976 research outputs found
Electronic structure basis for the titanic magnetoresistance in WTe
The electronic structure basis of the extremely large magnetoresistance in
layered non-magnetic tungsten ditelluride has been investigated by
angle-resolved photoelectron spectroscopy. Hole and electron pockets of
approximately the same size were found at the Fermi level, suggesting that
carrier compensation should be considered the primary source of the effect. The
material exhibits a highly anisotropic, quasi one-dimensional Fermi surface
from which the pronounced anisotropy of the magnetoresistance follows. A change
in the Fermi surface with temperature was found and a high-density-of-states
band that may take over conduction at higher temperatures and cause the
observed turn-on behavior of the magnetoresistance in WTe was identified
Gapped Surface States in a Strong-Topological-Semimetal
A three-dimensional strong-topological-insulator or -semimetal hosts
topological surface states which are often said to be gapless so long as
time-reversal symmetry is preserved. This narrative can be mistaken when
surface state degeneracies occur away from time-reversal-invariant momenta. The
mirror-invariance of the system then becomes essential in protecting the
existence of a surface Fermi surface. Here we show that such a case exists in
the strong-topological-semimetal BiSe. Angle-resolved photoemission
spectroscopy and \textit{ab initio} calculations reveal partial gapping of
surface bands on the BiSe-termination of BiSe(111), where an 85
meV gap along closes to zero toward the mirror-invariant
azimuth. The gap opening is attributed to an interband
spin-orbit interaction that mixes states of opposite spin-helicity.Comment: 5 pages, 3 figure
Tunneling in graphene-topological insulator hybrid devices
Hybrid graphene-topological insulator (TI) devices were fabricated using a
mechanical transfer method and studied via electronic transport. Devices
consisting of bilayer graphene (BLG) under the TI BiSe exhibit
differential conductance characteristics which appear to be dominated by
tunneling, roughly reproducing the BiSe density of states. Similar
results were obtained for BLG on top of BiSe, with 10-fold greater
conductance consistent with a larger contact area due to better surface
conformity. The devices further show evidence of inelastic phonon-assisted
tunneling processes involving both BiSe and graphene phonons. These
processes favor phonons which compensate for momentum mismatch between the TI
and graphene points. Finally, the utility of these tunnel
junctions is demonstrated on a density-tunable BLG device, where the
charge-neutrality point is traced along the energy-density trajectory. This
trajectory is used as a measure of the ground-state density of states
Quasiparticle Liquid in the Highly Overdoped Bi2212
We present results from the study of a highly overdoped (OD) Bi2212 with a
K using high resolution angle-resolved photoemission spectroscopy.
The temperature dependent spectra near the () point show the presence of
the sharp peak well above . From the nodal direction, we make comparison
of the self-energy with the optimally doped and underdoped cuprates, and the
Mo(110) surface state. We show that this OD cuprate appears to have properties
that approach that of the Mo. Further analysis shows that the OD has a more
-independent lineshape at the Fermi surface than the lower-doped cuprates.
This allows for a realistic comparison of the nodal lifetime values to the
experimental resistivity measurements via Boltzmann transport formulation. All
these observations point to the validity of the quasiparticle picture for the
OD even in the normal state within a certain energy and momentum range.Comment: 4 pages, 4 figure
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