11 research outputs found
One-Step Hydrothermal Synthesis of High-Performance Gas-Sensing Crystals CdIn<sub>2</sub>O<sub>4</sub> with Octahedral Shape
Octahedrally shaped CdIn<sub>2</sub>O<sub>4</sub> was
synthesized
in a one-step hydrothermal reaction without any surfactant. These
octahedral particles used as an ethanol sensor revealed excellent
gas response, which is comparable to the well-known SnO<sub>2</sub>-based gas sensors. The octahedral CdIn<sub>2</sub>O<sub>4</sub> powder
possesses the active {111} facets, which contribute to the higher
gas-sensing performance of octahedral CdIn<sub>2</sub>O<sub>4</sub> than that of the nanosized CdIn<sub>2</sub>O<sub>4</sub> powder
obtained by coprecipitation method. The XPS results demonstrated that
the CdIn<sub>2</sub>O<sub>4</sub> octahedra enclosed by {111} facets
provided more oxygen vacancies, resulting in the enhanced performance.
The calculation also showed higher surface energies for the {111}
orientation, which confirms the mechanism of the enhanced gas-sensing
performance of the octahedral particles. The as-formed crystals with
controlled morphology provide insights for the designed strategy of
high-performance gas-sensing materials, and this synthetic route provides
flexibility and selectivity for the deliberate preparation of other
functional materials
Synthesis, Structure, and Magnetic Properties of (Tb<sub>1–<i>x</i></sub>Mn<sub><i>y</i></sub>)MnO<sub>3−δ</sub>
Two
compounds (Tb<sub>1–<i>x</i></sub>Mn<sub><i>y</i></sub>)MnO<sub>3−δ</sub> (W1, <i>x</i> = 0.089, <i>y</i> = 0.063; W2, <i>x</i> = 0.122, <i>y</i> = 0.102) have been synthesized by solid-state method and
characterized using neutron diffraction and magnetic measurements.
They crystallize in space group <i>Pnma</i> at room temperature
and <i>Pna2</i><sub>1</sub> at low temperature. W1 shows
a sinusoidal antiferromagnetic order, and W2 shows both sinusoidal
and canted commensurate antiferromagnetic orders. The magnetic moments
of the commensurate antiferromagnetic order for W2 are antiferromagnetically
coupled along the <i>a</i>- and <i>c</i>-axes,
and ferromagnetically coupled along the <i>b-</i>axis in
the <i>Pna</i>2<sub>1</sub> setting. Strong ferromagnetic
response is induced by doping more Mn into the Tb site of (Tb<sub>1–<i>x</i></sub>Mn<sub><i>y</i></sub>)MnO<sub>3−δ.</sub
Synthesis and Characterization of a Layered Silicogermanate PKU-22 and Its Topotactic Condensation to a Three-Dimensional <b>STI</b>-type Zeolite
A new
layered silicogermanate, PKU-22, was hydrothermally synthesized
under fluoride conditions using the tetraethylammonium (TEA<sup>+</sup>) cation as the structure directing agent (SDA). The crystal structure
was determined by single crystal X-ray diffraction. Structure analysis
reveals that PKU-22 is constructed by <u>sti</u> layers
stacking along the [100] direction in an ···AAAA···
manner, with TEA<sup>+</sup> cations occurring in the interlayer spaces
and F<sup>–</sup> anions residing within the layer and connecting
to Ge atoms, which also act as the charge compensation species. <i>In situ</i> temperature-variable powder X-ray diffraction results
indicated that PKU-22 could be transferred into a three-dimensional <b>STI</b>-type zeolite PKU-22a on heating. It is interesting that
the TEA<sup>+</sup> cations remain intact in the structure of the
condensed product. Solid-state NMR, inductively coupled plasma atomic
emission spectroscopy, thermogravimetric-differential scanning calorimetry,
and carbon, hydrogen, and nitrogen elemental analyses were applied
to aid the structure analysis of PKU-22 and illustrate its transformation.
