12 research outputs found

    Tunable Red Luminescence in Nitridomagnesoaluminates α‑Sr<sub>2</sub>[MgAl<sub>5</sub>N<sub>7</sub>]:Eu<sup>2+</sup>, β‑Sr<sub>2</sub>[MgAl<sub>5</sub>N<sub>7</sub>]:Eu<sup>2+</sup>, and Sr<sub>8</sub>[LiMg<sub>2</sub>Al<sub>21</sub>N<sub>28</sub>]:Eu<sup>2+</sup>

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    Red-emitting phosphors with the general sum formula Sr<sub>8</sub>[Li<sub>(2–0.5<i>x</i>)</sub>Mg<sub><i>x</i></sub>Al<sub>(22–0.5<i>x</i>)</sub>N<sub>28</sub>]:Eu<sup>2+</sup> for application in warm-white illumination grade light emitting diodes were obtained by reacting the metals, hydrides, and nitrides in molybdenum crucibles in a hot isostatic press. Upon irradiation with blue light (440 nm), the materials exhibit red luminescence (emission maximum: 633–665 nm; full width at half-maximum (fwhm): 1736–1964 cm<sup>–1</sup>, 78–82 nm) tunable by adjusting the compositional variable <i>x</i> (here, 2 and 4) as well as the activator concentration (here, 0.075–1 atom-% Eu<sup>2+</sup>). The materials show promising thermal behavior of the emission with relative quantum efficiencies, compared to room temperature, of 66% (<i>x</i> = 0) and 84% (<i>x</i> = 2) at 200 °C. α-Sr<sub>8</sub>[Li<sub>(2–0.5<i>x</i>)</sub>Mg<sub><i>x</i></sub>Al<sub>(22–0.5<i>x</i>)</sub>N<sub>28</sub>]:Eu<sup>2+</sup> (<i>x</i> = 2 and 4) crystallizes isotypically with Sr<sub>4</sub>[LiAl<sub>11</sub>N<sub>14</sub>]:Eu<sup>2+</sup> in the orthorhombic space group <i>Pnnm</i> (no. 58) with unit cell parameters <i>a</i> = 10.51818(5)–10.54878(6), <i>b</i> = 10.44513(5)–10.48253(6), and <i>c</i> = 3.25704(1)–3.272752(15) Å. β-Sr<sub>2</sub>[MgAl<sub>5</sub>N<sub>7</sub>]:Eu<sup>2+</sup> (<i>x</i> = 4) crystallizes in the monoclinic space group <i>C</i>2/<i>m</i> (no. 12) with unit cell parameters <i>a</i> = 11.12874(11), <i>b</i> = 3.27289(3), <i>c</i> = 10.54530(11) Å, and β = 109.8939(7)° and is obtained as side phase (≤40 wt %) in syntheses with <i>x</i> = 4. The crystal structure of β-Sr<sub>2</sub>[MgAl<sub>5</sub>N<sub>7</sub>]:Eu<sup>2+</sup> consists of a network of vertex- and edge-sharing Al­(/Mg)­N<sub>4</sub> tetrahedra with four- and five-membered ring channels along [010]. The Sr<sup>2+</sup> ions are located within the five-membered ring channels and are coordinated cube-like by eight N atoms

    Oxonitridosilicate Oxides <i>RE</i><sub>26</sub>Ba<sub>6</sub>[Si<sub>22</sub>O<sub>19</sub>N<sub>36</sub>]O<sub>16</sub>:Eu<sup>2+</sup> (<i>RE</i> = Y, Tb) with a Unique Layered Structure and Orange-Red Luminescence for <i>RE</i> = Y

