10 research outputs found
Reversible Thermosalient Effect of <i>N</i>′‑2-Propylidene-4-hydroxybenzohydrazide Accompanied by an Immense Negative Compressibility: Structural and Theoretical Arguments Aiming toward the Elucidation of Jumping Phenomenon
The
temperature-induced reversible phase transition of <i>N</i>′-2-propylidene-4-hydroxybenzohydrazide
from the polymorphic Form II to Form III, and <i>vice versa</i>, is accompanied by the dramatic change of the macroscopic dimensions
of the crystal which resulted in the pronounced mechanical motion
(jumping) during the phase transition. Prior to the phase transition,
the extremely large uniaxial negative thermal expansion along one
crystal axis (<i>b</i> axis<i>)</i> was observed,
together with the positive thermal expansions along the other two
crystal axes. Form III of <i>N</i>′-2-propylidene-4-hydroxybenzohydrazide
exhibits the thermal expansion α<sub><i>c</i></sub> = 360 × 10<sup>–6</sup> K<sup>–1</sup>, which
is the largest value ever noticed in any organic or metal–organic
crystal. From the structural point of view, a thermosalient effect
is escorted by the springlike behavior of the <i>zig-zag</i> molecular assemblies along the <i>c</i> axis. First-principles
electronic structure calculations show that negative thermal expansion
arises from the elastic properties of the crystal which show uniaxial
negative compressibilities, NLC. Form III exhibits the negative compressibility
along the 001 direction β<sub>3</sub> = −28 TPa<sup>–1</sup>, which is 1 order of magnitude larger than that of any organic compound
and, in fact, is comparable to compressibilities of molecular frameworks
showing the most pronounced NLC behavior. Elastic properties are also
the reason for the reversibility of Form II to Form III transition
in contrast to the irreversible Form I to Form II transition. Low
energy springlike phonons are easily thermally excited and can assist
in the overcoming of the energy barrier between the two phases that
precedes thermosalient transition
Reversible Thermosalient Effect of <i>N</i>′‑2-Propylidene-4-hydroxybenzohydrazide Accompanied by an Immense Negative Compressibility: Structural and Theoretical Arguments Aiming toward the Elucidation of Jumping Phenomenon
The
temperature-induced reversible phase transition of <i>N</i>′-2-propylidene-4-hydroxybenzohydrazide
from the polymorphic Form II to Form III, and <i>vice versa</i>, is accompanied by the dramatic change of the macroscopic dimensions
of the crystal which resulted in the pronounced mechanical motion
(jumping) during the phase transition. Prior to the phase transition,
the extremely large uniaxial negative thermal expansion along one
crystal axis (<i>b</i> axis<i>)</i> was observed,
together with the positive thermal expansions along the other two
crystal axes. Form III of <i>N</i>′-2-propylidene-4-hydroxybenzohydrazide
exhibits the thermal expansion α<sub><i>c</i></sub> = 360 × 10<sup>–6</sup> K<sup>–1</sup>, which
is the largest value ever noticed in any organic or metal–organic
crystal. From the structural point of view, a thermosalient effect
is escorted by the springlike behavior of the <i>zig-zag</i> molecular assemblies along the <i>c</i> axis. First-principles
electronic structure calculations show that negative thermal expansion
arises from the elastic properties of the crystal which show uniaxial
negative compressibilities, NLC. Form III exhibits the negative compressibility
along the 001 direction β<sub>3</sub> = −28 TPa<sup>–1</sup>, which is 1 order of magnitude larger than that of any organic compound
and, in fact, is comparable to compressibilities of molecular frameworks
showing the most pronounced NLC behavior. Elastic properties are also
the reason for the reversibility of Form II to Form III transition
in contrast to the irreversible Form I to Form II transition. Low
energy springlike phonons are easily thermally excited and can assist
in the overcoming of the energy barrier between the two phases that
precedes thermosalient transition
A 3D Oxalate-Based Network as a Precursor for the CoMn<sub>2</sub>O<sub>4</sub> Spinel: Synthesis and Structural and Magnetic Studies
A novel heterometallic oxalate-based
compound of the formula {[Co(bpy)<sub>3</sub>][Mn<sub>2</sub>(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub>]·H<sub>2</sub>O}<sub><i>n</i></sub> (<b>1</b>; bpy = 2,2′-bipyridine) was
synthesized and characterized by elemental analysis, IR spectroscopy,
single-crystal X-ray diffraction (XRD), and magnetization measurement.