The scheme of the topotactic condensation of PKU-22 to PKU-22a is
proposed
Solid-State <sup>29</sup>Si NMR and Neutron-Diffraction Studies of Sr<sub>0.7</sub>K<sub>0.3</sub>SiO<sub>2.85</sub> Oxide Ion Conductors
K/Na-doped
SrSiO<sub>3</sub>-based oxide
ion conductors were recently reported as promising candidates for
low-temperature solid-oxide fuel cells. Sr<sub>0.7</sub>K<sub>0.3</sub>SiO<sub>2.85</sub>, close to the solid-solution limit of Sr<sub>1–<i>x</i></sub>K<sub><i>x</i></sub>SiO<sub>3–0.5<i>x</i></sub>, was characterized by solid-state <sup>29</sup>Si
NMR spectroscopy and neutron powder diffraction (NPD). Differing with
the average structure containing the vacancies stabilized within the
isolated Si<sub>3</sub>O<sub>9</sub> tetrahedral rings derived from
the NPD study, the <sup>29</sup>Si NMR data provides new insight into
the local defect structure in Sr<sub>0.7</sub>K<sub>0.3</sub>SiO<sub>2.85</sub>. The Q<sup>1</sup>-linked tetrahedral Si signal in the <sup>29</sup>Si NMR data suggests that the Si<sub>3</sub>O<sub>9</sub> tetrahedral rings in the K-doped SrSiO<sub>3</sub> materials were
broken, forming Si<sub>3</sub>O<sub>8</sub> chains. The Si<sub>3</sub>O<sub>8</sub> chains can be stabilized by either bonding with the
oxygen atoms of the absorbed lattice water molecules, leading to the
Q<sup>1</sup>-linked tetrahedral Si, or sharing oxygen atoms with
neighboring Si<sub>3</sub>O<sub>9</sub> units, which is consistent
with the Q<sup>3</sup>-linked tetrahedral Si signal detected in the <sup>29</sup>Si NMR spectra
On the Structure of α‑BiFeO<sub>3</sub>
Polycrystalline and
monocrystalline α-BiFeO<sub>3</sub> crystals have been synthesized
by solid state reaction and flux growth method, respectively. X-ray,
neutron, and electron diffraction techniques are used to study the
crystallographic and magnetic structure of α-BiFeO<sub>3.</sub> The present data show that α-BiFeO<sub>3</sub> crystallizes
in space group <i>P</i>1 with <i>a</i> = 0.563 17(1)
nm, <i>b</i> = 0.563 84(1) nm, <i>c</i> = 0.563 70(1) nm, α = 59.33(1)°, β = 59.35(1)°,
γ = 59.38(1)°, and the magnetic structure of α-BiFeO<sub>3</sub> can be described by space group <i>P</i>1 with
magnetic modulation vector in reciprocal space <b>q</b> = 0.0045<b>a</b>* – 0.0045<b>b</b>*, which is the magnetic structure
model proposed by I. Sosnowska applied
to the new <i>P</i>1 crystal symmetry of α-BiFeO<sub>3</sub>
An Open-Framework Aluminophosphite with Face-Sharing AlO<sub>6</sub> Octahedra Dimers and Extra-Large 14-Ring Channels
PKU-25Al,
an open-framework aluminophosphite possessing extra-large
intersecting 14-ring (14R) channels and a novel Al/P ratio of 9/14,
was hydrothermally synthesized using commercially available 4-dimethylaminopyridine
(DMAP) as organic structure-directing agents (OSDA). Two types of
secondary building units (SBUs), SBU-1 with 6*1 units and racemic
SBU-2 composed of two chiral 41 units, are utilized to construct
the porous layers with a 4.6.12-net topology and the chains with unprecedented
face-sharing AlO<sub>6</sub> octahedra dimers, respectively. Stringing
the ABAB stacked layers via the chains would achieve the PKU-25Al
framework with a unique topology as well as numerous chiral channel
motifs. Meanwhile, the protonated DMAP molecules interact with the
inorganic framework through hydrogen bonding and reside in the voids
with an exceptional triangular pattern. PKU-25Al is the first aluminophosphite
with extra-large channels and enriches the materials chemistry of
the open-framework families with exceptive structures
Phase Transitions and Polymerization of C<sub>6</sub>H<sub>6</sub>–C<sub>6</sub>F<sub>6</sub> Cocrystal under Extreme Conditions
Pressure-induced
polymerization (PIP) of aromatic molecules can
generate saturated carbon nanostructures. As a strongly interacted
π–π stacking unit, the C<sub>6</sub>H<sub>6</sub>–C<sub>6</sub>F<sub>6</sub> adduct is widely applied in supramolecular
chemistry, and it provides a good preorganization for the PIP. Here
we investigated the structural variation of C<sub>6</sub>H<sub>6</sub>–C<sub>6</sub>F<sub>6</sub> cocrystal and the subsequent PIP
process under high pressure. Four new molecular-complex phases V,
