344 research outputs found
First-Order Type Effects in YBaCuO at the Onset of Superconductivity
We present results of Raman scattering experiments on tetragonal for doping levels between 0 and
0.07 holes/CuO. Below the onset of superconductivity at , we find evidence of a diagonal superstructure. At ,
lattice and electron dynamics change discontinuously with the charge and spin
properties being renormalized at all energy scales. The results indicate that
charge ordering is intimately related to the transition at and
that the maximal transition temperature to superconductivity at optimal doping
depends on the type of ordering at .Comment: 4 pages, 4 figure
Electron interactions and charge ordering in LaSrCuO
We present results of inelastic light scattering experiments on
single-crystalline LaSrCuO in the doping range and TlBaCuO at and . The main
emphasis is placed on the response of electronic excitations in the
antiferromagnetic phase, in the pseudogap range, in the superconducting state,
and in the essentially normal metallic state at , where no
superconductivity could be observed. In most of the cases we compare B
and B spectra which project out electronic properties close to
and , respectively. In the channel of electron-hole excitations
we find universal behavior in B symmetry as long as the material
exhibits superconductivity at low temperature. In contrast, there is a strong
doping dependence in B symmetry: (i) In the doping range we observe rapid changes of shape and temperature dependence of the
spectra. (ii) In LaSrCuO new structures appear for
which are superposed on the electron-hole continuum. The temperature dependence
as well as model calculations support an interpretation in terms of
charge-ordering fluctuations. For the response from fluctuations
disappears at B and appears at B symmetry in full agreement with
the orientation change of stripes found by neutron scattering. While, with a
grain of salt, the particle-hole continuum is universal for all cuprates the
response from fluctuating charge order in the range is so
far found only in LaSrCuO. We conclude that
LaSrCuO is close to static charge order and, for this reason,
may have a suppressed .Comment: 17 pages, 15 figure
Magnetic Breakdown in the electron-doped cuprate superconductor NdCeCuO: the reconstructed Fermi surface survives in the strongly overdoped regime
We report on semiclassical angle-dependent magnetoresistance oscillations
(AMRO) and the Shubnikov-de Haas effect in the electron-overdoped cuprate
superconductor NdCeCuO. Our data provide convincing evidence
for magnetic breakdown in the system. This shows that a reconstructed
multiply-connected Fermi surface persists, at least at strong magnetic fields,
up to the highest doping level of the superconducting regime. Our results
suggest an intimate relation between translational symmetry breaking and the
superconducting pairing in the electron-doped cuprate superconductors.Comment: 5 pages, 4 figures, submitted to PR
Electronic structure of Pr_{2-x}Ce_xCuO_4 studied via ARPES and LDA+DMFT+\Sigma_k
The electron-doped Pr(2-x)Ce(x)CuO(4) (PCCO) compound in the pseudogap regime
(x~0.15) was investigated using angle-resolved photoemission spectroscopy
(ARPES) and the generalized dynamical mean-field theory (DMFT) with the
k-dependent self-energy (LDA+DMFT+\Sigma_k). Model parameters (hopping integral
values and local Coulomb interaction strength) for the effective one-band
Hubbard model were calculated by the local density approximation (LDA) with
numerical renormalization group method (NRG) employed as an "impurity solver"
in DMFT computations. An "external" k-dependent self-energy \Sigma_k was used
to describe interaction of correlated conducting electrons with short-range
antiferromagnetic (AFM) pseudogap fluctuations. Both experimental and
theoretical spectral functions and Fermi surfaces (FS) were obtained and
compared demonstrating good semiquantitative agreement. For both experiment and
theory normal state spectra of nearly optimally doped PCCO show clear evidence
for a pseudogap state with AFM-like nature. Namely, folding of quasiparticle
bands as well as presence of the "hot spots" and "Fermi arcs" were observed.Comment: 4 pages, 4 figures, as accepted to PRB Rapid Communications. Title is
changed by Editor
Identifying firing mammalian neurons in networks with high-resolution multi-transistor array (MTA)
Fermi Surface of the Electron-doped Cuprate Superconductor Nd_{2-x}Ce_xCuO_{4} Probed by High-Field Magnetotransport
We report on the study of the Fermi surface of the electron-doped cuprate
superconductor NdCeCuO by measuring the interlayer
magnetoresistance as a function of the strength and orientation of the applied
magnetic field. We performed experiments in both steady and pulsed magnetic
fields on high-quality single crystals with Ce concentrations of to
0.17. In the overdoped regime of we found both semiclassical
angle-dependent magnetoresistance oscillations (AMRO) and Shubnikov-de Haas
(SdH) oscillations. The combined AMRO and SdH data clearly show that the
appearance of fast SdH oscillations in strongly overdoped samples is caused by
magnetic breakdown. This observation provides clear evidence for a
reconstructed multiply-connected Fermi surface up to the very end of the
overdoped regime at . The strength of the superlattice potential
responsible for the reconstructed Fermi surface is found to decrease with
increasing doping level and likely vanishes at the same carrier concentration
as superconductivity, suggesting a close relation between translational
symmetry breaking and superconducting pairing. A detailed analysis of the
high-resolution SdH data allowed us to determine the effective cyclotron mass
and Dingle temperature, as well as to estimate the magnetic breakdown field in
the overdoped regime.Comment: 23 pages, 8 figure
An Investigation of Particle-Hole Asymmetry in the Cuprates via Electronic Raman Scattering
In this paper we examine the effects of electron-hole asymmetry as a
consequence of strong correlations on the electronic Raman scattering in the
normal state of copper oxide high temperature superconductors. Using
determinant quantum Monte Carlo simulations of the single-band Hubbard model,
we construct the electronic Raman response from single particle Green's
functions and explore the differences in the spectra for electron and hole
doping away from half filling. The theoretical results are compared to new and
existing Raman scattering experiments on hole-doped LaSrCuO
and electron-doped NdCeCuO. These findings suggest that the
Hubbard model with fixed interaction strength qualitatively captures the doping
and temperature dependence of the Raman spectra for both electron and hole
doped systems, indicating that the Hubbard parameter U does not need to be
doping dependent to capture the essence of this asymmetry.Comment: 13 pages, 10 figure
Advances in single crystal growth and annealing treatment of electron-doped HTSC
High quality electron-doped HTSC single crystals of and have been
successfully grown by the container-free traveling solvent floating zone
technique. The optimally doped and crystals have transition temperatures
of \,K and \,K, respectively, with a transition width of less than
\,K. We found a strong dependence of the optimal growth parameters on the Ce
content . We discuss the optimization of the post-growth annealing treatment
of the samples, the doping extension of the superconducting dome for both
compounds as well as the role of excess oxygen. The absolute oxygen content of
the as-grown crystals is determined from thermogravimetric experiments and is
found to be . This oxygen surplus is nearly completely removed by a
post-growth annealing treatment. The reduction process is reversible as
demonstrated by magnetization measurements. In as-grown samples the excess
oxygen resides on the apical site O(3). This apical oxygen has nearly no doping
effect, but rather influences the evolution of superconductivity by inducing
additional disorder in the CuO layers. The very high crystal quality of
is particularly manifest in magnetic quantum
oscillations observed on several samples at different doping levels. They
provide a unique opportunity of studying the Fermi surface and its dependence
on the carrier concentration in the bulk of the crystals.Comment: 19 pages, 7 figures, submitted to Eur. Phys. J.
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