19 research outputs found
Structural Phase Transitions in a New Compound Eu<sub>2</sub>AgGe<sub>3</sub>
A new
intermetallic compound Eu<sub>2</sub>AgGe<sub>3</sub> has been synthesized
using high-frequency induction heating method. Single-crystal X-ray
diffraction data showed that Eu<sub>2</sub>AgGe<sub>3</sub> crystallizes
in the orthorhombic Ba<sub>2</sub>LiSi<sub>3</sub> structure type,
with <i>Fddd</i> space group and lattice parameters <i>a</i> = 8.7069(17) Ã…, <i>b</i> = 15.011(3) Ã…, <i>c</i> = 17.761(4) Ã…. Eu<sub>2</sub>AgGe<sub>3</sub> is
composed of infinite arrays of hexagonal [Ag<sub>3</sub>Ge<sub>3</sub>] units stacked along the [001] direction, and the Eu sites are sandwiched
between these parallel hexagonal networks. Temperature-dependent powder
XRD data and DTA hint toward a structural phase transition from orthorhombic
to hexagonal above 477 K and an unusual reversible transition to the
original phase, i.e., orthorhombic phase at around 718 K. Magnetic
measurements on Eu<sub>2</sub>AgGe<sub>3</sub> sample show paramagnetic
behavior above 100 K and weak ferromagnetic interactions below 80
K. Mössbauer spectroscopy and X-ray absorption near-edge spectroscopic
(XANES) studies reveal that Eu atoms in Eu<sub>2</sub>AgGe<sub>3</sub> exist in the divalent oxidation state
Metallic Yb<sub>2</sub>AuGe<sub>3</sub>: An Ordered Superstructure in the AlB<sub>2</sub>‑Type Family with Mixed-Valent Yb and a High-Temperature Phase Transition
The intermetallic compound Yb<sub>2</sub>AuGe<sub>3</sub> was synthesized
from indium flux. Yb<sub>2</sub>AuGe<sub>3</sub> crystallizes in the
orthorhombic Ca<sub>2</sub>AgSi<sub>3</sub>-type structure which is
an ordered superstructure of the AlB<sub>2</sub> structure type. The
structure was refined in the <i>Fmmm</i> space group with
lattice parameters <i>a</i> = 8.5124(17) Ã…, <i>b</i> = 14.730(3) Ã…, <i>c</i> = 8.4995(17) Ã….
Temperature-dependent powder X-ray diffraction studies show that Yb<sub>2</sub>AuGe<sub>3</sub> undergoes a phase transition from orthorhombic
to hexagonal upon heating above 773 K. The compound shows weak paramagnetism
that derives from a combination of Curie and Pauli paramagnetism with
a magnetic moment value of 0.33(2) μ<sub>B</sub>/Yb atom. Magnetic
ordering was not observed down to 2 K. Yb<sub>2</sub>AuGe<sub>3</sub> is metallic, and at low temperature the resistivity varies as <i>T</i><sup>2</sup>, indicating possible Fermi liquid behavior.
Heat capacity measurements suggest that Yb<sub>2</sub>AuGe<sub>3</sub> is possibly a moderate heavy fermion system
Metallic Yb<sub>2</sub>AuGe<sub>3</sub>: An Ordered Superstructure in the AlB<sub>2</sub>‑Type Family with Mixed-Valent Yb and a High-Temperature Phase Transition
The intermetallic compound Yb<sub>2</sub>AuGe<sub>3</sub> was synthesized
from indium flux. Yb<sub>2</sub>AuGe<sub>3</sub> crystallizes in the
orthorhombic Ca<sub>2</sub>AgSi<sub>3</sub>-type structure which is
an ordered superstructure of the AlB<sub>2</sub> structure type. The
structure was refined in the <i>Fmmm</i> space group with
lattice parameters <i>a</i> = 8.5124(17) Ã…, <i>b</i> = 14.730(3) Ã…, <i>c</i> = 8.4995(17) Ã….
