6 research outputs found
ZSMâ5 Zeolite: Complete Al Bond Connectivity and Implications on Structure Formation from Solid-State NMR and Quantum Chemistry Calculations
Al
site distribution in the structurally complex and industrially
important ZSM-5 zeolite is determined by studying the spectroscopic
response of AlÂ(OSi)<sub>4</sub> units and using a self-consistent
combination of up-to-date solid-state NMR correlations (<sup>29</sup>Siâ<sup>27</sup>Al and <sup>1</sup>Hâ<sup>27</sup>Al <i>D</i>-HMQC) and quantum chemistry methods (DFT-D). To unravel
the driving forces behind specific Al sitting positions, our approach
focuses on ZSM-5 containing its more efficient OSDA, tetrapropylammonium
Transparency through Structural Disorder: A New Concept for Innovative Transparent Ceramics
Transparent
polycrystalline ceramics present significant economical and functional
advantages over single crystal materials for optical, communication,
and laser technologies. To date, transparency in these ceramics is
ensured either by an optical isotropy (i.e., cubic symmetry) or a
nanometric crystallite size, and the main challenge remains to eliminate
porosity through complex high pressureâhigh temperature synthesis.
Here we introduce a new concept to achieve ultimate transparency reaching
the theoretical limit. We use a controlled degree of chemical disorder
in the structure to obtain optical isotropy at the micrometer length
scale. This approach can be applied in the case of anisotropic structures
and micrometer scale crystal size ceramics. We thus report Sr<sub>1+<i>x</i>/2</sub>Al<sub>2+<i>x</i></sub>Si<sub>2â<i>x</i></sub>O<sub>8</sub> (0 < <i>x</i> †0.4) readily scalable polycrystalline ceramics elaborated
by full and congruent crystallization from glass. These materials
reach 90% transmittance. This innovative method should drive the development
of new highly transparent materials with technologically relevant
applications
Local Disorder and Tunable Luminescence in Sr<sub>1â<i>x</i>/2</sub>Al<sub>2â<i>x</i></sub>Si<sub><i>x</i></sub>O<sub>4</sub> (0.2 †<i>x</i> †0.5) Transparent Ceramics
Eu-doped Sr<sub>1â<i>x</i>/2</sub>Al<sub>2â<i>x</i></sub>Si<sub><i>x</i></sub>O<sub>4</sub> (<i>x</i> = 0.2,
0.4, and 0.5) transparent ceramics have been synthesized by full and
congruent crystallization from glasses prepared by aerodynamic levitation
and laser-heating method. Structural refinements from synchrotron
and neutron powder diffraction data show that the ceramics adopt a
1 Ă 1 Ă 2 superstructure compared to the SrAl<sub>2</sub>O<sub>4</sub> hexagonal polymorph. While the observed superstructure
reflections indicate a long-range ordering of the Sr vacancies in
the structure, <sup>29</sup>Si and <sup>27</sup>Al solid-state NMR
measurements associated with DFT computations reveal a significant
degree of disorder in the fully polymerized tetrahedral network. This
is evidenced through the presence of SiâOâSi bonds,
as well as SiÂ(OAl)<sub>4</sub> units at remote distances of the Sr
vacancies and AlÂ(OAl)<sub>4</sub> units in the close vicinity of Sr
vacancies departing from local charge compensation in the network.