The molecular structure of <b>1</b> is made of a three-dimensional
(3D) anionic network, [Mn<sub>2</sub>(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub>]<sub><i>n</i></sub><sup>2<i>n</i>–</sup>, and tris-chelated cations [Co(bpy)<sub>3</sub>]<sup>2+</sup> occupying
the vacancies of the framework. Splitting between the zero-field-cooled
(ZFC) and field-cooled (FC) branches of susceptibility below the small
peak at 13 K indicates magnetic ordering. Compound <b>1</b> was
used as a single-source precursor for the formation of the mixed-metal
oxide CoMn<sub>2</sub>O<sub>4</sub>. This conversion via thermal decomposition
was explored by thermal analysis (TGA and DTA), IR spectroscopy, powder
XRD, and magnetic susceptibility measurement. From refined structural
parameters, it could be seen that the spinel obtained by the thermal
treatment of <b>1</b> at 800 °C is characterized by the
inversion parameter δ = 21%, and therefore the structural formula
at room temperature can be written as <sup>tet</sup>[Co<sub>0.79</sub>Mn<sub>0.21</sub>]<sup>oct</sup>[Co<sub>0.105</sub>Mn<sub>0.895</sub>]<sub>2</sub>O<sub>4</sub>. The temperature dependence of magnetization
for CoMn<sub>2</sub>O<sub>4</sub> points to at least three magnetic
phases: the ferrimagnetic state is observed below 83 K, and up to
180 K blocking of the magnetic moments of nanocrystallites of 31 nm
appears, transforming to paramagnetic-like behavior above 180 K. Microstructural
characterization of the CoMn<sub>2</sub>O<sub>4</sub> sample was carried
out by means of XRD line-broadening analysis
Single-Step Preparation of the Mixed Ba<sup>II</sup>–Nb<sup>V</sup> Oxides from a Heteropolynuclear Oxalate Complex
A novel oxalate-based complex of the formula {Ba<sub>2</sub>(H<sub>2</sub>O)<sub>5</sub>[NbO(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub>]HC<sub>2</sub>O<sub>4</sub>}·H<sub>2</sub>O (<b>1</b>) was prepared from an aqueous solution containing the [NbO(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub>]<sup>3–</sup> and Ba<sup>2+</sup> entities in the molar ratio 1:2, and characterized by X-ray
single-crystal diffraction, IR spectroscopy, and thermal analysis.
The crystal packing of <b>1</b> reveals a complex three-dimensional
(3D) network: the Nb polyhedron is connected to eight neighboring
Ba polyhedra through the oxalate ligands and the oxo-oxygen group,
whereas the Ba polyhedra share edges and vertices. The ability of
compound <b>1</b> to act as a single-source precursor for the
formation of bimetallic oxides was investigated by the thermal analysis
(TGA and DSC) and X-ray powder diffraction. Thermal processing of <b>1</b> resulted in the formation of mixed-metal oxide phases, Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> and Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub>. Three stable polymorphs of Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> were isolated: the known, hexagonal <i>α-</i> and orthorhombic γ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub>, and another one, not previously reported, hexagonal δ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> polymorph. The new, δ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> polymorph has the 6H-perovskite
structure (space group <i>P</i>6<sub>3</sub>/<i>m</i>), in which the Nb<sub>2</sub>O<sub>9</sub><sup>8–</sup> face-sharing
octahedral dimers are interconnected via corners to the regular BaO<sub>6</sub><sup>10–</sup> octahedra. Formation of the mixed-metal
oxides takes place at different temperatures: the Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> oxide occurred at ∼700 °C, as the
major crystalline oxide phase; by heating the sample up to 1135 °C,
the α-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> form was obtained,
whereas the heating at 1175 °C caused the crystallization of
two polymorphs, γ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> and
δ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub>. Special focus was
set on the electrical properties of the prepared mixed Ba<sup>II</sup>–Nb<sup>V</sup> oxides obtained by this molecular pathway
in a single-step preparation
Single-Step Preparation of the Mixed Ba<sup>II</sup>–Nb<sup>V</sup> Oxides from a Heteropolynuclear Oxalate Complex
A novel oxalate-based complex of the formula {Ba<sub>2</sub>(H<sub>2</sub>O)<sub>5</sub>[NbO(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub>]HC<sub>2</sub>O<sub>4</sub>}·H<sub>2</sub>O (<b>1</b>) was prepared from an aqueous solution containing the [NbO(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub>]<sup>3–</sup> and Ba<sup>2+</sup> entities in the molar ratio 1:2, and characterized by X-ray
single-crystal diffraction, IR spectroscopy, and thermal analysis.
