146 research outputs found
Fermi-surface transformation across the pseudogap critical point of the cuprate superconductor LaNdSrCuO
The electrical resistivity and Hall coefficient R of the
tetragonal single-layer cuprate Nd-LSCO were measured in magnetic fields up to
T, large enough to access the normal state at , for closely
spaced dopings across the pseudogap critical point at .
Below , both coefficients exhibit an upturn at low temperature, which
gets more pronounced with decreasing . Taken together, these upturns show
that the normal-state carrier density at drops upon entering the
pseudogap phase. Quantitatively, it goes from at to at . By contrast, the mobility does not change appreciably, as
revealed by the magneto-resistance. The transition has a width in doping and
some internal structure, whereby R responds more slowly than to the
opening of the pseudogap. We attribute this difference to a Fermi surface that
supports both hole-like and electron-like carriers in the interval , with compensating contributions to R. Our data are in excellent
agreement with recent high-field data on YBCO and LSCO. The quantitative
consistency across three different cuprates shows that a drop in carrier
density from to is a universal signature of the pseudogap
transition at . We discuss the implication of these findings for the
nature of the pseudogap phase.Comment: 11 pages, 12 figure
Spectroscopic Fingerprint of Phase-Incoherent Superconductivity in the Cuprate Pseudogap State
A possible explanation for the existence of the cuprate "pseudogap" state is
that it is a d-wave superconductor without quantum phase rigidity. Transport
and thermodynamic studies provide compelling evidence that supports this
proposal, but few spectroscopic explorations of it have been made. One
spectroscopic signature of d-wave superconductivity is the particle-hole
symmetric "octet" of dispersive Bogoliubov quasiparticle interference
modulations. Here we report on this octet's evolution from low temperatures to
well into the underdoped pseudogap regime. No pronounced changes occur in the
octet phenomenology at the superconductor's critical temperature Tc, and it
survives up to at least temperature T ~ 1.5Tc. In the pseudogap regime, we
observe the detailed phenomenology that was theoretically predicted for
quasiparticle interference in a phase-incoherent d-wave superconductor. Thus,
our results not only provide spectroscopic evidence to confirm and extend the
transport and thermodynamics studies, but they also open the way for
spectroscopic explorations of phase fluctuation rates, their effects on the
Fermi arc, and the fundamental source of the phase fluctuations that suppress
superconductivity in underdoped cuprates.Comment: 27 pages, 12 figure
Ground simulations of electron current to wide probes for electrodynamic tethers
Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/76486/1/AIAA-2001-3337-341.pd
Nernst Effect of stripe ordering LaEuSrCuO
We investigate the transport properties of
LaEuSrCuO (, 0.08, 0.125, 0.15, 0.2) with a
special focus on the Nernst effect in the normal state. Various anomalous
features are present in the data. For and 0.15 a kink-like anomaly is
present in the vicinity of the onset of charge stripe order in the LTT phase,
suggestive of enhanced positive quasiparticle Nernst response in the stripe
ordered phase. At higher temperature, all doping levels except exhibit
a further kink anomaly in the LTO phase which cannot unambiguously be related
to stripe order. Moreover, a direct comparison between the Nernst coefficients
of stripe ordering LaEuSrCuO and superconducting
LaSrCuO at the doping levels and reveals
only weak differences. Our findings make high demands on any scenario
interpreting the Nernst response in hole-doped cuprates
Mammalian Whiskers and the Euler Spiral
Mammal whiskers are often used as a model for understanding the sensory circuits in the brain. Signals from the whiskers, especially their forces, are processed throughout the brain, particularly in the somatosensory “barrel” cortex. Before attempting to interpret the neuronal signals, it is imperative to understand the signals received by the whisker follicles themselves and therefore accurately modelling whisker mechanics is important. Previously, whiskers have been modelled as a parabola based on Cartesian coordinates of the whisker centerline, but we propose that an Euler spiral model is a simple way to capture many aspects of whisker shape. In this study, we model 516 rat (Rattus norvegicus) whiskers as plane model curves with a linear relationship between arc length, s, and curvature, k, such that k(s) = A(s) + B and show that any original rat whisker can be mapped onto a normalized Euler spiral. The Euler spiral provides a convenient and highly accurate model for analytical studies, particularly intrinsically curved rods such as whiskers. The simplistic description in terms of coefficients A and B allows average whiskers to be created from data sets. In addition, vibrissae of many different species, such as pygmy shrew or grey seal, can be readily compared based on their shape alone
Direct measurement of the upper critical field in a cuprate superconductor
The upper critical field Hc2 is a fundamental measure of the pairing
strength, yet there is no agreement on its magnitude and doping dependence in
cuprate superconductors. We have used thermal conductivity as a direct probe of
Hc2 in the cuprates YBa2Cu3Oy and YBa2Cu4O8 to show that there is no vortex
liquid at T = 0, allowing us to use high-field resistivity measurements to map
out the doping dependence of Hc2 across the phase diagram. Hc2(p) exhibits two
peaks, each located at a critical point where the Fermi surface undergoes a
transformation. The condensation energy obtained directly from Hc2, and
previous Hc1 data, undergoes a 20-fold collapse below the higher critical
point. These data provide quantitative information on the impact of competing
phases in suppressing superconductivity in cuprates.Comment: to appear in Nature Communications; Supplementary Information file
available upon reques
Superconducting Fluctuation investigated by THz Conductivity of LaSrCuO Thin Films
Frequency-dependent terahertz conductivities of LaSrCuO thin
films with various carrier concentrations were investigated. The imaginary part
of the complex conductivity considerably increased from far above a
zero-resistance superconducting transition temperature,
, because of the existence of the fluctuating
superfluid density with a short lifetime. The onset temperature of the
superconducting fluctuation is at most for
underdoped samples, which is consistent with the previously reported analysis
of microwave conductivity. The superconducting fluctuation was not enhanced
under a 0.5 T magnetic field. We also found that the temperature dependence of
the superconducting fluctuation was sensitive to the carrier concentration of
LaSrCuO, which reflects the difference in the nature of the
critical dynamics near the superconducting transition temperature. Our results
suggest that the onset temperature of the Nernst signal is not related to the
superconducting fluctuation we argued in this paper.Comment: J. Phys. Soc. Jpn. in pres
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