5 research outputs found
Ba<sub>3</sub>Ga<sub>3</sub>N<sub>5</sub>î—¸A Novel Host Lattice for Eu<sup>2+</sup>-Doped Luminescent Materials with Unexpected Nitridogallate Substructure
The alkaline earth nitridogallate Ba<sub>3</sub>Ga<sub>3</sub>N<sub>5</sub> was synthesized from the elements in a sodium
flux at 760
°C utilizing weld shut tantalum ampules. The crystal structure
was solved and refined on the basis of single-crystal X-ray diffraction
data. Ba<sub>3</sub>Ga<sub>3</sub>N<sub>5</sub> (space group <i>C</i>2/<i>c</i> (No. 15), <i>a</i> = 16.801(3), <i>b</i> = 8.3301(2), <i>c</i> = 11.623(2) Å, β
= 109.92(3)°, <i>Z</i> = 8) contains a hitherto unknown
structural motif in nitridogallates, namely, infinite strands made
up of GaN<sub>4</sub> tetrahedra, each sharing two edges and at least
one corner with neighboring GaN<sub>4</sub> units. There are three
Ba<sup>2+</sup> sites with coordination numbers six or eight, respectively,
and one Ba<sup>2+</sup> position exhibiting a low coordination number
4 corresponding to a distorted tetrahedron. Eu<sup>2+</sup>-doped
samples show red luminescence when excited by UV irradiation at room
temperature. Luminescence investigations revealed a maximum emission
intensity at 638 nm (FWHM =2123 cm<sup>–1</sup>). Ba<sub>3</sub>Ga<sub>3</sub>N<sub>5</sub> is the first nitridogallate for which
parity allowed broadband emission due to Eu<sup>2+</sup>-doping has
been found. The electronic structure of both Ba<sub>3</sub>Ga<sub>3</sub>N<sub>5</sub> as well as isoelectronic but not isostructural
Sr<sub>3</sub>Ga<sub>3</sub>N<sub>5</sub> was investigated by DFT
methods. The calculations revealed a band gap of 1.53 eV for Sr<sub>3</sub>Ga<sub>3</sub>N<sub>5</sub> and 1.46 eV for Ba<sub>3</sub>Ga<sub>3</sub>N<sub>5</sub>
Nontypical Luminescence Properties and Structural Relation of Ba<sub>3</sub>P<sub>5</sub>N<sub>10</sub>X:Eu<sup>2+</sup> (X = Cl, I): Nitridophosphate Halides with Zeolite-like Structure
The isotypic nitridophosphates Ba<sub>3</sub>P<sub>5</sub>N<sub>10</sub>X (X = Cl, I) have been synthesized
by high-temperature reaction
under pressures between 1 and 5 GPa. The crystal structures of both
compounds were solved and refined using single-crystal X-ray diffraction
data. Accuracy of the structure determination as well as phase purity
of the products were confirmed by Rietveld refinement and FTIR spectroscopy.
The band gap values (4.0–4.3 eV) for the direct transitions
were determined from UV–vis data using the Kubelka–Munk
function and were confirmed by DFT calculations. Both compounds crystallize
in the Ba<sub>3</sub>P<sub>5</sub>N<sub>10</sub>Br structure type
(space group <i>Pnma</i> (No. 62), <i>Z</i> =
8; Ba<sub>3</sub>P<sub>5</sub>N<sub>10</sub>Cl, <i>a</i> = 12.5182(5) Ã…, <i>b</i> = 13.1798(5) Ã…, <i>c</i> = 13.7676(6) Ã…, <i>R</i>1 = 0.0214, <i>wR</i>2 = 0.0526; Ba<sub>3</sub>P<sub>5</sub>N<sub>10</sub>I, <i>a</i> = 12.6311(7) Ã…, <i>b</i> = 13.2565(8) Ã…, <i>c</i> = 13.8689(8) Ã…, <i>R</i>1 = 0.0257, <i>wR</i>2 = 0.0586) with a tetrahedra network being analogous
to the topology of the JOZ zeolite structure type. The crystal structure
is built up of all-side vertex-sharing PN<sub>4</sub> tetrahedra leading
to a zeolite-like framework with three-dimensional <i>achter</i>-ring channels containing alternately Ba and respective halide atoms.
The condensed <i>dreier</i>-, <i>vierer</i>-,
and <i>sechser</i>-rings form two different composite building
units made up of 3<sup>4</sup>4<sup>2</sup>8<sup>6</sup>-cages. Upon
being doped with Eu<sup>2+</sup>, the title compounds exhibit intriguing
luminescence properties, which were compared with that of Ba<sub>3</sub>P<sub>5</sub>N<sub>10</sub>Br:Eu<sup>2+</sup>. Upon excitation by
near-UV light, nonsaturated color luminescence from multiple emission
centers was observed in the orange (X = Cl) and cyan to amber (X =
I) spectral range of the visible spectrum
Ca[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup>î—¸A Narrow-Band Red-Emitting Nitridolithoaluminate
CaÂ[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup> is an intriguing
new narrow-band red-emitting phosphor material with potential for
application in high-power phosphor-converted light-emitting diodes
(pc-LEDs). With excitation by blue InGaN-based LEDs, the compound
exhibits an emission maximum at 668 nm with a full width at half maximum
of only 1333 cm<sup>–1</sup> (∼60 nm). CaÂ[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup> was synthesized from Ca, LiAlH<sub>4</sub>, LiN<sub>3</sub>, AlF<sub>3</sub>, and EuF<sub>3</sub> in
weld-shut Ta ampules, and the structure was solved and refined on
the basis of single-crystal X-ray diffraction data. After isotypical
crystallization with NaÂ[Li<sub>3</sub>SiO<sub>4</sub>], the compound
forms a highly condensed framework of AlN<sub>4</sub> and LiN<sub>4</sub> tetrahedra [<i>I</i>4<sub>1</sub>/<i>a</i> (no. 88), <i>Z</i> = 16, <i>a</i> = 11.1600(16)
Ã…, and <i>c</i> = 12.865(3) Ã…] and can thus by
classified as a nitridolithoaluminate. Both types of polyhedra are
connected to each other by common edges and corners, yielding a high
degree of condensation, κ = 1. The Ca site is positioned in
the center of <i>vierer</i> ring channels along [001] and
coordinated in a cuboidal manner by eight N atoms. To validate the
presence of Li, transmission electron microscopy (TEM) investigations
employing electron energy-loss spectroscopy (EELS) were carried out.
