Magnetotransport across Weyl semimetal grain boundaries
arXiv:2509.09668 · doi:10.1103/99q1-37q7
Abstract
A clean interface between two Weyl semimetals features a universal, field-linear tunnel magnetoconductance of per magnetic flux quantum, where is the number of chirality-preserving topological interface Fermi arcs. In this work we show that the linearity of the magnetoconductance is robust with to interface disorder. The slope of the magnetoconductance changes at a characteristic field strength -- the field strength for which the time taken to traverse the Fermi arc due to the Lorentz force is equal to the mean inter-arc scattering time. For fields much larger than , the magnetoconductance is unaffected by disorder. For fields much smaller than , the slope is no longer determined by but by the simple fraction , where and are the numbers of Weyl-node pairs in the left and right Weyl semimetal, respectively. We also consider the effect of spatially correlated disorder potentials, where we find that decreases exponentially with increasing correlation length. Our results provide a possible explanation for the recently observed robustness of the negative linear magnetoresistance in grained Weyl semimetals.
8+3 pages, 6 figures
References in corpus (9)
- Quantized Transport in Graphene p-n Junctions in Magnetic Field
- Surface conduction and reduced electrical resistivity in ultrathin noncrystalline NbP semimetal
- Fermi arc reconstruction at the interface of twisted Weyl semimetals
- Robust negative longitudinal magnetoresistance and spin-orbit torque in sputtered Pt3Sn topological semimetal
- Surface-dominated conductance scaling in Weyl semimetal NbAs
- Atomically Sharp Internal Interface in a Chiral Weyl Semimetal Nanowire
- Fermi-arc metals
- Magnetic Breakdown and Chiral Magnetic Effect at Weyl-Semimetal Tunnel Junctions
- Quantum Oscillation Signatures of Fermi Arcs in Tunnel Magnetoconductance