37 research outputs found
Three New Alkaline Beryllium Borates LiBeBO<sub>3</sub>, Li<sub>6</sub>Be<sub>3</sub>B<sub>4</sub>O<sub>12</sub>, and Li<sub>8</sub>Be<sub>5</sub>B<sub>6</sub>O<sub>18</sub> in the Ternary Phase Diagrams Li<sub>2</sub>O–BeO–B<sub>2</sub>O<sub>3</sub>
The
phase diagram in the Li<sub>2</sub>O–BeO–B<sub>2</sub>O<sub>3</sub> system has been systematically investigated
by the methods of visual polythermal analysis, spontaneous crystallization,
and X-ray diffraction. Three new alkaline beryllium borates, namely,
LiBeBO<sub>3</sub>, Li<sub>6</sub>Be<sub>3</sub>B<sub>4</sub>O<sub>12</sub>, and Li<sub>8</sub>Be<sub>5</sub>B<sub>6</sub>O<sub>18</sub>, were synthesized with molten fluxes based on Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> solvent in this system. All of the materials
are centrosymmetric. The similarity of the fundamental building block
of the title compounds has been compared. Thermal analysis and powder
XRD studies were applied to determine phase relation and their incongruent
melting behavior. The UV–vis diffuse reflectance spectroscopy
demonstrated that the UV cutoff edges of the aforementioned materials
are all below 200 nm
Alkaline-Alkaline Earth Fluoride Carbonate Crystals ABCO<sub>3</sub>F (A = K, Rb, Cs; B = Ca, Sr, Ba) as Nonlinear Optical Materials
A new series of alkaline–alkaline earth fluoride carbonates (KSrCO3F, RbSrCO3F, KCaCO3F, RbCaCO3F, CsCaCO3F, and Cs3Ba4(CO3)3F5) were synthesized by spontaneous crystallization with molten fluxes. Their crystal structures, except for Cs3Ba4(CO3)3F5, exhibit the stacking of [AF]∞ (A = K, Rb, Cs) and [B(CO3)]∞ (B = Ca, Sr) layers, and the coplanar alignment of [CO3] triangles. The results from the UV–vis diffuse reflectance spectroscopy study of the powder samples indicated that the short-wavelength absorption edges were all below 200 nm, except for Cs3Ba4(CO3)3F5, which is about 210 nm. Second-harmonic generation (SHG) on polycrystalline samples was measured using the Kurtz and Perry technique, which indicated that these carbonates are all phase-matchable materials in both visible and the UV region, and their measured SHG coefficients were about 3.33, 3.33, 3.61, 1.11, 1.11, and 1.20 times as large as that of d36 (KDP), respectively
Alkaline-Alkaline Earth Fluoride Carbonate Crystals ABCO<sub>3</sub>F (A = K, Rb, Cs; B = Ca, Sr, Ba) as Nonlinear Optical Materials
A new series of alkaline–alkaline earth fluoride carbonates (KSrCO<sub>3</sub>F, RbSrCO<sub>3</sub>F, KCaCO<sub>3</sub>F, RbCaCO<sub>3</sub>F, CsCaCO<sub>3</sub>F, and Cs<sub>3</sub>Ba<sub>4</sub>(CO<sub>3</sub>)<sub>3</sub>F<sub>5</sub>) were synthesized by spontaneous crystallization with molten fluxes. Their crystal structures, except for Cs<sub>3</sub>Ba<sub>4</sub>(CO<sub>3</sub>)<sub>3</sub>F<sub>5</sub>, exhibit the stacking of [AF]<sub>∞</sub> (A = K, Rb, Cs) and [B(CO<sub>3</sub>)]<sub>∞</sub> (B = Ca, Sr) layers, and the coplanar alignment of [CO<sub>3</sub>] triangles. The results from the UV–vis diffuse reflectance spectroscopy study of the powder samples indicated that the short-wavelength absorption edges were all below 200 nm, except for Cs<sub>3</sub>Ba<sub>4</sub>(CO<sub>3</sub>)<sub>3</sub>F<sub>5</sub>, which is about 210 nm. Second-harmonic generation (SHG) on polycrystalline samples was measured using the Kurtz and Perry technique, which indicated that these carbonates are all phase-matchable materials in both visible and the UV region, and their measured SHG coefficients were about 3.33, 3.33, 3.61, 1.11, 1.11, and 1.20 times as large as that of <i>d</i><sub>36</sub> (KDP), respectively
Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> and Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>: Rare Earth Fluoride Carbonates as Deep-UV Nonlinear Optical Materials
Two
nonlinear optical fluoride carbonate crystals (Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> and Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>) have been synthesized
under subcritical hydrothermal condition. Both crystals crystallize
in the noncentrosymmetric space group <i>Cc</i> (No. 9).
