11 research outputs found
Orientational disorder and phase transitions in crystals of (NH4)2NbOF5
Structural phase transitions in a crystal of (NH4)2NbOF5 are the consequence of dynamic changes in its structural units as the temperature decreases. Using X-ray diffraction, it is possible to identify O and F atoms in the disordered structure of (NH4)2NbOF5 as a result of its dynamic nature
Optical and calorimetric studies of K2TaF7
Optical and calorimetric experiments on K2TaF7 are performed in a wide temperature range. No features were
found in the behavior of the birefringence Δnb(T), the angle of rotation of the indicatrix ϕ(T) and the heat
capacity ΔCp(T) except for those associated with the Pnma↔P21/c phase transition. Structural transformation
was characterized as strong first order “proper” ferroelastic accompanied by a huge angle ϕ ≈40° and strong pretransition
phenomena in Δnb(T). Two contributions to the anomalies of the optical properties were found associated
with the photoelastic effect and the transition parameter related linearly to the spontaneous deformation.
Thermal treatments cause correlated changes in temperature and enthalpy of the phase transition,
which leads to the invariance of the large magnitude of the corresponding entropy ΔS=22 J/mol·K which does
not match the model with the absence of structural disorder in the Pnma phase
Heat capacity, thermal expansion and sensitivity to hydrostatic pressure of (NH4)3SiF7 at successive structural phase transitions
Heat capacity, thermal dilatation, permittivity and sensitivity to external pressure of (NH4)3SiF7 were studied. Due to the absence of cubic phases Pm3m and Pa3, a strong decrease in the total entropy change dSi = 19 J/molK associated
with four successive transformations P4=mbm - Pbam - P21=c11 - P1 - P121/c1 was found in silicate in comparison with other double uoride salts (NH4)3MeF7 (Me: Ge, Ti, Sn). Using analysis of the excess heat capacity in the framework of the thermodynamic theory, the entropies associated with each individual phase transition were determined. In accordance with the entropic parameters, the complete ordering of the structural elements occurs in the monoclinic phase P21=c11. Further change in symmetry is associated with small entropy changes which prove insignicant displacement of structural units.
A T-p phase diagram was constructed and good agreement was found between measured and calculated baric coefficients
Anomalous behaviour of thermodynamic properties at successive phase transitions in (NH4)3GeF7
Heat capacity, thermal dilatation, susceptibility to hydrostatic pressure and dielectric properties associated with
succession of three phase transitions below room temperature in double fluoride salt (NH4)3GeF7 were studied.
A possible transformation into the parent Pm-3m cubic phase was not observed up to the decomposition of
compound. Nonferroelectric nature of structural distortions was confirmed. The DTA under pressure studies
revealed a high temperature stability of two phases: P4/mbm and Pbam. The entropies of the phase transitions
agree well with the model of structural distortions. Analysis of the thermal properties associated with the
individual phase transitions in the framework of thermodynamic equations has shown a high reliability of the
data obtained
Bonding and Structure of Oxofluoroniobate-Based Glasses
Glasses
based on the oxofluoroniobate anion have been characterized by vibrational
and solid-state NMR spectroscopy. The mechanism of glass formation
in the systems K<sub>2</sub>NbOF<sub>5</sub>–MF<sub>3</sub> (M = Al, In) has been suggested. A glass network is built from the
chains of corner-sharing octahedra through −Nb–F(O)–M–
and −Nb–F–Nb– bridges. Isolated NbOF<sub>5</sub><sup>2–</sup> octahedra are also present, which is
consistent with the glass composition. The high ionic mobility of
NbOF<sub>5</sub><sup>2–</sup> due to its fast reorientations
results in equalization of the Nb–O and Nb–F distances,
which is reflected in the appearance of the IR band at 700–800
cm<sup>–1</sup> not observed in the Raman spectrum. Its assignment
to bridging −Nb–O–Nb– species accepted
in the literature was not proven
Thermal, structural, optical, dielectric and barocaloric properties at ferroelastic phase transition in trigonal (NH4)2SnF6: A new look at the old compound
Текст статьи не публикуется в открытом доступе в соответствии с политикой журнала.Structural phase transition P-3m1 ↔ P-1 of the first order and nonferroelectric nature was found in (NH4)2SnF6 at about 110 K in the process of thermal, optical, dielectric and X-ray studies. Order-disorder transformation is accompanied by large changes of entropy (ΔS0 = 16.4 J/mol•K) and volume (ΔV0/V ≈ 1 %). The structural model associated with three orientations of NH4 tetrahedra in P-3m1 phase and their complete ordering in P-1 phase was suggested with the entropy change (ΔS0 = 18.3 J/mol•K) close to the experimental value. A good agreement between baric coefficients measured in a direct way (dT0/dp = -157 K/GPa) and evaluated using entropy and volume changes at phase transition (- 170 K/GPa) was found. Barocaloric effects in (NH4)2SnF6 are comparable with those of known solid state refrigerants and are characterised by a low-pressure need for realising their maximum values
Thermal, structural, optical, dielectric and barocaloric properties at ferroelastic phase transition in trigonal (NH4)2SnF6: A new look at the old compound
Текст статьи не публикуется в открытом доступе в соответствии с политикой журнала.Structural phase transition P-3m1 ↔ P-1 of the first order and nonferroelectric nature was found in (NH4)2SnF6 at about 110 K in the process of thermal, optical, dielectric and X-ray studies. Order-disorder transformation is accompanied by large changes of entropy (ΔS0 = 16.4 J/mol•K) and volume (ΔV0/V ≈ 1 %). The structural model associated with three orientations of NH4 tetrahedra in P-3m1 phase and their complete ordering in P-1 phase was suggested with the entropy change (ΔS0 = 18.3 J/mol•K) close to the experimental value. A good agreement between baric coefficients measured in a direct way (dT0/dp = -157 K/GPa) and evaluated using entropy and volume changes at phase transition (- 170 K/GPa) was found. Barocaloric effects in (NH4)2SnF6 are comparable with those of known solid state refrigerants and are characterised by a low-pressure need for realising their maximum values
Synthesis, Structural, Magnetic, and Electronic Properties of Cubic CsMnMoO<sub>3</sub>F<sub>3</sub> Oxyfluoride
A powder sample of CsMnMoO<sub>3</sub>F<sub>3</sub> oxyfluoride
has been prepared by solid state synthesis. The pyrochlore-related
crystal structure of CsMnMoO<sub>3</sub>F<sub>3</sub> has been refined
by the Rietveld method at <i>T</i> = 298 K (space group <i>Fd-</i>3<i>m</i>, <i>a</i> = 10.59141(4)
Å, <i>V</i> = 1188.123(8) Å<sup>3</sup>; <i>R</i><sub>B</sub> = 3.44%). The stability of the cubic phase
has been obtained over the temperature range <i>T</i> =
110–293 K by heat capacity measurements. Magnetic properties
have been measured over the range of <i>T</i> = 2–300
K. The electronic structure of CsMnMoO<sub>3</sub>F<sub>3</sub> has
been evaluated by X-ray photoelectron spectroscopy. Chemical bonding
effects have been discussed for all metal ions using binding energy
difference parameters and wide comparison with related oxides and
fluorides. The competition between O<sup>2–</sup> and F<sup>–</sup> ions for metal valence electrons has been found