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    The oxonitridosilicate oxides <i>RE</i><sub>26</sub>Ba<sub>6</sub>[Si<sub>22</sub>O<sub>19</sub>N<sub>36</sub>]­O<sub>16</sub>:Eu<sup>2+</sup> (<i>RE</i> = Y, Tb) were synthesized by high-temperature reaction in a radiofrequency furnace starting from <i>RE</i>F<sub>3</sub>, <i>RE</i><sub>2</sub>O<sub>3</sub> (<i>RE</i> = Y, Tb), BaH<sub>2</sub>, Si­(NH)<sub>2</sub>, and EuF<sub>3</sub>. The structure elucidation is based on single-crystal X-ray data. The isotypic materials crystallize in the monoclinic space group <i>Pm</i> (no. 6) [<i>Z</i> = 3, <i>a</i> = 16.4285(8), <i>b</i> = 20.8423(9), <i>c</i> = 16.9257(8) Å, β = 119.006(3)° for <i>RE</i> = Y and <i>a</i> = 16.5465(7), <i>b</i> = 20.9328(9), <i>c</i> = 17.0038(7) Å, β = 119.103(2)° for <i>RE</i> = Tb]. The unique silicate layers are made up from Q<sup>1</sup>-, Q<sup>2</sup>-, and Q<sup>3</sup>-type Si­(O/N)<sub>4</sub>- as well as Q<sup>4</sup>-type SiN<sub>4</sub>-tetrahedra, forming three slightly differing types of cages. The corresponding 3-fold superstructure as well as pronounced hexagonal pseudosymmetry complicated the structure elucidation. Rietveld refinement on powder X-ray diffraction data, energy-dispersive X-ray spectroscopy and infrared spectroscopy support the findings from single-crystal X-ray data. When excited with UV to blue light, Y<sub>26</sub>Ba<sub>6</sub>[Si<sub>22</sub>O<sub>19</sub>N<sub>36</sub>]­O<sub>16</sub>:Eu<sup>2+</sup> shows broad orange-red luminescence (λ<sub>em</sub> = 628 nm, fwhm ≈ 125 nm/3130 cm<sup>–1</sup>). An optical band gap of 4.2 eV was determined for the doped compound by means of UV/vis spectroscopy

    Unprecedented Deep-Red Ce<sup>3+</sup> Luminescence of the Nitridolithosilicates Li<sub>38.7</sub><i>RE</i><sub>3.3</sub>Ca<sub>5.7</sub>[Li<sub>2</sub>Si<sub>30</sub>N<sub>59</sub>]O<sub>2</sub>F (<i>RE</i> = La, Ce, Y)

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    Ce<sup>3+</sup> doped solids find broad application, e.g. in phosphor converted light emitting diodes, utilizing the usually broad blue to yellow-orange emission of the respective phosphors. The red to infrared spectral range was not yet accessible with the activator Ce<sup>3+</sup>, even in nitride host materials. Here, we report on the nitridolithosilicates Li<sub>38.7</sub><i>RE</i><sub>3.3</sub>Ca<sub>5.7</sub>[Li<sub>2</sub>Si<sub>30</sub>N<sub>59</sub>]­O<sub>2</sub>F (<i>RE</i> = La, Ce, Y) with unique, red-shifted Ce<sup>3+</sup> luminescence. The materials were synthesized by solid-state metathesis reactions in tantalum ampules. The isotypic crystal structures exhibit a highly condensed three-dimensional network made up of SiN<sub>4</sub> and LiN<sub>4</sub> tetrahedra. Crystal structures were refined from single-crystal and powder X-ray diffraction data. The results are supported by energy-dispersive X-ray spectroscopy as well as charge distribution, lattice energy, and bond valence sum calculations. Optical band gaps of ≈4 eV were determined from diffuse reflectance UV/vis data using Tauc plots. The nitridolithosilicates are highly excitable from the UV to the green-yellow spectral range with a preferred excitation wavelength of λ<sub>exc</sub> ≈ 540 nm. The emission spectra peak is in the deep-red with λ<sub>em</sub> = 638–651 nm (fwhm ≈ 3600 cm<sup>–1</sup>). According to the unique absorption and emission properties, application as luminescent solar concentrators or in horticultural lighting appears promising

    Narrow-Band Yellow-Orange Emitting La<sub>3–<i>x</i></sub>Ca<sub>1.5<i>x</i></sub>Si<sub>6</sub>N<sub>11</sub>:Eu<sup>2+</sup> (<i>x</i> ≈ 0.77): A Promising Phosphor for Next-Generation Amber pcLEDs

