83 research outputs found
Lattice effects in the LaSrCuO compounds
Systematic Raman studies on several cuprates (YBaCuO, YBaCuO or BiSrCaCuO) have shown that at optimal doping the compounds
are at the edge of lattice instability; once this level is exceeded, by means
of doping or applying external hydrostatic pressure, the changes in the
transition temperature are accompanied by spectral modifications. There are
strong indications that the reduction in T is correlated with a
separation into nanoscale phases, which involve the oxygen atoms of the
CuO planes. In this work, modifications with doping in the Raman
spectra of the LaSrCuO compound are presented,
which show that spin or charge ordering is coupled with lattice distortions in
the whole doping region.Comment: 6 pages, 6 figure
Pressure-induced lattice instabilities and superconductivity in YBa2Cu4O8 and optimally doped YBa2Cu3O7-{\delta}
Combined synchrotron angle-dispersive powder diffraction and micro-Raman
spectroscopy are used to investigate the pressure-induced lattice instabilities
that are accompanied by T anomalies in YBaCuO, in comparison with the optimally doped YBaCuO and the non-superconducting PrBaCuO. In the first two superconducting systems there is a clear
anomaly in the evolution of the lattice parameters and an increase of lattice
disorder with pressure, that starts at as well as
irreversibility that induces a hysteresis. On the contrary, in the Pr-compound
the lattice parameters follow very well the expected equation of state (EOS) up
to 7 GPa. In complete agreement with the structural data, the micro-Raman data
of the superconducting compounds show that the energy and width of the A phonons show anomalies at the same pressure range where the lattice
parameters deviate from the EOS and the average Cu2-O bond length
exhibits a strong contraction and correlate with the non-linear pressure
dependence of T. This is not the case for the non superconducting Pr
sample, clearly indicating a connection with the charge carriers. It appears
that the cuprates close to optimal doping are at the edge of lattice
instability.Comment: 6 pages, 7 figure
Isotope effect on the E2g phonon and mesoscopic phase separation near the electronic topological transition in Mg1-xAlxB2
We report the boron isotope effect on the E2g phonon mode by micro-Raman
spectroscopy on the ternary Mg1-xAlxB2 system, synthesized with pure isotopes
10B and 11B. The isotope coefficient on the phonon frequency is near 0.5 in the
full range decreasing near x = 0. The intraband electron-phonon (e-ph)
coupling, for the electrons in the sigma band, has been extracted from the E2g
line-width and frequency softening. Tuning the Fermi energy near the electronic
topological transition (ETT), where the sigma Fermi surface changes from 2D to
3D topology the E2g mode, shows the known Kohn anomaly on the 2D side of the
ETT and a splitting of the E2g phonon frequency into a hard and soft component
from x = 0 to x = 0.28. The results suggest a minor role of the intraband
phonon mediated pairing in the control of the high critical temperature in
Mg1-xAlxB2. The common physical features of diborides with the novel multigap
FeAs-based superconductors and cuprates is discussed.Comment: 19 pages, 6 figure
Local lattice distortions vs. structural phase transition in NdFeAsO1-xFx
The lattice properties at low temperatures of two samples of NdFeAsO1-xFx
(x=0.05 and 0.25) have been examined in order to investigate possible
structural phase transition that may occur in the optimally doped
superconducting sample with respect to the non-superconducting low-F
concentration compound. In order to detect small modifications in the ion
displacements with temperature micro-Raman and high resolution synchrotron
powder diffraction measurements were carried out. No increase of the width of
the (220) or (322) tetragonal diffraction peaks and microstrains could be found
in the superconducting sample from synchrotron XRD measurements. On the other
hand, the atomic displacement parameters deviate from the expected behavior, in
agreement with modifications in the phonon width, as obtained by Raman
scattering. These deviations occur around 150 K for both F dopings, with
distinct differences among the two compounds, i.e., they decrease at low doping
and increase for the superconducting sample. The data do not support a hidden
phase transition to an orthorhombic phase in the superconducting compound, but
point to an isostructural lattice deformation. Based on the absence of magnetic
effects in this temperature range for the superconducting sample, we attribute
the observed lattice anomalies to the formation of local lattice distortions
that, being screened by the carriers, can only acquire long-range coherence by
means of a structural phase transition at low doping levels
Technologies and extraction methods of polyphenolic compounds derived from pomegranate (Punica granatum) peels. a mini review
The interest in using plant by-product extracts as functional ingredients is continuously rising due to environmental and financial prospects. The development of new technologies has led to the achievement of aqueous extracts with high bioactivity that is preferable due to organic solvents nonuse. Recently, widely applied and emerging technologies, such as Simple Stirring, Pressure-Applied Extraction, Enzymatic Extraction, Ultrasound-Assisted Extraction, Pulsed Electric Fields, High Hydrostatic Pressure, Ohmic Heating, Microwave Assistant Extraction and the use of “green” solvents such as the deep eutectic solvents, have been investigated in order to contribute to the minimization of disadvantages on the extraction of bioactive compounds. This review is focused on bioactive compounds derived from pomegranate (Punica granatum) peels and highlighted the most attractive extraction methods. It is believed that these findings could be a useful tool for the pomegranate juices industry to apply an effective and economically viable extraction process, transforming a by-product to a high added value functional product. © 2021 by the authors. Licensee MDPI, Basel, Switzerland
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