Randomized trial explores the coexistence of electronic phases in low-electron-density n-HgTe, implying new insights for material applications.
Magnetotransport phenomena are investigated in a nominally pure n-HgTe single crystal with an exceptionally low electron concentration of 7.3 × 1014 cm−3. The results enable the proposal and validation of a band model positing the coexistence of two distinct electronic phases within the Brillouin zone: a trivial (intrinsic gapless) phase and a nontrivial (Weyl semimetal) phase. The trivial phase is identified by two principal signatures: a T32 power-law temperature dependence of the electron concentration and a strictly quadratic magnetic-field dependence of the transverse magnetoresistance at elevated temperatures. Conversely, the nontrivial phase is characterized by three key hallmarks: a large, non-saturating transverse magnetoresistance at low temperatures; the observation of the chiral magnetic effect as a direct consequence of the chiral anomaly; and an unconventional magnetic-field dependence of the Hall resistance at 0.3 K, which may be indicative of Weyl node annihilation in the quantum limit. Based on this second set of signatures, low-electron-density n-HgTe can be classified as a suitable candidate for a non-centrosymmetric Weyl semimetal. The obtained results are of significant interest both for fundamental condensed matter physics and for potential applications in spintronics, optoelectronics, and magnetic sensorics.
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Lonchakov et al. (2026) studied this question.
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