24 research outputs found
A Series of Ca(II) or Ba(II) Inorganic–Organic Hybrid Frameworks Based on Aromatic Polycarboxylate Ligands with the Inorganic M–O–M (M = Ca, Ba) Connectivity from 1D to 3D
Solvothermal reactions of CaÂ(NO<sub>3</sub>)<sub>2</sub> or BaÂ(NO<sub>3</sub>)<sub>2</sub> with aromatic carboxylate ligands
afforded four
new inorganic–organic hybrid frameworks, [CaÂ(PBDC)Â(H<sub>2</sub>O)<sub>3</sub>]<sub><i>n</i></sub> (<b>1</b>), [CaÂ(OBDC)Â(H<sub>2</sub>O)]<sub><i>n</i></sub> (<b>2</b>), [Ba<sub>5</sub>(OBDC)<sub>4</sub>(H<sub>2</sub>O)<sub>2</sub>(NO<sub>3</sub>)<sub>2</sub>]<sub><i>n</i></sub> (<b>3</b>), and
[Ba<sub>3</sub>(BTC)<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub>]<sub><i>n</i></sub> (<b>4</b>) (H<sub>2</sub>PBDC = terephthalic
acid, H<sub>2</sub>OBDC = phthalic acid, H<sub>3</sub>BTC = 1,3,5-benzenetricarboxylic
acid). These compounds have been fully characterized by single crystal
X-ray diffraction, powder X-ray diffraction, satisfactory elemental
analysis, IR spectra, and TG analysis. X-ray analysis shows that compound <b>1</b> features a one-dimensional chain (1D) structure with the
I<sup>1</sup>O<sup>0</sup> connectivity, both compound <b>2</b> and compound <b>3</b> feature a two-dimensional (2D) layer
structure with the I<sup>1</sup>O<sup>1</sup> connectivity, I<sup>2</sup>O<sup>0</sup> connectivity, respectively, compound <b>4</b> features a three-dimensional (3D) framework with a rare I<sup>3</sup>O<sup>0</sup> connectivity. Thermal stabilities and luminescent properties
of compounds <b>1</b>–<b>4</b> and NLO property
of compound <b>4</b> have also been investigated
Large Mid-IR Second-Order Nonlinear-Optical Effects Designed by the Supramolecular Assembly of Different Bond Types without IR Absorption
Two
new different-bond-type hybrid compounds, (Hg<sub>6</sub>P<sub>4</sub>Cl<sub>3</sub>)Â(PbCl<sub>3</sub>) (<b>1</b>) and (Hg<sub>23</sub>P<sub>12</sub>)Â(ZnCl<sub>4</sub>)<sub>6</sub> (<b>2</b>), with
supramolecular interactions between host and guest moieties, which
based on metal–pnicogen, pnicogen–pnicogen, and metal–halogen
bonds were obtained by solid-state reactions. Compounds <b>1</b> and <b>2</b> show large second-harmonic-generation (SHG) activity
and are transparent in the wide mid-IR region, providing an effective
route for searching new IR nonlinear-optical material systems by combining
two or more different bond types with no IR absorption within a single
compound through supramolecular assembly. Theory predications based
on first-principles calculations are also performed on the SHG properties
of <b>1</b> and <b>2</b>
Large Mid-IR Second-Order Nonlinear-Optical Effects Designed by the Supramolecular Assembly of Different Bond Types without IR Absorption
Two
new different-bond-type hybrid compounds, (Hg<sub>6</sub>P<sub>4</sub>Cl<sub>3</sub>)Â(PbCl<sub>3</sub>) (<b>1</b>) and (Hg<sub>23</sub>P<sub>12</sub>)Â(ZnCl<sub>4</sub>)<sub>6</sub> (<b>2</b>), with
supramolecular interactions between host and guest moieties, which
based on metal–pnicogen, pnicogen–pnicogen, and metal–halogen
bonds were obtained by solid-state reactions. Compounds <b>1</b> and <b>2</b> show large second-harmonic-generation (SHG) activity
and are transparent in the wide mid-IR region, providing an effective
route for searching new IR nonlinear-optical material systems by combining
two or more different bond types with no IR absorption within a single
compound through supramolecular assembly. Theory predications based
on first-principles calculations are also performed on the SHG properties
of <b>1</b> and <b>2</b>
A Highly Stable 3D Acentric Zinc Metal–Organic Framework Based on Two Symmetrical Flexible Ligands: High Second-Harmonic-Generation Efficiency and Tunable Photoluminescence
A 3D
metal–organic framework (MOF), [ZnÂ(BPHY)Â(SA)]<sub><i>n</i></sub> (<b>1</b>; BPHY = 1,2-bisÂ(4-pyridyl)Âhydrazine, H<sub>2</sub>SA = succinic acid), which crystallizes in a noncentrosysmmetric
space group (<i>Cc</i>), has been solvothermally obtained
and testified to be a good nonlinear-optical material with the largest
second-harmonic-generation response among the known MOFs based on
sysmmetric ligands and high stability. Ultraviolet-to-visible tunable
emission for <b>1</b> is observed
Design and Syntheses of Electron-Transfer Photochromic Metal–Organic Complexes Using Nonphotochromic Ligands: A Model Compound and the Roles of Its Ligands
The model compound [ZnÂ(HCOO)<sub>2</sub>(4,4′-bipy)] (<b>1</b>; 4,4′-bipy = 4,4′-bipyridine)
is selected in this work to demonstrate the effectiveness of our previously
proposed design strategy for electron-transfer photochromic metal–organic
complexes. The electron-transfer photochromic behavior of <b>1</b> has been discovered for the first time. Experimental and theoretical