The transparent ceramics can be doped by europium to induce light
emission arising from the volume under UV excitation. Luminescence
measurements then reveal the coexistence of Eu<sup>2+</sup> and Eu<sup>3+</sup> in the samples, thereby allowing tuning the emission color
depending on the excitation wavelength and suggesting possible applications
such as solid state lighting
Synthesis and Structure Resolution of RbLaF<sub>4</sub>
The synthesis and structure resolution of RbLaF<sub>4</sub> are
described. RbLaF<sub>4</sub> is synthesized by solid-state reaction
between RbF and LaF<sub>3</sub> at 425 °C under a nonoxidizing
atmosphere. Its crystal structure has been resolved by combining neutron
and synchrotron powder diffraction data refinements (<i>Pnma,</i> <i>a</i> = 6.46281(2) Ă
, <i>b</i> = 3.86498(1)
Ă
, <i>c</i> = 16.17629(4) Ă
, <i>Z</i> = 4). One-dimensional <sup>87</sup>Rb, <sup>139</sup>La, and <sup>19</sup>F MAS NMR spectra have been recorded and are in agreement
with the proposed structural model. Assignment of the <sup>19</sup>F resonances is performed on the basis of both <sup>19</sup>Fâ<sup>139</sup>La <i>J</i>-coupling multiplet patterns observed
in a heteronuclear DQ-filtered <i>J</i>-resolved spectrum
and <sup>19</sup>Fâ<sup>87</sup>Rb HMQC MAS experiments. DFT
calculations of both the <sup>19</sup>F isotropic chemical shieldings
and the <sup>87</sup>Rb, <sup>139</sup>La electric field gradient
tensors using the GIPAW and PAW methods implemented in the CASTEP
code are in good agreement with the experimental values and support
the proposed structural model. Finally, the conductivity of RbLaF<sub>4</sub> and luminescence properties of Eu-doped LaRbF<sub>4</sub> are investigated
Synthesis and Structure Resolution of RbLaF<sub>4</sub>
The synthesis and structure resolution of RbLaF<sub>4</sub> are
described. RbLaF<sub>4</sub> is synthesized by solid-state reaction
between RbF and LaF<sub>3</sub> at 425 °C under a nonoxidizing
atmosphere. Its crystal structure has been resolved by combining neutron
and synchrotron powder diffraction data refinements (<i>Pnma,</i> <i>a</i> = 6.46281(2) Ă
, <i>b</i> = 3.86498(1)
Ă
, <i>c</i> = 16.17629(4) Ă
, <i>Z</i> = 4). One-dimensional <sup>87</sup>Rb, <sup>139</sup>La, and <sup>19</sup>F MAS NMR spectra have been recorded and are in agreement
with the proposed structural model. Assignment of the <sup>19</sup>F resonances is performed on the basis of both <sup>19</sup>Fâ<sup>139</sup>La <i>J</i>-coupling multiplet patterns observed
in a heteronuclear DQ-filtered <i>J</i>-resolved spectrum
and <sup>19</sup>Fâ<sup>87</sup>Rb HMQC MAS experiments. DFT
calculations of both the <sup>19</sup>F isotropic chemical shieldings
and the <sup>87</sup>Rb, <sup>139</sup>La electric field gradient
tensors using the GIPAW and PAW methods implemented in the CASTEP
code are in good agreement with the experimental values and support
the proposed structural model. Finally, the conductivity of RbLaF<sub>4</sub> and luminescence properties of Eu-doped LaRbF<sub>4</sub> are investigated
New Transparent Glass-Ceramics Based on the Crystallization of âAnti-glassâ Spherulites in the Bi<sub>2</sub>O<sub>3</sub>âNb<sub>2</sub>O<sub>5</sub>âTeO<sub>2</sub> System
The crystallization of the Bi<sub>0.5</sub>Nb<sub>0.5</sub>Te<sub>3</sub>O<sub>8</sub> (7.14 Bi<sub>2</sub>O<sub>3</sub>â7.14Nb<sub>2</sub>O<sub>5</sub>â85.72TeO<sub>2</sub>) glass composition
shows numerous original spherulite-like shape or âdropletsâ
crystalline domains through the bulk. Both SEM-EDS and microprobe
measurements demonstrate that both these droplets and the glassy matrix
present the same composition. The combination of information obtained
from various complementary techniques, electron probe microanalysis,
Raman, and SEM-EDS, then leads to the identification of the spherulites
as a new Bi<sub>0.5</sub>Nb<sub>0.5</sub>Te<sub>3</sub>O<sub>8</sub> âanti-glassâ phase. However, the crystallization mechanism
is complex since microcracks are observed at the surface of the spherulites
in some glass-ceramic materials, suggesting a confined crystal growth.
Therefore, the crystallization process appears much different from
a homogeneous congruent crystallization. The photoluminescence (PL)
properties of the (1 wt %) Er<sub>2</sub>O<sub>3</sub>-doped Bi<sub>0.5</sub>Nb<sub>0.5</sub>Te<sub>3</sub>O<sub>8</sub> glass-ceramics
were investigated during isothermal crystallization of the parent
glass at 380 °C. The evolution of the PL signal (<sup>4</sup>I<sub>13/2</sub> â <sup>4</sup>I<sub>15/2</sub> transition)
enables indirect detection of the first steps of crystallization.
Moreover, the PL data indicate random nucleation with respect to the
location of Er<sup>3+</sup> ions, whereas the integrated PL intensity
and lifetime values show very comparable evolution trends as a function
of the crystallization rate