5 research outputs found
Giant Mechanocaloric Effects in Fluorite-Structured Superionic Materials
Mechanocaloric
materials experience a change in temperature when a mechanical stress
is applied on them adiabatically. Thus, far, only ferroelectrics and
superelastic metallic alloys have been considered as potential mechanocaloric
compounds to be exploited in solid-state cooling applications. Here
we show that giant mechanocaloric effects occur in hitherto overlooked
fast ion conductors (FIC), a class of multicomponent materials in
which above a critical temperature, <i>T</i><sub>s</sub>, a constituent ionic species undergoes a sudden increase in mobility.
Using first-principles and molecular dynamics simulations, we found
that the superionic transition in fluorite-structured FIC, which is
characterized by a large entropy increase of the order of 10<sup>2</sup> JK<sup>–1</sup> kg<sup>–1</sup>, can be externally
tuned with hydrostatic, biaxial, or uniaxial stresses. In particular, <i>T</i><sub>s</sub> can be reduced several hundreds of degrees
through the application of moderate tensile stresses due to the concomitant
drop in the formation energy of Frenkel pair defects. We predict that
the adiabatic temperature change in CaF<sub>2</sub> and PbF<sub>2</sub>, two archetypal fluorite-structured FIC, close to their critical
points are of the order of 10<sup>2</sup> and 10<sup>1</sup> K, respectively.
This work advocates that FIC constitute a new family of mechanocaloric
materials showing great promise for prospective solid-state refrigeration
applications
Electronic, Vibrational, and Structural Properties of the Natural Mineral Ferberite (FeWO<sub>4</sub>): A High-Pressure Study
This paper reports an experimental high-pressure study
of natural
mineral ferberite (FeWO4) up to 20 GPa using diamond-anvil
cells. First-principles calculations have been used to support and
complement the results of the experimental techniques. X-ray diffraction
patterns show that FeWO4 crystallizes in the wolframite
structure at ambient pressure and is stable over a wide pressure range,
as is the case for other wolframite AWO4 (A = Mg, Mn, Co,
Ni, Zn, or Cd) compounds. No structural phase transitions were observed
for FeWO4, in the pressure range investigated. The bulk
modulus (B0 = 136(3) GPa) obtained from
the equation of state is very close to the recently reported value
for CoWO4 (131(3) GPa). According to our optical absorption
measurements, FeWO4 has an indirect band gap that decreases
from 2.00(5) eV at ambient pressure to 1.56(5) eV at 16 GPa. First-principles
simulations yield three infrared-active phonons, which soften with
pressure, in contrast to the Raman-active phonons. These results agree
with Raman spectroscopy experiments on FeWO4 and are similar
to those previously reported for MgWO4. Our results on
FeWO4 are also compared to previous results on other wolframite-type
compounds
New Polymorph of InVO<sub>4</sub>: A High-Pressure Structure with Six-Coordinated Vanadium
A new wolframite-type polymorph of
InVO<sub>4</sub> is identified under compression near 7 GPa by in
situ high-pressure (HP) X-ray diffraction (XRD) and Raman spectroscopic
investigations on the stable orthorhombic InVO<sub>4</sub>. The structural
transition is accompanied by a large volume collapse (Δ<i>V</i>/<i>V</i> = −14%) and a drastic increase
in bulk modulus (from 69 to 168 GPa). Both techniques also show the
existence of a third phase coexisting with the low- and high-pressure
phases in a limited pressure range close to the transition pressure.
XRD studies revealed a highly anisotropic compression in orthorhombic
InVO<sub>4</sub>. In addition, the compressibility becomes nonlinear
in the HP polymorph. The volume collapse in the lattice is related
to an increase of the polyhedral coordination around the vanadium
atoms. The transformation is not fully reversible. The drastic change
in the polyhedral arrangement observed at the transition is indicative
of a reconstructive phase transformation. The HP phase here found
is the only modification of InVO<sub>4</sub> reported to date with
6-fold coordinated vanadium atoms. Finally, Raman frequencies and
pressure coefficients in the low- and high-pressure phases of InVO<sub>4</sub> are reported
Experimental and Theoretical Studies on α‑In<sub>2</sub>Se<sub>3</sub> at High Pressure
α(R)-In<sub>2</sub>Se<sub>3</sub> has been experimentally and theoretically studied under compression
at room temperature by means of X-ray diffraction and Raman scattering
measurements as well as by <i>ab initio</i> total-energy
and lattice-dynamics calculations. Our study has confirmed the α
(<i>R</i>3<i>m</i>) → β′ (<i>C</i>2/<i>m</i>) → β (<i>R</i>3̅<i>m</i>) sequence of pressure-induced phase transitions
and has allowed us to understand the mechanism of the monoclinic <i>C</i>2/<i>m</i> to rhombohedral <i>R</i>3̅<i>m</i> phase transition. The monoclinic <i>C</i>2/<i>m</i> phase enhances its symmetry gradually
until a complete transformation to the rhombohedral <i>R</i>3̅<i>m</i> structure is attained above 10–12
GPa. The second-order character of this transition is the reason for
the discordance in previous measurements. The comparison of Raman
measurements and lattice-dynamics calculations has allowed us to tentatively
assign most of the Raman-active modes of the three phases. The comparison
of experimental results and simulations has helped to distinguish
between the different phases of In<sub>2</sub>Se<sub>3</sub> and resolve
current controversies
Compression of Silver Sulfide: X-ray Diffraction Measurements and Total-Energy Calculations
Angle-dispersive X-ray diffraction measurements have
been performed
in acanthite, Ag<sub>2</sub>S, up to 18 GPa in order to investigate
its high-pressure structural behavior. They have been complemented
by ab initio electronic structure calculations. From our experimental
data, we have determined that two different high-pressure phase transitions
take place at 5 and 10.5 GPa. The first pressure-induced transition
is from the initial anti-PbCl<sub>2</sub>-like monoclinic structure
(space group <i>P</i>2<sub>1</sub>/<i>n</i>) to
an orthorhombic Ag<sub>2</sub>Se-type structure (space group <i>P</i>2<sub>1</sub>2<sub>1</sub>2<sub>1</sub>). The compressibility
of the lattice parameters and the equation of state of both phases
have been determined. A second phase transition to a <i>P</i>2<sub>1</sub>/<i>n</i> phase has been found, which is a
slight modification of the low-pressure structure (Co<sub>2</sub>Si-related
structure). The initial monoclinic phase was fully recovered after
decompression. Density functional and, in particular, GGA+U calculations
present an overall good agreement with the experimental results in
terms of the high-pressure sequence, cell parameters, and their evolution
with pressure