5 research outputs found
Narrow-Band Red Emission in the Nitridolithoaluminate Sr<sub>4</sub>[LiAl<sub>11</sub>N<sub>14</sub>]:Eu<sup>2+</sup>
The
new narrow-band red-emitting phosphor material Sr<sub>4</sub>[LiAl<sub>11</sub>N<sub>14</sub>]:Eu<sup>2+</sup> was synthesized
by solid-state reaction using a tungsten crucible with a cover plate
in a tube furnace. When excited with blue light (460 nm), it exhibits
red fluorescence with an emission maximum at 670 nm and a full width
at half-maximum of 1880 cm<sup>–1</sup> (∼85 nm). The
crystal structure was solved and refined from single-crystal X-ray
diffraction data. This new compound from the group of the nitridolithoaluminates
crystallizes in the orthorhombic space group <i>Pnnm</i> (No. 58) with the following unit-cell parameters: <i>a</i> = 10.4291(7) Ã…, <i>b</i> = 10.4309(7) Ã…, and <i>c</i> = 3.2349(2) Ã…. Sr<sub>4</sub>[LiAl<sub>11</sub>N<sub>14</sub>]:Eu<sup>2+</sup> shows a pronounced tetragonal pseudo-symmetry.
It consists of a framework of disordered (Al/Li)ÂN<sub>4</sub> and
AlN<sub>4</sub> tetrahedra that are connected to each other by common
corners and edges. Along the [001] direction, the tetrahedral network
creates empty four-membered-ring channels as well as five-membered-ring
channels, in which the Sr<sup>2+</sup> cations are located
Magnesium Double Nitride Mg<sub>3</sub>GaN<sub>3</sub> as New Host Lattice for Eu<sup>2+</sup> Doping: Synthesis, Structural Studies, Luminescence, and Band-Gap Determination
The
double nitride Mg<sub>3</sub>GaN<sub>3</sub> and binary nitride
Mg<sub>3</sub>N<sub>2</sub> were synthesized from the elements by
reaction with NaN<sub>3</sub> in a sodium flux. Reactions were carried
out at 760 °C in welded shut tantalum ampules. Mg<sub>3</sub>GaN<sub>3</sub> was obtained as single crystals (space group <i>R</i>3̅<i>m</i> (No. 166), <i>a</i> = 3.3939(5) Å and <i>c</i> = 25.854(5) Å, <i>Z</i> = 3, <i>R</i>1 = 0.0252, <i>wR</i>2 = 0.0616 for 10 refined parameters, 264 diffraction data points).
This double nitride consists of an uncharged three-dimensional network
of MgN<sub>4</sub> and mixed (Mg/Ga)ÂN<sub>4</sub> tetrahedra, which
share common corners and edges. First-principles density functional
theory (DFT) calculations predict Mg<sub>3</sub>GaN<sub>3</sub> to
have a direct band gap of 3.0 eV, a value supported by soft X-ray
spectroscopy measurements at the N K-edge. Eu<sup>2+</sup>-doped samples
show yellow luminescence when irradiated with UV to blue light (λ<sub>max</sub> = 578 nm, full width at half maximum (fwhm) = 132 nm).
Eu<sup>2+</sup>-doped samples of Mg<sub>3</sub>N<sub>2</sub> also
show luminescence at room temperature when excited with ultraviolet
(UV) to blue light. The maximum intensity of the emission band is
found at 589 nm (fwhm = 145 nm)
Structural Redetermination and Photoluminescence Properties of the Niobium Oxyphosphate (NbO)<sub>2</sub>P<sub>4</sub>O<sub>13</sub>
The structure of (NbO)<sub>2</sub>P<sub>4</sub>O<sub>13</sub> was solved and refined based on new single-crystal
diffraction data revealing considerably more complexity than previously
described. (NbO)<sub>2</sub>P<sub>4</sub>O<sub>13</sub> crystallizes
in the triclinic space group <i>P</i>1Ì… with <i>Z</i> = 6. The lattice parameters determined at room temperature
are <i>a</i> = 1066.42(4) pm, <i>b</i> = 1083.09(4)
pm, <i>c</i> = 1560.46(5) pm, α = 98.55(1)°,
β = 95.57(1)°, γ = 102.92(1)°, and <i>V</i> = 1.7213(2) nm<sup>3</sup>. The superstructure contains 64 unique
atoms including two disordered semioccupied oxygen positions. An unusual
180° bond angle between two [P<sub>4</sub>O<sub>13</sub>]<sup>6–</sup> groups was refined to form half-occupied, split positions
in agreement with previous reports. The IR and Raman spectra reflect
the appearance of overlapping bands assignable to specific group vibrations
as well as P–O–P linkages present in the [P<sub>4</sub>O<sub>13</sub>]<sup>6–</sup> entities. Investigation of the
powdered product concerning its photoluminescence properties revealed
an excitability in the UV at 270 nm assigned to O2p–Nb4d charge
transfer transitions. A resulting broad-band emission with the maximum
in the visible region at 455 nm was determined
High-Pressure Synthesis and Characterization of Li<sub>2</sub>Ca<sub>3</sub>[N<sub>2</sub>]<sub>3</sub>An Uncommon Metallic Diazenide with [N<sub>2</sub>]<sup>2–</sup> Ions
