We study electric field and temperature gradient driven magnetoconductivity of a Weyl semimetal system. To analyze the responses, we utilize the kinetic equation with semiclassical equations of motion modified by the Berry curvature and orbital magnetization of the wave-packet. Apart from known positive quadratic magnetoconductivity, we show that due to chiral anomaly, the magnetconductivity can become non-analytic function of the magnetic field, proportional to 3/2 power of the magnetic field at finite temperatures. We also show that time-reversal symmetry breaking tilt of the Dirac cones results in linear magnetoconductivity. This is due to one-dimensional chiral anomaly the tilt is responsible for.
PACS numbers:Introduction. Three dimensional Dirac and Weyl semimetals are materials whose band structure has a linearly touching conduction and valence bands, 1-4 the Dirac cones. Dirac semimetal is degenerate in electron's right and left chiralities, while the Weyl semimetal has the two chiralities split in energy or momentum. Inversion or time-reversal symmetries must be broken to obtain the splitting of chiralities in Dirac semimetal.Theoretically, the linear band touching introduces the non-trivial Berry 5 curvature in to the description of the fermion dynamics. The Berry curvature in this case is an effective magnetic field in k− space which is created by a magnetic monopole located at the band touching point. For a review on effects of Berry curvature on electronic properties see Ref. [6].Weyl semimetals with broken time-reversal symmetry are characterized by the anomalous Hall effect.4,7 Due to splitting of the Dirac cones, there are chiral edge states on the physical boundaries of the system.2,4 Apart from that there is the so-called chiral anomaly of the Dirac fermions -non-conservation of particles with a given chirality in presence of magnetic and electric fields.