The Hall number across a van Hove singularity
arXiv:1611.03875 · doi:10.1103/PhysRevB.96.045132
Abstract
In the context of the relaxation time approximation to Boltzmann transport theory, we examine the behavior of the Hall number, , of a metal in the neighborhood of a Lifshitz transition from a closed Fermi surface to open sheets. We find a universal non-analytic dependence of on the electron density in the high field limit, but a non-singular dependence at low fields. The existence of an assumed nematic transition produces a doping dependent similar to that observed in recent experiments in the high temperature superconductor YBaCuO.
References added, text modified to include extended discussion of the modified Figure 4. 5 pages, 4 figures, with 13 pages of Supplemental Material
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- Intrinsic nonlinear Hall effect and gate-switchable Berry curvature sliding in twisted bilayer graphene
- Restored strange metal phase through suppression of charge density waves in underdoped YBaCuO
- Vanishing nematic order beyond the pseudogap phase in overdoped cuprate superconductors
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- Charge carrier drop at the onset of pseudogap behavior in the two-dimensional Hubbard model
- Transport signatures of the pseudogap critical point in the cuprate superconductor BiSrLaCuO
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- Origin of anomalous magnetotransport in kagome superconductors AVSb (A=K,Rb,Cs)
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