Dinitrogen (N<sub>2</sub>) ligation
is a common and well-characterized
structural motif in bioinorganic synthesis. In solid-state chemistry,
on the other hand, homonuclear dinitrogen entities as structural building
units proved existence only very recently. High-pressure/high-temperature
(HP/HT) syntheses have afforded a number of binary diazenides and
pernitrides with [N<sub>2</sub>]<sup>2–</sup> and [N<sub>2</sub>]<sup>4–</sup> ions, respectively. Here, we report on the
HP/HT synthesis of the first ternary diazenide. Li<sub>2</sub>Ca<sub>3</sub>[N<sub>2</sub>]<sub>3</sub> (space group <i>Pmma</i>, no. 51, <i>a</i> = 4.7747(1), <i>b</i> = 13.9792(4), <i>c</i> = 8.0718(4)
Ã…, <i>Z</i> = 4, <i>wR</i><sub>p</sub> =
0.08109) was synthesized by controlled thermal decomposition of a
stoichiometric mixture of lithium azide and calcium azide in a multianvil
device under a pressure of 9 GPa at 1023 K. Powder X-ray diffraction
analysis reveals strongly elongated N–N bond lengths of <i>d</i><sub>NN</sub> = 1.34(2)–1.35(3) Å exceeding
those of previously known, binary diazenides. In fact, the refined
N–N distances in Li<sub>2</sub>Ca<sub>3</sub>[N<sub>2</sub>]<sub>3</sub> would rather suggest the presence of [N<sub>2</sub>]<sup>3·–</sup> radical ions. Also, characteristic features
of the N–N stretching vibration occur at lower wavenumbers
(1260–1020 cm<sup>–1</sup>) than in the binary phases,
and these assignments are supported by first-principles phonon calculations.
Ultimately, the true character of the N<sub>2</sub> entity in Li<sub>2</sub>Ca<sub>3</sub>[N<sub>2</sub>]<sub>3</sub> is probed by a variety
of complementary techniques, including electron diffraction, electron
spin resonance spectroscopy (ESR), magnetic and electric conductivity
measurements, as well as density-functional theory calculations (DFT).
Unequivocally, the title compound is shown to be metallic containing
diazenide [N<sub>2</sub>]<sup>2–</sup> units according to the
formula (Li<sup>+</sup>)<sub>2</sub>(Ca<sup>2+</sup>)<sub>3</sub>([N<sub>2</sub>]<sup>2–</sup>)<sub>3</sub>·(e<sup>–</sup>)<sub>2</sub>
High-Pressure Synthesis and Characterization of Li<sub>2</sub>Ca<sub>3</sub>[N<sub>2</sub>]<sub>3</sub>An Uncommon Metallic Diazenide with [N<sub>2</sub>]<sup>2–</sup> Ions
Dinitrogen (N<sub>2</sub>) ligation
is a common and well-characterized
structural motif in bioinorganic synthesis. In solid-state chemistry,
on the other hand, homonuclear dinitrogen entities as structural building
units proved existence only very recently. High-pressure/high-temperature
(HP/HT) syntheses have afforded a number of binary diazenides and
pernitrides with [N<sub>2</sub>]<sup>2–</sup> and [N<sub>2</sub>]<sup>4–</sup> ions, respectively. Here, we report on the
HP/HT synthesis of the first ternary diazenide. Li<sub>2</sub>Ca<sub>3</sub>[N<sub>2</sub>]<sub>3</sub> (space group <i>Pmma</i>, no. 51, <i>a</i> = 4.7747(1), <i>b</i> = 13.9792(4), <i>c</i> = 8.0718(4)
Ã…, <i>Z</i> = 4, <i>wR</i><sub>p</sub> =
0.08109) was synthesized by controlled thermal decomposition of a
stoichiometric mixture of lithium azide and calcium azide in a multianvil
device under a pressure of 9 GPa at 1023 K. Powder X-ray diffraction
analysis reveals strongly elongated N–N bond lengths of <i>d</i><sub>NN</sub> = 1.34(2)–1.35(3) Å exceeding
those of previously known, binary diazenides. In fact, the refined
N–N distances in Li<sub>2</sub>Ca<sub>3</sub>[N<sub>2</sub>]<sub>3</sub> would rather suggest the presence of [N<sub>2</sub>]<sup>3·–</sup> radical ions. Also, characteristic features
of the N–N stretching vibration occur at lower wavenumbers
(1260–1020 cm<sup>–1</sup>) than in the binary phases,
and these assignments are supported by first-principles phonon calculations.
Ultimately, the true character of the N<sub>2</sub> entity in Li<sub>2</sub>Ca<sub>3</sub>[N<sub>2</sub>]<sub>3</sub> is probed by a variety
of complementary techniques, including electron diffraction, electron
spin resonance spectroscopy (ESR), magnetic and electric conductivity
measurements, as well as density-functional theory calculations (DFT).
Unequivocally, the title compound is shown to be metallic containing
diazenide [N<sub>2</sub>]<sup>2–</sup> units according to the
formula (Li<sup>+</sup>)<sub>2</sub>(Ca<sup>2+</sup>)<sub>3</sub>([N<sub>2</sub>]<sup>2–</sup>)<sub>3</sub>·(e<sup>–</sup>)<sub>2</sub>