VI, VII, and VIII have been identified and characterized by the in
situ Raman, IR, synchrotron X-ray, and neutron diffraction. The phase
V is different from the phases observed at low temperature, which
has a tilted column structure. Phases VI and VII have a structure
similar to phase V. Phase VIII polymerizes irreversibly upon compression
above 25 GPa without any catalyst, producing sp<sup>3</sup>(CH/F)<sub><i>n</i></sub> materials. The π–π interaction
is still dominant below 0.5 GPa but is most likely to be overstepped
under further compression, which is important for discussing the supramolecular
phase transition and the polymerization process
Topotactic Reduction toward a Noncentrosymmetric Deficient Perovskite Tb<sub>0.50</sub>Ca<sub>0.50</sub>Mn<sub>0.96</sub>O<sub>2.37</sub> with Ordered Mn Vacancies and Piezoelectric Behavior
Low-temperature
reduction of perovskite Tb<sub>0.5</sub>Ca<sub>0.5</sub>MnO<sub>3–<i>x</i></sub> yields novel crystal-structured
noncentrosymmetric compound Tb<sub>0.50</sub>Ca<sub>0.50</sub>Mn<sub>0.96</sub><sup>2.33+</sup>O<sub>2.37</sub>, which unusually crystallizes
in cubic lattice <i>I</i>23 (<i>a</i> ∼
15.27 Å) based on a 4<i>a</i><sub>p</sub> × 4<i>a</i><sub>p</sub> × 4<i>a</i><sub>p</sub> expansion
relative to the simple cubic perovskite unit cell. Rietveld refinements
and HAADF-STEM images are used for the structure determination, revealing
a rare-typed metal-anion coordination framework which consists of
corner-shared tetrahedra and pyramids, and edge-shared bipyramids
and octahedra. <sup>2</sup>/<sub>64</sub> B-site Mn-ordered vacancies
are observed for the first time acting as the apex and body center
of the <i>I</i> lattice in reduced systems. Room-temperature
piezoelectricity is detected, with a quasistatic <i>d</i><sub>33</sub> value of ∼0.32 pC N<sup>–1</sup> and
inverse <i>d</i><sub>33</sub> value of ∼10.5 pm V<sup>–1</sup>. This phase primarily exhibits antiferromagnetic
ordering below <i>T</i><sub>N</sub> ∼ 70 K, with
ferromagnetic responses resulted from spin-canting below 40 K. This
work provides a new way toward synthesizing unconventional acentric
materials, in the absence of second-order Jahn–Teller active
“distortion centers”
An Open-Framework Aluminophosphite with Face-Sharing AlO<sub>6</sub> Octahedra Dimers and Extra-Large 14-Ring Channels
PKU-25Al,
an open-framework aluminophosphite possessing extra-large
intersecting 14-ring (14R) channels and a novel Al/P ratio of 9/14,
was hydrothermally synthesized using commercially available 4-dimethylaminopyridine
(DMAP) as organic structure-directing agents (OSDA). Two types of
secondary building units (SBUs), SBU-1 with 6*1 units and racemic
SBU-2 composed of two chiral 41 units, are utilized to construct
the porous layers with a 4.6.12-net topology and the chains with unprecedented
face-sharing AlO<sub>6</sub> octahedra dimers, respectively. Stringing
the ABAB stacked layers via the chains would achieve the PKU-25Al
framework with a unique topology as well as numerous chiral channel
motifs. Meanwhile, the protonated DMAP molecules interact with the
inorganic framework through hydrogen bonding and reside in the voids
with an exceptional triangular pattern. PKU-25Al is the first aluminophosphite
with extra-large channels and enriches the materials chemistry of
the open-framework families with exceptive structures
On the Structure of α‑BiFeO<sub>3</sub>
Polycrystalline and
monocrystalline α-BiFeO<sub>3</sub> crystals have been synthesized
by solid state reaction and flux growth method, respectively. X-ray,
neutron, and electron diffraction techniques are used to study the
crystallographic and magnetic structure of α-BiFeO<sub>3.</sub> The present data show that α-BiFeO<sub>3</sub> crystallizes
in space group <i>P</i>1 with <i>a</i> = 0.563 17(1)
nm, <i>b</i> = 0.563 84(1) nm, <i>c</i> = 0.563 70(1) nm, α = 59.33(1)°, β = 59.35(1)°,
γ = 59.38(1)°, and the magnetic structure of α-BiFeO<sub>3</sub> can be described by space group <i>P</i>1 with
magnetic modulation vector in reciprocal space <b>q</b> = 0.0045<b>a</b>* – 0.0045<b>b</b>*, which is the magnetic structure
model proposed by I. Sosnowska applied
to the new <i>P</i>1 crystal symmetry of α-BiFeO<sub>3</sub>