The structure of Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> with high density of [CO<sub>3</sub>] groups
is described as 1D [Na<sub>5</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>] chains connected by [CO<sub>3</sub>] triangles, forming
an intricate three-dimensional framework. Lu<sup>3+</sup> and Na<sup>+</sup> cations are alternatively ordered and disordered in the cavities
of the 3D network. The structure of Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub> is built up from the [NaLu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>] layers which are separated by other Na<sup>+</sup> cations. The [CO<sub>3</sub>] anionic groups arrange approximately
coparallel to the plane. The second harmonic generation (SHG) measurement
indicates that Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> and Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub> have large SHG responses that are approximately 4.29 and
4.21 times KH<sub>2</sub>PO<sub>4</sub> (KDP), respectively. The responses
are also phase-matchable in the visible region. In addition, it exhibits
wide transparent regions ranging from UV to near IR with a short UV
cutoff edge (<200 nm), which suggests that the new compounds are
promising as deep-UV NLO materials
Layered Perovskite-like Nitrate Cs<sub>2</sub>Pb(NO<sub>3</sub>)<sub>2</sub>Br<sub>2</sub> as a Multifunctional Optical Material
A novel alkali metal lead halide
nitrate, Cs2Pb(NO3)2Br2, has been successfully synthesized
via a hydrothermal method. Interestingly, the title compound features
a distinctive Ruddlesden–Popper perovskite-like layered structure,
which induces the outstanding multifunctional optical properties,
including a large birefringence (0.147@546 nm) and broad light-orange
emission. Detailed structural analysis and theoretical calculations
revealed that the large birefringence originates from the p−π
interaction between the Pb2+ cations and NO3 groups and that the excellent luminescence properties derive from
the distortion of PbO4Br4 polyhedra. This work
not only enriches the variant structure types of layered perovskites
but also guides the further exploration of all-inorganic multifunctional
optical materials
Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> and Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>: Rare Earth Fluoride Carbonates as Deep-UV Nonlinear Optical Materials
Two
nonlinear optical fluoride carbonate crystals (Na8Lu2(CO3)6F2 and Na3Lu(CO3)2F2) have been synthesized
under subcritical hydrothermal condition. Both crystals crystallize
in the noncentrosymmetric space group Cc (No. 9).
The structure of Na8Lu2(CO3)6F2 with high density of [CO3] groups
is described as 1D [Na5Lu(CO3)2F2] chains connected by [CO3] triangles, forming
an intricate three-dimensional framework. Lu3+ and Na+ cations are alternatively ordered and disordered in the cavities
of the 3D network. The structure of Na3Lu(CO3)2F2 is built up from the [NaLu(CO3)2F2] layers which are separated by other Na+ cations. The [CO3] anionic groups arrange approximately
coparallel to the plane. The second harmonic generation (SHG) measurement
indicates that Na8Lu2(CO3)6F2 and Na3Lu(CO3)2F2 have large SHG responses that are approximately 4.29 and
4.21 times KH2PO4 (KDP), respectively. The responses
are also phase-matchable in the visible region. In addition, it exhibits
wide transparent regions ranging from UV to near IR with a short UV
cutoff edge (<200 nm), which suggests that the new compounds are
promising as deep-UV NLO materials
Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> and Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>: Rare Earth Fluoride Carbonates as Deep-UV Nonlinear Optical Materials
Two
nonlinear optical fluoride carbonate crystals (Na8Lu2(CO3)6F2 and Na3Lu(CO3)2F2) have been synthesized
under subcritical hydrothermal condition. Both crystals crystallize
in the noncentrosymmetric space group Cc (No. 9).
