$B^2$ to $B$-linear magnetoresistance due to impeded orbital motion
R. D. H. Hinlopen, F. A. Hinlopen, J. Ayres, N. E. Hussey

TL;DR
This paper proposes a fundamental principle explaining the ubiquitous linear magnetoresistance in strange metals, attributing it to regions on the Fermi surface that impede orbital motion, leading to a universal behavior across various correlated materials.
Contribution
It introduces a theoretical framework linking Fermi surface features to linear magnetoresistance, independent of specific material details.
Findings
Bounded sectors on the Fermi surface can cause B-linear magnetoresistance.
The theory accounts for the transition from quadratic to linear behavior.
Impeding orbital motion is a key mechanism in anomalous magnetotransport.
Abstract
Strange metals exhibit a variety of anomalous magnetotransport properties, the most striking of which is a resistivity that increases linearly with magnetic field over a broad temperature and field range. The ubiquity of this behavior across a spectrum of correlated metals - both single- and multi-band, with either dominant spin and/or charge fluctuations, of varying levels of disorder or inhomogeneity and in proximity to a quantum critical point or phase - obligates the search for a fundamental underlying principle that is independent of the specifics of any material. Strongly anisotropic (momentum-dependent) scattering can generate -linear magnetoresistance but only at intermediate field strengths. At high enough fields, the magnetoresistance must eventually saturate. Here, we consider the ultimate limit of such anisotropy, a region or regions on the Fermi surface that impede…
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Taxonomy
TopicsSuperconducting Materials and Applications · Physics of Superconductivity and Magnetism
