Extended Data Fig. 3: Success of ADMR-derived modelling of the in-plane transport of overdoped Tl2201.
From: Incoherent transport across the strange-metal regime of overdoped cuprates
a, The c-axis ADMR of Tl2201 with Tc = 15 K measured at 50 K and at various (labelled) azimuthal angles taken from ref. 48. b, Projection of the in-plane Fermi surface derived from the ADMR fitting. c, Schematic showing the isotropic T2 component (black solid line) and anisotropic T + T2 component (red solid line) of the scattering rate as deduced from the ADMR fitting. d, Black dots: ρab(T) data for overdoped Tl2201 (Tc = 15 K) in which superconductivity has been suppressed by a magnetic field (H ‖ c)46 and corresponding simulation based on the ADMR fitting48. The difference in the residual resistivities is probably because different samples have been used in the two studies46,48. e, Corresponding simulation for RH(T)48. f, Simulation of RH(H) = ρxy(H)/H at various temperatures as indicated. g, Same simulation data plotted versus H/ρ(0) where here, ρ(0) is the zero-field resistivity at each temperature. h, RH(H) versus H/ρ(0) data taken from ref. 25. For overdoped Tl2201 (Tc = 25 K) for comparison with the simulation in g. The larger absolute values of RH in h relative to g are due to the fact that the high-field data in h are taken on a sample with a higher Tc value where the anisotropy in τ−1(ϕ) is expected to be larger.