Temperature-dependent powder X-ray diffraction studies show that Yb<sub>2</sub>AuGe<sub>3</sub> undergoes a phase transition from orthorhombic
to hexagonal upon heating above 773 K. The compound shows weak paramagnetism
that derives from a combination of Curie and Pauli paramagnetism with
a magnetic moment value of 0.33(2) μ<sub>B</sub>/Yb atom. Magnetic
ordering was not observed down to 2 K. Yb<sub>2</sub>AuGe<sub>3</sub> is metallic, and at low temperature the resistivity varies as <i>T</i><sup>2</sup>, indicating possible Fermi liquid behavior.
Heat capacity measurements suggest that Yb<sub>2</sub>AuGe<sub>3</sub> is possibly a moderate heavy fermion system
Crystal Structure and Magnetic Properties of Indium Flux Grown EuAu<sub>2</sub>In<sub>4</sub> and EuAuIn<sub>4</sub>
Two new intermetallic compounds EuAuIn<sub>4</sub> and EuAu<sub>2</sub>In<sub>4</sub> having plate- and rodlike
shapes, respectively,
were synthesized using indium as an active metal flux. Both compounds
crystallize in the orthorhombic system and can be classified as polyindide
systems due to the presence of [In<sub>4</sub>] tetrameric units.
EuAuIn<sub>4</sub> adopts the YNiAl<sub>4</sub> structure type with <i>Cmcm</i> space group and lattice parameters <i>a</i> = 4.6080(3) Ã…, <i>b</i> = 17.0454(8) Ã…, <i>c</i> = 7.5462(4). EuAu<sub>2</sub>In<sub>4</sub> crystallizes
in the NdRh<sub>2</sub>Sn<sub>4</sub> structure type with <i>Pnma</i> space group and lattice parameters <i>a</i> = 18.5987(7) Ã…, <i>b</i> = 4.6616(2) Ã…, and <i>c</i> = 7.4669(3) Ã…. EuAuIn<sub>4</sub> consists of three-dimensional
[AuIn<sub>4</sub>] units, and the europium atoms reside in the distorted
hexagonal channels, whereas, in EuAu<sub>2</sub>In<sub>4</sub>, the
europium atoms are enclosed by three-dimensional cages of [Au<sub>2</sub>In<sub>4</sub>] polyanionic units. Magnetic susceptibility
measurements showed Curie–Weiss behavior within the temperature
range of 80–300 K for EuAu<sub>2</sub>In<sub>4</sub> and 10–300
K for EuAu<sub>2</sub>In<sub>4</sub> with an effective magnetic moment
(μ<sub>eff</sub>) of 5.88 and 7.76 μ<sub>B</sub>/Eu atom,
respectively. The negative Curie–Weiss paramagnetic temperature
in both compounds suggests antiferromagnetic interactions
Facile Aqueous-Phase Synthesis of the PtAu/Bi<sub>2</sub>O<sub>3</sub> Hybrid Catalyst for Efficient Electro-Oxidation of Ethanol
In
this work, we present a facile aqueous-phase synthesis of a hybrid
catalyst consisting of PtAu alloy supported on Bi<sub>2</sub>O<sub>3</sub> microspheres. Multistep reduction of HAuCl<sub>4</sub> and
K<sub>2</sub>PtCl<sub>4</sub> salts on Bi<sub>2</sub>O<sub>3</sub> and subsequent annealing lead to the formation of this hybrid catalyst.
To the best of our knowledge, this is the first report of using Bi<sub>2</sub>O<sub>3</sub> as a catalyst support in fuel cell applications.