Furthermore, to confirm the electrostatic bonding interactions and
the chemical composition, lattice energy calculations [Madelung part
of lattice energy (MAPLE)] have been performed
Nitridomagnesosilicate Ba[Mg<sub>3</sub>SiN<sub>4</sub>]:Eu<sup>2+</sup> and Structure–Property Relations of Similar Narrow-Band Red Nitride Phosphors
The
nitridomagnesosilicate BaÂ[Mg<sub>3</sub>SiN<sub>4</sub>] has
been synthesized in an arc-welded Ta ampule. The crystal structure
was solved and refined from single-crystal X-ray data and Rietveld
refinement on the basis of powder X-ray diffraction data, revealing
a distorted triclinic variant of the UCr<sub>4</sub>C<sub>4</sub> structure
type (space group <i>P</i>1̅ (no. 2), <i>Z</i> = 1, <i>a</i> = 3.451(1), <i>b</i> = 6.069(5), <i>c</i> = 6.101(4) Å, α = 85.200(7), β = 73.697(5),
γ = 73.566(8)°, <i>R</i><sub>p</sub> = 0.0218, <i>R</i><sub>wp</sub> = 0.0290). The crystal structure of BaÂ[Mg<sub>3</sub>SiN<sub>4</sub>] consists of a highly condensed network of
(Mg,Si)ÂN<sub>4</sub> tetrahedra with Ba<sup>2+</sup> centered inside <i>vierer</i> ring channels along [100] in a cuboidal coordination
by N<sup>3–</sup>. From UV/vis-reflectance data, a band gap
of ∼4.0 eV was estimated. Doping with Eu<sup>2+</sup> shows
promising luminescence properties of λ<sub>em</sub> = 670 nm
with an fwhm ∼1970 cm<sup>–1</sup>. Furthermore, anomalous
luminescence phenomena, such as trapped-exciton emission, were identified
and considered. BaÂ[Mg<sub>3</sub>SiN<sub>4</sub>]:Eu<sup>2+</sup> is
a further narrow-band red-emitting phosphor and is discussed concerning
the structure–property relations of recently reported Eu<sup>2+</sup>-doped nitrides with narrow-band red emission
Group (III) Nitrides <i>M</i>[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>] (<i>M</i> = Ca, Sr, Ba, Eu) and Ba[Mg<sub>2</sub>Ga<sub>2</sub>N<sub>4</sub>]î—¸Structural Relation and Nontypical Luminescence Properties of Eu<sup>2+</sup> Doped Samples
The isotypic nitridomagnesoaluminates <i>M</i>[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>] (<i>M</i> = Ca,Sr,
Ba,Eu) as well as a novel nitridomagnesogallate BaÂ[Mg<sub>2</sub>Ga<sub>2</sub>N<sub>4</sub>] have been synthesized by high-temperature reactions
in arc-welded tantalum ampules. The crystal structures were solved
and refined using single-crystal X-ray diffraction or powder X-ray
diffraction data, respectively. All compounds crystallize in the UCr<sub>4</sub>C<sub>4</sub>-structure type (space group <i>I</i>4/<i>m</i> (no. 87), <i>Z</i> = 2, CaÂ[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.0655(11), <i>c</i> = 3.2857(7) Ã…, <i>wR</i>2 = 0.085 SrÂ[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.1008(11), <i>c</i> = 3.3269(7) Ã…, <i>wR</i>2 = 0.084; EuÂ[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.1539(12), <i>c</i> = 3.3430(7) Ã…, <i>wR</i>2 = 0.033; BaÂ[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.2602(9), <i>c</i> = 3.43198(19) Ã…, <i>wR</i>p = 0.031; BaÂ[Mg<sub>2</sub>Ga<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.3654(12), <i>c</i> = 3.4411(7) Ã…, <i>wR</i>2 = 0.031) forming
highly condensed anionic networks of disordered (Al/Mg)ÂN<sub>4</sub> and (Ga/Mg)ÂN<sub>4</sub> units, connected to each other by common
edges and corners. The <i>M</i><sup>2+</sup> site is centered
in <i>vierer</i> ring channels along [001] and coordinated
in a cuboidal surrounding by N. Eu<sup>2+</sup> doped samples of <i>M</i>[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>] (<i>M</i> = Ca,Sr,Ba) exhibit nontypical luminescence properties including
trapped exciton emission in the red spectral region. These compounds
widen the group of novel red-emitting materials such as CaÂ[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup>, SrÂ[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup>, or SrÂ[Mg<sub>3</sub>SiN<sub>4</sub>]:Eu<sup>2+</sup>. Therefore, deep discussion of the observed anomalous luminescence
is essential to understand the correlations between all these materials,
which are fundamental to design narrow band luminescence of Eu<sup>2+</sup> systems