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    The nitridosilicate La<sub>3–<i>x</i></sub>Ca<sub>1.5<i>x</i></sub>Si<sub>6</sub>N<sub>11</sub>:Eu<sup>2+</sup> (<i>x</i> ≈ 0.77) was synthesized in a radiofrequency furnace starting from LaF<sub>3</sub>, La­(NH<sub>2</sub>)<sub>3</sub>, CaH<sub>2</sub>, Si­(NH)<sub>2</sub>, and EuF<sub>3</sub>. The crystal structure was solved and refined from single-crystal X-ray data in the tetragonal space group <i>P</i>4<i>bm</i> (no. 100) with <i>a</i> = 10.1142(6), <i>c</i> = 4.8988(3) Å, and <i>Z</i> = 2. Thereby, the so far unknown charge balance mechanism in the system (La,Ca)<sub>3</sub>Si<sub>6</sub>N<sub>11</sub>, which is necessary as bivalent Ca<sup>2+</sup> substitutes trivalent La<sup>3+</sup>, was clarified. Accordingly, charge balance is achieved by incorporation of Ca<sup>2+</sup> on three cation sites, including an additional third site compared to the homeotypic La<sub>3</sub>Si<sub>6</sub>N<sub>11</sub> structure type. The results are supported by Rietveld refinement on powder X-ray diffraction data as well as energy-dispersive X-ray spectroscopy. Fourier transform infrared spectroscopy indicates absence of N–H bonds. An optical band gap of ≈ 4.0 eV was determined using UV/vis reflectance spectroscopy. The Eu<sup>2+</sup> doped compound exhibits a remarkably narrow emission in the yellow-orange spectral range (λ<sub>em</sub> ≈ 587 nm, fwhm ≈ 60 nm/1700 cm<sup>–1</sup>). Because of the intriguing yellow-orange luminescence, La<sub>3–<i>x</i></sub>Ca<sub>1.5<i>x</i></sub>Si<sub>6</sub>N<sub>11</sub>:Eu<sup>2+</sup> (<i>x</i> ≈ 0.77) is a promising candidate for application in next-generation amber phosphor-converted light emitting diodes

    Direct Measurements of Energy Levels and Correlation with Thermal Quenching Behavior in Nitride Phosphors

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    Highly efficient narrow-band red emitting (RE) phosphors are the most desired and requested materials for developing illumination grade phosphor-converted light emitting diodes (pcLEDs). This study presents direct measurements of RE energy levels, critical to the color and efficiency of LED phosphors. For the first time, we experimentally determine the energetic separation of the Eu 5d state and the conduction band, which is the key indicator of quantum efficiency. This was achieved for the next-generation pcLED phosphors Li<sub>2</sub>Ca<sub>2</sub>[Mg<sub>2</sub>Si<sub>2</sub>N<sub>6</sub>]:Eu<sup>2+</sup>, Ba­[Li<sub>2</sub>(Al<sub>2</sub>Si<sub>2</sub>)­N<sub>6</sub>]:Eu<sup>2+</sup>, and Sr­[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup> using resonant inelastic X-ray scattering. Band to band and 4f to valence band transitions are directly observed in X-ray excited optical luminescence spectra of Sr­[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup> and Sr­[Mg<sub>3</sub>SiN<sub>4</sub>]:Eu<sup>2+</sup>. These techniques are widely applicable and create a comprehensive, experimental picture of the Eu<sup>2+</sup> energy levels in these compounds, leading to a complete understanding of all pertinent electronic processes. This study forms the base needed for a detailed discussion of the structure–property relationships, such as specific atoms, coordination and density of states, underpinning phosphor color and efficiency

    Luminescence of the Narrow-Band Red Emitting Nitridomagnesosilicate Li<sub>2</sub>(Ca<sub>1–<i>x</i></sub>Sr<sub><i>x</i></sub>)<sub>2</sub>[Mg<sub>2</sub>Si<sub>2</sub>N<sub>6</sub>]:Eu<sup>2+</sup> (<i>x</i> = 0–0.06)