data illustrate that the photochromism of <b>1</b> can be attributed
to the electron transfer from formato to 4,4′-bipy and the
formation of a radical photoproduct. The electron transfer prefers
to occur between formato and 4,4′-bipy, which are combined
directly by the ZnÂ(II) atoms. A high-contrast (up to 8.3 times) photoluminescence
switch occurs during the photochromic process. The similarity of photochromic
behaviors among <b>1</b> and its analogues as well as viologen
compounds has also been found. Photochromic studies of this model
compound indicate that new electron-transfer photochromic metal–organic
complexes can be largely designed and synthesized by the rational
assembly of nonphotochromic electron-donating and electron-accepting
ligands
Novel p‑Type Conductive Semiconductor Nanocrystalline Film as the Back Electrode for High-Performance Thin Film Solar Cells
Thin
film solar cells, due to the low cost, high efficiency, long-term
stability, and consumer applications, have been widely applied for
harvesting green energy. All of these thin film solar cells generally
adopt various metal thin films as the back electrode, like Mo, Au,
Ni, Ag, Al, graphite, and so forth. When they contact with p-type
layer, it always produces a Schottky contact with a high contact potential
barrier, which greatly affects the cell performance. In this work,
we report for the first time to find an appropriate p-type conductive
semiconductor film, digenite Cu<sub>9</sub>S<sub>5</sub> nanocrystalline
film, as the back electrode for CdTe solar cells as the model device.
Its low sheet resistance (16.6 Ω/sq) could compare to that of
the commercial TCO films (6–30 Ω/sq), like FTO, ITO,
and AZO. Different from the traditonal metal back electrode, it produces
a successive gradient-doping region by the controllable Cu diffusion,
which greatly reduces the contact potential barrier. Remarkably, it
achieved a comparable power conversion efficiency (PCE, 11.3%) with
the traditional metal back electrode (Cu/Au thin films, 11.4%) in
CdTe cells and a higher PCE (13.8%) with the help of the Au assistant
film. We believe it could also act as the back electrode for other
thin film solar cells (α-Si, CuInS<sub>2</sub>, CIGSe, CZTS,
etc.), for their performance improvement
Syntheses, Structures, and Nonlinear Optical Properties of Two Sulfides Na<sub>2</sub>In<sub>2</sub>MS<sub>6</sub> (M = Si, Ge)
The first two new Na-containing sulfides
Na<sub>2</sub>In<sub>2</sub>MS<sub>6</sub> (M = Si (<b>1</b>), Ge (<b>2</b>)) in
the Na<sub>2</sub>Q–B<sub>2</sub>Q<sub>3</sub>–CQ<sub>2</sub> (B = Ga, In; C = Si, Ge, Sn; Q = S, Se) system were prepared
for the first time through conventional high-temperature solid-state
reaction. They are isostructural with space group <i>Cc</i> (No. 9) in monoclinic phases and feature three-dimensional frameworks
built by the <sub>∞</sub><sup>1</sup>[In<sub>2</sub>MS<sub>6</sub>]<sup>2–</sup> (M = Si,
Ge) chains through corner-sharing InS<sub>4</sub> tetrahedra and MS<sub>4</sub> (M = Si, Ge) tetrahedra, with Na<sup>+</sup> cation located
in the cavities. They display moderate second harmonic generation
(SHG) conversion efficiencies compared with commercial AgGaS<sub>2</sub>, with phase-matching behavior at 1800 nm and laser-induced damage
thresholds 6.9 and 4.0 times higher than that of AgGaS<sub>2</sub>, respectively. Therefore, the output SHG intensities of <b>1</b> and <b>2</b> will be ∼4.3 and 4.0 times larger than
that of AgGaS<sub>2</sub>, when the intensity of incident laser increased
to close the damage energy of <b>1</b> and <b>2</b>, indicating
their potential for high-power nonlinear optical application
Thiophosphates Containing Ag<sup>+</sup> and Lone-Pair Cations with Interchiral Double Helix Show Both Ionic Conductivity and Phase Transition
Quaternary metal thiophosphates containing
second-order Jahn–Teller distorted d<sup>10</sup> Ag<sup>+</sup> and lone-pair cations, Ag<sub>3</sub>BiÂ(PS<sub>4</sub>)<sub>2</sub> (<b>1</b>), Ag<sub>7</sub>SnÂ(PS<sub>4</sub>)<sub>3</sub> (<b>2</b>), and Ag<sub>7</sub>PbÂ(PS<sub>4</sub>)<sub>3</sub> (<b>3</b>), were obtained by solid-state synthesis. The structural
frameworks of <b>2</b> and <b>3</b> feature an infinite
1-D interchiral double helix <sub>∞</sub><sup>1</sup>(Ag<sub>3</sub>P<sub>2</sub>S<sub>11</sub>),
which is rare in inorganic compounds. Compound <b>3</b> undergoes
a significant first-order structural phase transition from monoclinic
to hexagonal at ∼204 °C. This can be ascribed to the significant
mismatch in the expansion coefficients between Pb–S (Ag–S)
and P–S bonds evaluated by bond valence theory. The three compounds
are Ag<sup>+</sup> ionic conductors, and Ag<sup>+</sup> ion migration
pathways are proposed by calculating maps of low bond valence mismatch.