The structure of Na8Lu2(CO3)6F2 with high density of [CO3] groups
is described as 1D [Na5Lu(CO3)2F2] chains connected by [CO3] triangles, forming
an intricate three-dimensional framework. Lu3+ and Na+ cations are alternatively ordered and disordered in the cavities
of the 3D network. The structure of Na3Lu(CO3)2F2 is built up from the [NaLu(CO3)2F2] layers which are separated by other Na+ cations. The [CO3] anionic groups arrange approximately
coparallel to the plane. The second harmonic generation (SHG) measurement
indicates that Na8Lu2(CO3)6F2 and Na3Lu(CO3)2F2 have large SHG responses that are approximately 4.29 and
4.21 times KH2PO4 (KDP), respectively. The responses
are also phase-matchable in the visible region. In addition, it exhibits
wide transparent regions ranging from UV to near IR with a short UV
cutoff edge (<200 nm), which suggests that the new compounds are
promising as deep-UV NLO materials
Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> and Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>: Rare Earth Fluoride Carbonates as Deep-UV Nonlinear Optical Materials
Two
nonlinear optical fluoride carbonate crystals (Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> and Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>) have been synthesized
under subcritical hydrothermal condition. Both crystals crystallize
in the noncentrosymmetric space group <i>Cc</i> (No. 9).
The structure of Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> with high density of [CO<sub>3</sub>] groups
is described as 1D [Na<sub>5</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>] chains connected by [CO<sub>3</sub>] triangles, forming
an intricate three-dimensional framework. Lu<sup>3+</sup> and Na<sup>+</sup> cations are alternatively ordered and disordered in the cavities
of the 3D network. The structure of Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub> is built up from the [NaLu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>] layers which are separated by other Na<sup>+</sup> cations. The [CO<sub>3</sub>] anionic groups arrange approximately
coparallel to the plane. The second harmonic generation (SHG) measurement
indicates that Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> and Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub> have large SHG responses that are approximately 4.29 and
4.21 times KH<sub>2</sub>PO<sub>4</sub> (KDP), respectively. The responses
are also phase-matchable in the visible region. In addition, it exhibits
wide transparent regions ranging from UV to near IR with a short UV
cutoff edge (<200 nm), which suggests that the new compounds are
promising as deep-UV NLO materials
Using Multifunctional Ionic Liquids in the Synthesis of Crystalline Metal Phosphites and Hybrid Framework Solids
Several crystalline
metal phosphites and related hybrid framework solids were prepared
under ionothermal conditions using ionic liquids as the reactant,
templating agent, and solvent. These compounds display different structures
and some appealing properties such as proton conduction. A variety
of ionic liquids, metal ions, and additional synthetic variants (e.g.,
F- and organic ligands) can be introduced into the metal phosphite
systems, demonstrating the versatility of the synthetic strategy
Na<sub>8</sub>Lu<sub>2</sub>(CO<sub>3</sub>)<sub>6</sub>F<sub>2</sub> and Na<sub>3</sub>Lu(CO<sub>3</sub>)<sub>2</sub>F<sub>2</sub>: Rare Earth Fluoride Carbonates as Deep-UV Nonlinear Optical Materials
Two
nonlinear optical fluoride carbonate crystals (Na8Lu2(CO3)6F2 and Na3Lu(CO3)2F2) have been synthesized
under subcritical hydrothermal condition. Both crystals crystallize
in the noncentrosymmetric space group Cc (No. 9).
The structure of Na8Lu2(CO3)6F2 with high density of [CO3] groups
is described as 1D [Na5Lu(CO3)2F2] chains connected by [CO3] triangles, forming
an intricate three-dimensional framework. Lu3+ and Na+ cations are alternatively ordered and disordered in the cavities
of the 3D network. The structure of Na3Lu(CO3)2F2 is built up from the [NaLu(CO3)2F2] layers which are separated by other Na+ cations. The [CO3] anionic groups arrange approximately
coparallel to the plane. The second harmonic generation (SHG) measurement
indicates that Na8Lu2(CO3)6F2 and Na3Lu(CO3)2F2 have large SHG responses that are approximately 4.29 and
4.21 times KH2PO4 (KDP), respectively. The responses
are also phase-matchable in the visible region. In addition, it exhibits
wide transparent regions ranging from UV to near IR with a short UV
cutoff edge (<200 nm), which suggests that the new compounds are
promising as deep-UV NLO materials