The material was characterized by powder X-ray diffraction and various
microscopic techniques. This composite showed remarkable activity
as well as stability toward the electro-oxidation of ethanol in comparison
to commercially available Pt/C. The order of the reactivity was found
to be commercial Pt/C (50.4 mA/m<sup>2</sup>mg<sub>Pt</sub><sup>–1</sup>) < Pt/Bi<sub>2</sub>O<sub>3</sub>(10) (108 mA/m<sup>2</sup>mg<sub>Pt</sub><sup>–1</sup>) < PtAu/Bi<sub>2</sub>O<sub>3</sub>(10) (459 mA/m<sup>2</sup>mg<sub>Pt</sub><sup>–1</sup>). The
enhancement in the activity can be explained through cooperative effects,
namely, ligand effects of gold and Bi<sub>2</sub>O<sub>3</sub> support,
which helps in removing carbon monoxide molecules to avoid the poisoning
of the Pt active sites
Yb<sub>5</sub>Ga<sub>2</sub>Sb<sub>6</sub>: A Mixed Valent and Narrow-Band Gap Material in the RE<sub>5</sub>M<sub>2</sub>X<sub>6</sub> Family
A new
compound Yb<sub>5</sub>Ga<sub>2</sub>Sb<sub>6</sub> was synthesized
by the metal flux technique as well as high frequency induction heating.
Yb<sub>5</sub>Ga<sub>2</sub>Sb<sub>6</sub> crystallizes in the orthorhombic
space group <i>Pbam</i> (no. 55), in the Ba<sub>5</sub>Al<sub>2</sub>Bi<sub>6</sub> structure type, with a unit cell of <i>a</i> = 7.2769(2) Ã…, <i>b</i> = 22.9102(5) Ã…, <i>c</i> = 4.3984(14) Ã…, and <i>Z</i> = 2. Yb<sub>5</sub>Ga<sub>2</sub>Sb<sub>6</sub> has an anisotropic structure
with infinite anionic double chains (Ga<sub>2</sub>Sb<sub>6</sub>)<sup>10–</sup> cross-linked by Yb<sup>2+</sup> and Yb<sup>3+</sup> ions. Each single chain is made of corner-sharing GaSb<sub>4</sub> tetrahedra. Two such chains are bridged by Sb<sub>2</sub> groups
to form double chains of 1/∞ [Ga<sub>2</sub>Sb<sub>6</sub><sup>10–</sup>]. The compound satisfies the classical Zintl–Klemm
concept and is a narrow band gap semiconductor with an energy gap
of around 0.36 eV calculated from the electrical resistivity data
corroborating with the experimental absorption studies in the IR region
(0.3 eV). Magnetic measurements suggest Yb atoms in Yb<sub>5</sub>Ga<sub>2</sub>Sb<sub>6</sub> exist in the mixed valent state. Temperature
dependent magnetic susceptibility data follows the Curie–Weiss
behavior above 100 K and no magnetic ordering was observed down to
2 K. Experiments are accompanied by all electron full-potential linear
augmented plane wave (FP-LAPW) calculations based on density functional
theory to calculate the electronic structure and density of states.