The crystal packing of <b>1</b> reveals a complex three-dimensional
(3D) network: the Nb polyhedron is connected to eight neighboring
Ba polyhedra through the oxalate ligands and the oxo-oxygen group,
whereas the Ba polyhedra share edges and vertices. The ability of
compound <b>1</b> to act as a single-source precursor for the
formation of bimetallic oxides was investigated by the thermal analysis
(TGA and DSC) and X-ray powder diffraction. Thermal processing of <b>1</b> resulted in the formation of mixed-metal oxide phases, Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> and Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub>. Three stable polymorphs of Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> were isolated: the known, hexagonal <i>α-</i> and orthorhombic γ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub>, and another one, not previously reported, hexagonal δ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> polymorph. The new, δ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> polymorph has the 6H-perovskite
structure (space group <i>P</i>6<sub>3</sub>/<i>m</i>), in which the Nb<sub>2</sub>O<sub>9</sub><sup>8–</sup> face-sharing
octahedral dimers are interconnected via corners to the regular BaO<sub>6</sub><sup>10–</sup> octahedra. Formation of the mixed-metal
oxides takes place at different temperatures: the Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> oxide occurred at ∼700 °C, as the
major crystalline oxide phase; by heating the sample up to 1135 °C,
the α-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> form was obtained,
whereas the heating at 1175 °C caused the crystallization of
two polymorphs, γ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub> and
δ-Ba<sub>4</sub>Nb<sub>2</sub>O<sub>9</sub>. Special focus was
set on the electrical properties of the prepared mixed Ba<sup>II</sup>–Nb<sup>V</sup> oxides obtained by this molecular pathway
in a single-step preparation
Photoinduced Segregation Behavior in 2D Mixed Halide Perovskite: Effects of Light and Heat
Photoinduced halide segregation (PHS)
is a process of critical
importance for the performance of perovskite solar cells with mixed
halide absorber layers. However, PHS is still not well understood,
especially in the case of layered mixed halide perovskites (MHPs),
which are less commonly studied compared to their 3D counterparts.
Here, we investigated temperature- and light-induced PHS in 2D MHPs
with a phenylpropylammonium (PPA) spacer. We found that 2D PPA-based
MHPs exhibited complex segregation behavior dependence on temperature
and illumination intensity with the suppression of segregation observed
at high temperature (attributed to the highly exothermic nature of
the process) as well as moderate illumination intensities, illustrating
the importance of additional processes present in this particular
material, which exhibits distinctly different behavior compared to
2D MHPs with other aromatic cations
Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> Oxide Prepared from an Oxalate-Based Molecular PrecursorCharacterization and Properties
A novel
heterometallic oxalate-based compound, {Ba<sub>2</sub>(H<sub>2</sub>O)<sub>5</sub>[TaO(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub>]HC<sub>2</sub>O<sub>4</sub>}·H<sub>2</sub>O (<b>1</b>), was obtained
by using an (oxalato)tantalate(V) aqueous solution as a source of
the complex anion and characterized by X-ray single-crystal diffraction,
IR spectroscopy, and thermal analysis. Compound <b>1</b> is
a three-dimensional (3D) coordination polymer with the Ta atom connected
to eight neighboring Ba atoms through the oxalate ligands and the
oxo oxygen group. Thermal treatment of <b>1</b> up to 1200 °C
leads to molecular precursor-to-material conversion that yields the
mixed-metal γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> phase.
This high-temperature γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> polymorph has the 6<i>H</i>-perovskite structure (space
group <i>P</i>6<sub>3</sub>/<i>m</i>), in which
the Ta<sub>2</sub>O<sub>9</sub> face-sharing octahedral dimers are
interconnected via corners to the regular BaO<sub>6</sub> octahedra.
To date, γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> has never
been obtained at room temperature, because of the reduction of symmetry
(<i>P</i>6<sub>3</sub>/<i>m</i> → <i>P</i>2<sub>1</sub>/<i>c</i>) that usually occurs during
the cooling. Spectroscopic, optical, photocatalytic, and electrical
properties of the obtained γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> phase were investigated. In addition to the experimental
data, an absorption spectrum and band structure of the γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> polymorph were calculated using
density functional theory
Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> Oxide Prepared from an Oxalate-Based Molecular PrecursorCharacterization and Properties
A novel
heterometallic oxalate-based compound, {Ba<sub>2</sub>(H<sub>2</sub>O)<sub>5</sub>[TaO(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub>]HC<sub>2</sub>O<sub>4</sub>}·H<sub>2</sub>O (<b>1</b>), was obtained
by using an (oxalato)tantalate(V) aqueous solution as a source of
the complex anion and characterized by X-ray single-crystal diffraction,
IR spectroscopy, and thermal analysis. Compound <b>1</b> is
a three-dimensional (3D) coordination polymer with the Ta atom connected
to eight neighboring Ba atoms through the oxalate ligands and the
oxo oxygen group. Thermal treatment of <b>1</b> up to 1200 °C
leads to molecular precursor-to-material conversion that yields the
mixed-metal γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> phase.
