1,557 research outputs found
Correlation between and anisotropic scattering in TlBaCuO
Angle-dependent magnetoresistance measurements are used to determine the
isotropic and anisotropic components of the transport scattering rate in
overdoped TlBaCuO for a range of values between 15K
and 35K. The size of the anisotropic scattering term is found to scale linearly
with , establishing a link between the superconducting and normal state
physics. Comparison with results from angle resolved photoemission spectroscopy
indicates that the transport and quasiparticle lifetimes are distinct.Comment: 5 pages, 3 figures, accepted for publication in Physical Review
Letter
Telephone or video? A review of telemedicine consultations during the COVID-19 pandemic in a spinal MSK service
A service evaluation of the move to virtual appointments during the COVID-19 pandemic
Violation of the isotropic- approximation in overdoped La_{2-x}Sr_xCuO_4
Magnetotransport measurements on the overdoped cuprate La_{1.7}Sr_{0.3}CuO_4
are fitted using the Ong construction and band parameters inferred from
angle-resolved photoemission. Within a band picture, the low temperature Hall
data can only be fitted satisfactorily by invoking strong basal-plane
anisotropy in the mean-free-path . This violation of the isotropic-
approximation supports a picture of dominant small-angle elastic scattering in
cuprates due to out-of-plane substitutional disorder. We show that both band
anisotropy and anisotropy in the elastic scattering channel strongly
renormalize the Hall coefficient in overdoped La_{2-x}Sr_xCuO_4 over a wide
doping and temperature range.Comment: 4 pages, 4 figure
Shubnikov de Haas effect in the metallic state of NaCoO
Shubnikov de Haas oscillations for two well defined frequencies,
corresponding respectively to areas of 0.8 and 1.36% of the first Brillouin
zone (FBZ), were observed in single crystals of NaCoO. The
existence of Na superstructures in NaCoO, coupled with this
observation, suggests the possibility that the periods are due to the
reconstruction of the large Fermi surface around the point. An
alternative interpretation in terms of the long sought-after
pockets is also considered but found to be incompatible
with existing specific heat data.Comment: 5 pages 4 figure
Interlayer transverse magnetoresistance in the presence of an anisotropic pseudogap
The interlayer magnetoresistance of a quasi-two-dimensional layered metal with a d-wave pseudogap is calculated semiclassically. An expression for the interlayer resistivity as a function of the strength and direction of the magnetic field, the magnitude of the pseudogap, temperature, and scattering rate is obtained. We find that the pseudogap, by introducing low-energy nodal quasiparticle contours, smooths the dependence on field direction in a manner characteristic of its anisotropy. We thus propose that interlayer resistance measurements under a strong field of variable orientation can be used to fully characterize an anisotropic pseudogap. The general result is applied to the case of a magnetic field parallel to the conducting layers using a model band structure appropriate for overdoped Tâ„“2201
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