Linear magnetoresistance in 2H-NbSe2 is explained by impeded cyclotron motion at CDW-induced scattering sinks that also suppress quantum oscillations.
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SU(2) gauge theory plus DMFT with long-wavelength magnetic fluctuations produces damping asymmetry in chargon hole pockets that forms Fermi arcs in the underdoped regime.
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$H$-linear magnetoresistance in NbSe$_2$ due to impeded cyclotron motion
Linear magnetoresistance in 2H-NbSe2 is explained by impeded cyclotron motion at CDW-induced scattering sinks that also suppress quantum oscillations.
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The pseudogap in high-$T_c$ superconductors from SU(2) gauge symmetry and dynamic correlation effects
SU(2) gauge theory plus DMFT with long-wavelength magnetic fluctuations produces damping asymmetry in chargon hole pockets that forms Fermi arcs in the underdoped regime.