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    The nitridomagnesosilicates Li<sub>2</sub>Ca<sub>2</sub>[Mg<sub>2</sub>Si<sub>2</sub>N<sub>6</sub>]:Eu<sup>2+</sup> and Li<sub>2</sub>(Ca<sub>1.88</sub>Sr<sub>0.12</sub>)­[Mg<sub>2</sub>Si<sub>2</sub>N<sub>6</sub>]:Eu<sup>2+</sup> show narrow-band red emission at 638 and 634 nm, respectively, with an emission bandwidth of 62 nm (∼1513 cm<sup>–1</sup>) after excitation in the blue spectral region. Ce<sup>3+</sup>-doped samples show luminescence in the green spectral range (λ<sub>em</sub> = 540 nm). The compounds were synthesized via solid-state metathesis reaction in Li melts. Refinement of single-crystal X-ray diffraction data revealed that Li<sub>2</sub>(Ca<sub>1.88</sub>Sr<sub>0.12</sub>)­[Mg<sub>2</sub>Si<sub>2</sub>N<sub>6</sub>] crystallizes isomorphic to Li<sub>2</sub>Ca<sub>2</sub>[Mg<sub>2</sub>Si<sub>2</sub>N<sub>6</sub>]: <i>C</i>2/<i>m</i> [<i>Z</i> = 2, <i>a</i> = 5.5744(2), <i>b</i> = 9.8439(3), <i>c</i> = 6.0170(2) Å, β = 97.2520(10)°, <i>R</i><sub>1</sub> = 0.021, <i>wR</i><sub>2</sub> = 0.047]. Crystal composition was checked by EDS and ICP-OES measurements and luminescence properties are compared to state of the art narrow-band red emitting luminophors. On the basis of its narrow-band emission, application of the novel red luminophor in high CRI white pcLEDs is promising

    Ca<sub>18.75</sub>Li<sub>10.5</sub>[Al<sub>39</sub>N<sub>55</sub>]:Eu<sup>2+</sup>î—¸Supertetrahedron Phosphor for Solid-State Lighting

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    Highly efficient red-emitting luminescent materials deliver the foundation for next-generation illumination-grade white light-emitting diodes (LEDs). Recent studies demonstrate that the hardly explored class of nitridoaluminates comprises intriguing phosphor materials, e.g., Sr­[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup> or Ca­[LiAl<sub>3</sub>N<sub>4</sub>]:Eu<sup>2+</sup>. Here, we describe the novel material Ca<sub>18.75</sub>Li<sub>10.5</sub>[Al<sub>39</sub>N<sub>55</sub>]:Eu<sup>2+</sup> with highly efficient narrow-band red emission (λ<sub>em</sub> ≈ 647 nm, full width at half-maximum, fwhm ≈ 1280 cm<sup>–1</sup>). This compound features a rather uncommon crystal structure, comprising sphalerite-like T<sub>5</sub> supertetrahedra that are composed of tetrahedral AlN<sub>4</sub> units that are interconnected by additional AlN<sub>4</sub> moieties. The network charge is compensated by Ca<sup>2+</sup> and Li<sup>+</sup> ions located between the supertetrahedra. The crystal structure was solved and refined from single-crystal and powder X-ray diffraction data in the cubic space group <i>Fd</i>3̅<i>m</i> (No. 227) with <i>a</i> = 22.415(3) Å and <i>Z</i> = 8. To verify the presence of Li, transmission electron microscopy (TEM) investigations including electron energy-loss spectroscopy (EELS) were performed. Based on the intriguing luminescence properties, we proclaim high potential for application in high-power phosphor-converted white LEDs

    Efficient Yellow-Orange Phosphor Lu<sub>4</sub>Ba<sub>2</sub>[Si<sub>9</sub>ON<sub>16</sub>]O:Eu<sup>2+</sup> and Orange-Red Emitting Y<sub>4</sub>Ba<sub>2</sub>[Si<sub>9</sub>ON<sub>16</sub>]O:Eu<sup>2+</sup>: Two Oxonitridosilicate Oxides with Outstanding Structural Variety

