19 research outputs found
Bulk Band Gap and Surface State Conduction Observed in Voltage-Tuned Crystals of the Topological Insulator BiSe
We report a transport study of exfoliated few monolayer crystals of
topological insulator BiSe in an electric field effect (EFE) geometry.
By doping the bulk crystals with Ca, we are able to fabricate devices with
sufficiently low bulk carrier density to change the sign of the Hall density
with the gate voltage . We find that the temperature and magnetic
field dependent transport properties in the vicinity of this can be
explained by a bulk channel with activation gap of approximately 50 meV and a
relatively high mobility metallic channel that dominates at low . The
conductance (approximately 2 7), weak anti-localization, and
metallic resistance-temperature profile of the latter lead us to identify it
with the protected surface state. The relative smallness of the observed gap
implies limitations for EFE topological insulator devices at room temperature.Comment: 4 pages, 4 figures. In new version, panels have been removed from
Figures 1, 2, and 4 to improve clarity. Additional data included in Figure 4.
Introduction and discussion revised and expande
Thermal Hall Conductivity as a Probe of Gap Structure in Multi-band Superconductors: The Case of
The sign and profile of the thermal Hall conductivity gives
important insights into the gap structure of multi-band superconductors. With
this perspective, we have investigated and the thermal
conductivity in which display large
peak anomalies in the superconducting state. The anomalies imply that a large
hole-like quasiparticle (qp) population exists below the critical temperature
. We show that the qp mean-free-path inferred from
reproduces the observed anomaly in , providing a consistent
estimate of a large qp population. Further, we demonstrate that the hole-like
signal is consistent with a theoretical scenario where despite potentially
large gap variations on the electron pockets, the minimal homogeneous gap of
the superconducting phase resides at a hole pocket. Implications for probing
the gap structure in the broader class of pnictide superconductors are
discussed.Comment: 5 pages, 4 figures. Orientation significantly updated from previous
(0811.4668v1) reflecting new theoretical understanding of experimental
results and physical implications. Introduction, discussion, and figures
updated including additional figure for model calculatio
Superconductivity in CuxBi2Se3 and its implications for pairing in the undoped topological insulator
Bi2Se3 is one of a handful of known topological insulators. Here we show that
copper intercalation in the van der Waals gaps between the Bi2Se3 layers,
yielding an electron concentration of ~ 2 x 10^20cm-3, results in
superconductivity at 3.8 K in CuxBi2Se3 for x between 0.12 and 0.15. This
demonstrates that Cooper pairing is possible in Bi2Se3 at accessible
temperatures, with implications for study of the physics of topological
insulators and potential devices.Comment: 6 pages, 4 figure
Nernst-Ettingshausen effect in two-component electronic liquids
A simple model describing the Nernst-Ettingshausen effect (NEE) in
two-component electronic liquids is formulated. The examples considered include
graphite, where the normal and Dirac fermions coexist, superconductor in
fluctuating regime, with coexisting Cooper pairs and normal electrons, and the
inter-stellar plasma of electrons and protons. We give a general expression for
the Nernst constant and show that the origin of a giant NEE is in the strong
dependence of the chemical potential on temperature in all cases
p-type Bi2Se3 for topological insulator and low temperature thermoelectric applications
The growth and elementary properties of p-type Bi2Se3 single crystals are
reported. Based on a hypothesis about the defect chemistry of Bi2Se3, the
p-type behavior has been induced through low level substitutions (1 percent or
less) of Ca for Bi. Scanning tunneling microscopy is employed to image the
defects and establish their charge. Tunneling and angle resolved photoemission
spectra show that the Fermi level has been lowered into the valence band by
about 400 meV in Bi1.98Ca0.02Se3 relative to the n-type material. p-type single
crystals with ab plane Seebeck coefficients of +180 microVK-1 at room
temperature are reported. These crystals show a giant anomalous peak in the
Seebeck coefficient at low temperatures, reaching +120 microVK-1 at 7 K, giving
them a high thermoelectric power factor at low temperatures. In addition to its
interesting thermoelectric properties, p-type Bi2Se3 is of substantial interest
for studies of technologies and phenomena proposed for topological insulators.Comment: v2: STM characterization of n and p type Bi2Se3 is adde
Low temperature vortex liquid in
In the cuprates, the lightly-doped region is of major interest because
superconductivity, antiferromagnetism, and the pseudogap state
\cite{Timusk,Lee,Anderson} come together near a critical doping value .
These states are deeply influenced by phase fluctuations \cite{Emery} which
lead to a vortex-liquid state that surrounds the superconducting region
\cite{WangPRB01,WangPRB06}. However, many questions
\cite{Doniach,Fisher,FisherLee,Tesanovic,Sachdev} related to the nature of the
transition and vortex-liquid state at very low tempera- tures remain open
because the diamagnetic signal is difficult to resolve in this region. Here, we
report torque magnetometry results on (LSCO) which show
that superconductivity is lost at by quantum phase fluctuations. We find
that, in a magnetic field , the vortex solid-to-liquid transition occurs at
field much lower than the depairing field . The vortex liquid
exists in the large field interval , even in the limit 0.
The resulting phase diagram reveals the large fraction of the - plane
occupied by the quantum vortex liquid.Comment: 6 pages, 4 figures, submitted to Nature Physic
Development of ferromagnetism in the doped topological insulator Bi_(2−x)Mn_xTe_3
The development of ferromagnetism in Mn-doped Bi_2Te_3 is characterized through measurements on a series of single crystals with different Mn content. Scanning tunneling microscopy analysis shows that the Mn substitutes on the Bi sites, forming compounds of the type Bi_(2−x)Mn_xTe_3, and that the Mn substitutions are randomly distributed, not clustered. Mn doping first gives rise to local magnetic moments with Curie-like behavior, but by the compositions Bi_(1.96)Mn_(0.04)Te_3 and Bi_(1.91)Mn_(0.09)Te_3, a second-order ferromagnetic transition is observed, with T_C∼9–12 K. The easy axis of magnetization in the ferromagnetic phase is perpendicular to the Bi2Te3 basal plane. Thermoelectric power and Hall effect measurements show that the Mn-doped Bi_2Te_3 crystals are p-type. Angle-resolved photoemission spectroscopy measurements show that the topological surface states that are present in pristine Bi_2Te_3 are also present at 15 K in ferromagnetic Mn-doped Bi2−xMnxTe3 and that the dispersion relations of the surface states are changed in a subtle fashion
Momentum dependence of superconducting gap, strong-coupling dispersion kink, and tightly bound Cooper pairs in the high-T_c (Sr,Ba)_(1−x)(K,Na)_xFe_2As_2 superconductors
We present a systematic angle-resolved photoemission spectroscopic study of the high-Tc superconductor class (Sr/Ba)_(1−x)K_xFe_2As_2. By utilizing a photon-energy-modulation contrast and scattering geometry we report the Fermi surface and the momentum dependence of the superconducting gap, Δ(k⃗ ). A prominent quasiparticle dispersion kink reflecting strong scattering processes is observed in a binding-energy range of 25–55 meV in the superconducting state, and the coherence length or the extent of the Cooper pair wave function is found to be about 20 Å, which is uncharacteristic of a superconducting phase realized by the BCS-phonon-retardation mechanism. The observed 40±15 meV kink likely reflects contributions from the frustrated spin excitations in a J_1-J_2 magnetic background and scattering from the soft phonons. Results taken collectively provide direct clues to the nature of the pairing potential including an internal phase-shift factor in the superconducting order parameter which leads to a Brillouin zone node in a strong-coupling setting