Moreover, the optical properties of the three compounds were studied,
and electronic structure calculations were performed. The combination
of second-order Jahn–Teller distorted d<sup>10</sup> cation
and lone-pair cation provides a new strategy to explore new metal
thiophosphates with interesting structures and promising properties
Thiophosphates Containing Ag<sup>+</sup> and Lone-Pair Cations with Interchiral Double Helix Show Both Ionic Conductivity and Phase Transition
Quaternary metal thiophosphates containing
second-order Jahn–Teller distorted d<sup>10</sup> Ag<sup>+</sup> and lone-pair cations, Ag<sub>3</sub>BiÂ(PS<sub>4</sub>)<sub>2</sub> (<b>1</b>), Ag<sub>7</sub>SnÂ(PS<sub>4</sub>)<sub>3</sub> (<b>2</b>), and Ag<sub>7</sub>PbÂ(PS<sub>4</sub>)<sub>3</sub> (<b>3</b>), were obtained by solid-state synthesis. The structural
frameworks of <b>2</b> and <b>3</b> feature an infinite
1-D interchiral double helix <sub>∞</sub><sup>1</sup>(Ag<sub>3</sub>P<sub>2</sub>S<sub>11</sub>),
which is rare in inorganic compounds. Compound <b>3</b> undergoes
a significant first-order structural phase transition from monoclinic
to hexagonal at ∼204 °C. This can be ascribed to the significant
mismatch in the expansion coefficients between Pb–S (Ag–S)
and P–S bonds evaluated by bond valence theory. The three compounds
are Ag<sup>+</sup> ionic conductors, and Ag<sup>+</sup> ion migration
pathways are proposed by calculating maps of low bond valence mismatch.
Moreover, the optical properties of the three compounds were studied,
and electronic structure calculations were performed. The combination
of second-order Jahn–Teller distorted d<sup>10</sup> cation
and lone-pair cation provides a new strategy to explore new metal
thiophosphates with interesting structures and promising properties
Syntheses, Structures, and Nonlinear Optical Properties of Two Sulfides Na<sub>2</sub>In<sub>2</sub>MS<sub>6</sub> (M = Si, Ge)
The first two new Na-containing sulfides
Na<sub>2</sub>In<sub>2</sub>MS<sub>6</sub> (M = Si (<b>1</b>), Ge (<b>2</b>)) in
the Na<sub>2</sub>Q–B<sub>2</sub>Q<sub>3</sub>–CQ<sub>2</sub> (B = Ga, In; C = Si, Ge, Sn; Q = S, Se) system were prepared
for the first time through conventional high-temperature solid-state
reaction. They are isostructural with space group <i>Cc</i> (No. 9) in monoclinic phases and feature three-dimensional frameworks
built by the <sub>∞</sub><sup>1</sup>[In<sub>2</sub>MS<sub>6</sub>]<sup>2–</sup> (M = Si,
Ge) chains through corner-sharing InS<sub>4</sub> tetrahedra and MS<sub>4</sub> (M = Si, Ge) tetrahedra, with Na<sup>+</sup> cation located
in the cavities. They display moderate second harmonic generation
(SHG) conversion efficiencies compared with commercial AgGaS<sub>2</sub>, with phase-matching behavior at 1800 nm and laser-induced damage
thresholds 6.9 and 4.0 times higher than that of AgGaS<sub>2</sub>, respectively. Therefore, the output SHG intensities of <b>1</b> and <b>2</b> will be ∼4.3 and 4.0 times larger than
that of AgGaS<sub>2</sub>, when the intensity of incident laser increased
to close the damage energy of <b>1</b> and <b>2</b>, indicating
their potential for high-power nonlinear optical application