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    The oxonitridosilicate oxides Y<sub>4</sub>Ba<sub>2</sub>[Si<sub>9</sub>ON<sub>16</sub>]­O:Eu<sup>2+</sup> and Lu<sub>4</sub>Ba<sub>2</sub>[Si<sub>9</sub>ON<sub>16</sub>]­O:Eu<sup>2+</sup> have been synthesized starting from <i>RE</i>F<sub>3</sub>, <i>RE</i><sub>2</sub>O<sub>3</sub> (<i>RE</i> = Y, Lu), BaH<sub>2</sub>, Si­(NH)<sub>2</sub>, and EuF<sub>3</sub> in a radiofrequency furnace at 1550 °C. The crystal structures were solved and refined from single-crystal X-ray data supported with Rietveld refinement on X-ray powder diffraction data. Both compounds are isotypic and crystallize in monoclinic space group <i>P</i>2<sub>1</sub>/<i>c</i> (no. 14) with <i>Z</i> = 4 and <i>a</i> = 6.0756(2), <i>b</i> = 27.0606(9), <i>c</i> = 9.9471(3) Å, and β = 91.0008(8)° for <i>RE</i> = Y and <i>a</i> = 6.0290(3), <i>b</i> = 26.7385(12), <i>c</i> = 9.8503(5) Å, and β = 90.7270(30)° for <i>RE</i> = Lu. The unique crystal structure exhibits a three-dimensional network made up from Q<sup>4</sup>-type SiN<sub>4</sub> and Q<sup>3</sup>-type SiON<sub>3</sub> tetrahedra. Containing 4-fold bridging N<sup>[4]</sup> atoms in star-shaped units [N<sup>[4]</sup>(SiN<sub>3</sub>)<sub>4</sub>] next to N<sup>[3]</sup>, N<sup>[2]</sup>, O<sup>[1]</sup>, and noncondensed oxide ions, the title compounds illustrate the vast structural variety in (oxo)­nitridosilicates. Under excitation with UV to blue light, Y<sub>4</sub>Ba<sub>2</sub>[Si<sub>9</sub>ON<sub>16</sub>]­O:Eu<sup>2+</sup> shows emission in the orange-red spectral range (λ<sub>max</sub> = 622 nm, full width at half-maximum (fwhm) ≈ 2875 cm<sup>–1</sup>). Yellow-orange emitting Lu<sub>4</sub>Ba<sub>2</sub>[Si<sub>9</sub>ON<sub>16</sub>]­O:Eu<sup>2+</sup> (λ<sub>max</sub> = 586 nm, fwhm ≈ 2530 cm<sup>–1</sup>) exhibits high internal quantum efficiency (IQE) ≈ 85%. This makes Lu<sub>4</sub>Ba<sub>2</sub>[Si<sub>9</sub>ON<sub>16</sub>]­O:Eu<sup>2+</sup> a promising phosphor for low color rendering index (CRI) warm white phosphor converted light emitting diodes (pcLEDs)

    Narrow-Band Green Emitting Nitridolithoalumosilicate Ba[Li<sub>2</sub>(Al<sub>2</sub>Si<sub>2</sub>)N<sub>6</sub>]:Eu<sup>2+</sup> with Framework Topology <i>whj</i> for LED/LCD-Backlighting Applications

