nodes, three around each L point ([111] and equivalent directions) in the Brilloiun zone (see fig.1). Nodes related either by inversion or reflection about the {xy, yz, zx} planes have opposite chirality. Consequently the material is expected to have an anomalous hall response to applied uniaxial pressure and is susceptible to charge ordering in large magnetic fields [16].In a quantizing magnetic field, the Lowest Landua Level (LLL) is a linear function of the magnitude of a momentum, with the sign determined by the band structure. If an electric field is applied parallel to the magnetic field, the Adler-Bell-Jackiw (ABJ) [9,10] axial anomaly leads to an anomalous magneto-conductance. The origin of this effect is in the production of Weyl fermions of a given chirality and an equivalent annihilation of the opposite chirality [17]. This translates to a transfer of particles from one Weyl node to another of opposite chirality at a constant rate. To reach a steady state, this is balanced by inter-node scattering due to impurities.In the absence of the magnetic field, the intra-node scattering is quite effective in relaxing the momentum. In the presence of a large field, such that only the LLL is occupied, intra-node scattering is suppressed due to a lack of phase space. The...