Origin of extremely large magnetoresistance in the candidate type-II Weyl semimetal MoTe(2−x)

The recent observation of extremely large magnetoresistance (MR) in the transition-metal dichalcogenide MoTe(2) has attracted considerable interest due to its potential technological applications as well as its relationship with novel electronic states predicted for a candidate type-II Weyl semimetal. In order to understand the origin of the MR, the electronic structure of MoTe(2−x) (x = 0.08) is systematically tuned by application of pressure and probed via its Hall and longitudinal conductivities. With increasing pressure, a monoclinic-to-orthorhombic (1 T′ to T(d)) structural phase transition temperature (T*) gradually decreases from 210 K at 1 bar to 58 K at 1.1 GPa, and there is no anomaly associated with the phase transition at 1.4 GPa, indicating that a T = 0 K quantum phase transition occurs at a critical pressure (P(c)) between 1.1 and 1.4 GPa. The large MR observed at 1 bar is suppressed with increasing pressure and is almost saturated at 100% for P > P(c). The dependence on magnetic field of the Hall and longitudinal conductivities of MoTe(2−x) shows that a pair of electron and hole bands are important in the low-pressure T(d) phase, while another pair of electron and hole bands are additionally required in the high-pressure 1 T′ phase. The MR peaks at a characteristic hole-to-electron concentration ratio (n(c)) and is sharply suppressed when the ratio deviates from n(c) within the T(d) phase. These results establish the comprehensive temperature-pressure phase diagram of MoTe(2−x) and underscore that its MR originates from balanced electron-hole carrier concentrations.