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    Eu<sup>2+</sup>- as well as Ce<sup>3+</sup>-doped Ba­[Li<sub>2</sub>(Al<sub>2</sub>Si<sub>2</sub>)­N<sub>6</sub>] and its related Mg-substituted compounds Ba­[(Mg<sub>2–<i>x</i></sub>Li<sub><i>x</i></sub>) (Al<sub>4–<i>x</i></sub>Si<sub><i>x</i></sub>)­N<sub>6</sub>]:Eu<sup>2+</sup> (<i>x</i> = 0–2) with <i>x</i> = 1.6, 1.8 have been synthesized by metathesis reactions in tantalum ampules. Crystal structures were solved and refined from single-crystal X-ray diffraction data. All three compounds crystallize in tetragonal space group <i>P</i>4/<i>ncc</i> (no. 130) (<i>Z</i> = 4, Ba­[Li<sub>2</sub>(Al<sub>2</sub>Si<sub>2</sub>)­N<sub>6</sub>]:Eu<sup>2+</sup>: <i>a</i> = 7.8282(4), <i>c</i> = 9.9557(5) Å, <i>R</i>1 = 0.0144, <i>wR</i>2 = 0.0366). Their crystal structures, exhibiting the novel framework topology <i>whj</i>, consist of a highly condensed anionic tetrahedra network of disordered (Li/Mg)­N<sub>4</sub> and (Al/Si)­N<sub>4</sub> units connected to each other by common edges and corners. The degree of condensation (i.e., atomic ratio (Al,Li,Mg,Si):N) is κ = 1. The Ba<sup>2+</sup>-position is coordinated eight-fold by N<sup>3–</sup> in form of a truncated square pyramid. Upon doping with Eu<sup>2+</sup>, narrow-band emission in the green to yellow spectral range is observed (λ<sub>em</sub> = 532–562 nm, fwhm ≈ 1962 cm<sup>–1</sup>). Ce<sup>3+</sup>-doped crystals of Ba­[Li<sub>2</sub>(Al<sub>2</sub>Si<sub>2</sub>)­N<sub>6</sub>] show blue emission (λ<sub>em</sub> = 468; 507 nm). According to the tunability of the narrow-band green emission, application in LED-backlight liquid crystal displays appears promising

    Luminescence of an Oxonitridoberyllate: A Study of Narrow-Band Cyan-Emitting Sr[Be<sub>6</sub>ON<sub>4</sub>]:Eu<sup>2+</sup>

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    Oxo- and (oxo)­nitridoberyllates show exceptional potential as host lattices for application in illumination grade phosphor converted (pc)­LEDs due to their remarkable electronic and structural characteristics, allowing highly efficient narrow-band emission upon doping with Eu<sup>2+</sup>. Sr­[Be<sub>6</sub>ON<sub>4</sub>]:Eu<sup>2+</sup>, the first example of an oxonitridoberyllate phosphor, exhibits narrow-band cyan emission (λ<sub>em</sub> = 495 nm; full width at half-maximum, fwhm = 35 nm; ≈1400 cm<sup>–1</sup>), comparable to the emission of the oxonitridosilicate BaSi<sub>2</sub>O<sub>2</sub>N<sub>2</sub>:Eu<sup>2+</sup> (fwhm = 35 nm) or a cyan-emitting primary LED (fwhm = 27 nm). Sr­[Be<sub>6</sub>ON<sub>4</sub>]:Eu<sup>2+</sup> reveals a highly condensed rigid 3D network with a remarkably large degree of condensation [i.e., atomic ratio Be:(O,N)] of κ = 1.2 that is achieved by interconnection of highly condensed layers of BeN<sub>4</sub> tetrahedra by Be<sub>2</sub>ON<sub>6</sub> units via common edges. The crystal structure of Sr­[Be<sub>6</sub>ON<sub>4</sub>]:Eu<sup>2+</sup> was solved on the basis of single-crystal and powder XRD data (<i>C</i>2/<i>c</i>, no. 15, <i>a</i> = 13.9283(14), <i>b</i> = 5.7582(6), <i>c</i> = 4.9908(5) Å, β = 90.195(1)°, <i>Z</i> = 4, <i>R</i><sub>1</sub> = 0.033, <i>wR</i><sub>2</sub> = 0.065, GoF = 1.046). Sr­[Be<sub>6</sub>ON<sub>4</sub>]:Eu<sup>2+</sup> shows a close structural relationship to other nitride as well as oxide compounds, and therefore closes a structural gap helping to understand relations in Be-containing solid-state materials. The electronic structure of Sr­[Be<sub>6</sub>ON<sub>4</sub>]:Eu<sup>2+</sup> was characterized by X-ray spectroscopy measurements, supported by density functional theory (DFT) calculations. Due to its excellent emission properties, large band gap, rigid 3D network, as well as chemical and thermal stability, Sr­[Be<sub>6</sub>ON<sub>4</sub>]:Eu<sup>2+</sup> is a promising phosphor to close the cyan gap in efficient high-CRI pcLEDs (CRI, color rendering index)
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