The calculated band structure shows a weak overlap of valence band
and conduction band resulting in a pseudo gap in the density of states
revealing semimetallic character
Crystal Structure and Band Gap Engineering in Polyoxometalate-Based Inorganic–Organic Hybrids
We have demonstrated engineering
of the electronic band gap of the hybrid materials based on POMs (polyoxometalates),
by controlling its structural complexity through variation in the
conditions of synthesis. The pH- and temperature-dependent studies
give a clear insight into how these experimental factors affect the
overall hybrid structure and its properties. Our structural manipulations
have been successful in effectively tuning the optical band gap and
electronic band structure of this kind of hybrids, which can find
many applications in the field of photovoltaic and semiconducting
devices. We have also addressed a common crystallographic disorder
observed in Keggin-ion (one type of heteropolyoxometalate [POMs])-based
hybrid materials. Through a combination of crystallographic, spectroscopic,
and theoretical analysis of four new POM-based hybrids synthesized
with tactically varied reaction conditions, we trace the origin and
nature of the disorder associated with it and the subtle local structural
coordination involved in its core picture. While the crystallography
yields a centrosymmetric structure with planar coordination of Si,
our analysis with XPS, IR, and Raman spectroscopy reveals a tetrahedral
coordination with broken inversion symmetry, corroborated by first-principles
calculations
Crystal Structure and Band Gap Engineering in Polyoxometalate-Based Inorganic–Organic Hybrids
We have demonstrated engineering
of the electronic band gap of the hybrid materials based on POMs (polyoxometalates),
by controlling its structural complexity through variation in the
conditions of synthesis. The pH- and temperature-dependent studies
give a clear insight into how these experimental factors affect the
overall hybrid structure and its properties. Our structural manipulations
have been successful in effectively tuning the optical band gap and
electronic band structure of this kind of hybrids, which can find
many applications in the field of photovoltaic and semiconducting
devices. We have also addressed a common crystallographic disorder
observed in Keggin-ion (one type of heteropolyoxometalate [POMs])-based
hybrid materials. Through a combination of crystallographic, spectroscopic,
and theoretical analysis of four new POM-based hybrids synthesized
with tactically varied reaction conditions, we trace the origin and
nature of the disorder associated with it and the subtle local structural
coordination involved in its core picture. While the crystallography
yields a centrosymmetric structure with planar coordination of Si,
our analysis with XPS, IR, and Raman spectroscopy reveals a tetrahedral
coordination with broken inversion symmetry, corroborated by first-principles
calculations
Crystal Structure and Band Gap Engineering in Polyoxometalate-Based Inorganic–Organic Hybrids
We have demonstrated engineering
of the electronic band gap of the hybrid materials based on POMs (polyoxometalates),
by controlling its structural complexity through variation in the
conditions of synthesis. The pH- and temperature-dependent studies
give a clear insight into how these experimental factors affect the
overall hybrid structure and its properties. Our structural manipulations
have been successful in effectively tuning the optical band gap and
electronic band structure of this kind of hybrids, which can find
many applications in the field of photovoltaic and semiconducting
devices. We have also addressed a common crystallographic disorder
observed in Keggin-ion (one type of heteropolyoxometalate [POMs])-based
hybrid materials. Through a combination of crystallographic, spectroscopic,
and theoretical analysis of four new POM-based hybrids synthesized
with tactically varied reaction conditions, we trace the origin and
nature of the disorder associated with it and the subtle local structural
coordination involved in its core picture. While the crystallography
yields a centrosymmetric structure with planar coordination of Si,
our analysis with XPS, IR, and Raman spectroscopy reveals a tetrahedral
coordination with broken inversion symmetry, corroborated by first-principles
calculations
Crystal Structure and Band Gap Engineering in Polyoxometalate-Based Inorganic–Organic Hybrids
We have demonstrated engineering
of the electronic band gap of the hybrid materials based on POMs (polyoxometalates),
by controlling its structural complexity through variation in the
conditions of synthesis. The pH- and temperature-dependent studies
give a clear insight into how these experimental factors affect the
overall hybrid structure and its properties. Our structural manipulations
have been successful in effectively tuning the optical band gap and
electronic band structure of this kind of hybrids, which can find
many applications in the field of photovoltaic and semiconducting
devices. We have also addressed a common crystallographic disorder
observed in Keggin-ion (one type of heteropolyoxometalate [POMs])-based
hybrid materials. Through a combination of crystallographic, spectroscopic,
and theoretical analysis of four new POM-based hybrids synthesized
with tactically varied reaction conditions, we trace the origin and
nature of the disorder associated with it and the subtle local structural
coordination involved in its core picture. While the crystallography
yields a centrosymmetric structure with planar coordination of Si,
our analysis with XPS, IR, and Raman spectroscopy reveals a tetrahedral
coordination with broken inversion symmetry, corroborated by first-principles
calculations