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

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    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

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    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) Å, <i>b</i> = 13.1798(5) Å, <i>c</i> = 13.7676(6) Å, <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) Å, <i>b</i> = 13.2565(8) Å, <i>c</i> = 13.8689(8) Å, <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

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    Ca­[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). Ca­[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 Na­[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) Å, and <i>c</i> = 12.865(3) Å] 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

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    The nitridomagnesosilicate Ba­[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 Ba­[Mg<sub>3</sub>SiN<sub>4</sub>] consists of a highly condensed network of (Mg,Si)­N<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. Ba­[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

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    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 Ba­[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, Ca­[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.0655(11), <i>c</i> = 3.2857(7) Å, <i>wR</i>2 = 0.085 Sr­[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.1008(11), <i>c</i> = 3.3269(7) Å, <i>wR</i>2 = 0.084; Eu­[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.1539(12), <i>c</i> = 3.3430(7) Å, <i>wR</i>2 = 0.033; Ba­[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.2602(9), <i>c</i> = 3.43198(19) Å, <i>wR</i>p = 0.031; Ba­[Mg<sub>2</sub>Ga<sub>2</sub>N<sub>4</sub>]: <i>a</i> = 8.3654(12), <i>c</i> = 3.4411(7) Å, <i>wR</i>2 = 0.031) forming highly condensed anionic networks of disordered (Al/Mg)­N<sub>4</sub> and (Ga/Mg)­N<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 Ca­[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup>, Sr­[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup>, or Sr­[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
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