This high-temperature γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> polymorph has the 6<i>H</i>-perovskite structure (space
group <i>P</i>6<sub>3</sub>/<i>m</i>), in which
the Ta<sub>2</sub>O<sub>9</sub> face-sharing octahedral dimers are
interconnected via corners to the regular BaO<sub>6</sub> octahedra.
To date, γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> has never
been obtained at room temperature, because of the reduction of symmetry
(<i>P</i>6<sub>3</sub>/<i>m</i> → <i>P</i>2<sub>1</sub>/<i>c</i>) that usually occurs during
the cooling. Spectroscopic, optical, photocatalytic, and electrical
properties of the obtained γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> phase were investigated. In addition to the experimental
data, an absorption spectrum and band structure of the γ-Ba<sub>4</sub>Ta<sub>2</sub>O<sub>9</sub> polymorph were calculated using
density functional theory
Aqueous Sol–Gel Route toward Selected Quaternary Metal Oxides with Single and Double Perovskite-Type Structure Containing Tellurium
Highly crystalline SrFe<sub>2/3</sub>Te<sub>1/3</sub>O<sub>3</sub>, Ba<sub>3</sub>Fe<sub>2</sub>TeO<sub>9</sub>, and Ba<sub>2</sub>NiTeO<sub>6</sub> have been synthesized
by using a specially developed
sol–gel route methodology, reducing the time needed employing
solid-state routes and resulting in high reaction yield up to 75%.
These materials have been studied by X-ray powder diffraction (XRPD),
scanning and transmission electron microscopy, Raman spectroscopy,
and dielectric and magnetic measurements. At room temperature, the
crystal structure of SrFe<sub>2/3</sub>Te<sub>1/3</sub>O<sub>3</sub> is cubic, space group <i>Pm</i>3̅<i>m</i>, with <i>a</i> = 3.9373(2) Å, whereas Ba<sub>3</sub>Fe<sub>2</sub>TeO<sub>9</sub> crystallizes in the hexagonal crystal
system, space group <i>P</i>6<sub>3</sub>/<i>mmc</i>, <i>a</i> = 5.7691(4) Å, and <i>c</i> =
14.208(1) Å. The third studied perovskite Ba<sub>2</sub>NiTeO<sub>6</sub> crystallizes in the trigonal <i>R</i>3̅<i>m</i> space group with <i>a</i> = 5.7974(4) Å
and <i>c</i> = 28.599(2) Å. Based on structural characterization
results, the obtained single and double perovskite crystallites are
nearly in nanometer regime, ranging from 45 to 164 nm, building micrometer-sized
particles with visible well-faceted hexagonal morphology. Magnetic
measurements show the onset of ferrimagnetic ordering at relatively
high temperature of 667 K for the SrFe<sub>2/3</sub>Te<sub>1/3</sub>O<sub>3</sub>, whereas Ba<sub>3</sub>Fe<sub>2</sub>TeO<sub>9</sub> and Ba<sub>2</sub>NiTeO<sub>6</sub> show antiferromagnetic ordering
below 80 and 8.6 K, respectively. The measured room temperature dielectric
constants are in the range between 15 and 77
Synthesis of Lead-Free Perovskite Films by Combinatorial Evaporation: Fast Processes for Screening Different Precursor Combinations
We
demonstrate an evaporation-based combinatorial approach for
fast screening of precursor combinations for the synthesis of novel
perovskite materials. Nine material combinations can be explored simultaneously,
which enabled us to synthesize nine different lead-free perovskite
compounds. The structural properties (morphology, crystal structure)
and optical properties (UV–vis absorption spectra, photoluminescence)
of the prepared materials were investigated. Among these materials,
several Sn-based and Pd-based perovskites exhibit strong absorption
in the visible spectral range and thus may be of interest for photovoltaic
applications. In addition, butyl ammonium tin iodide exhibits bright
red emission, and it is of interest for potential light emitting applications