2022
DOI: 10.1039/d2qi00794k
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Efficient Cr3+-activated NaInP2O7 phosphor for broadband near-infrared LED applications

Abstract: Recently, Cr3+-activated phosphors have garnered attention for broadband near-infrared phosphor converted light-emitting diodes (NIR pc-LEDs) applications, but usually display low efficiency. Herein, we designed and synthesized a novel efficient broadband NIR...

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Cited by 21 publications
(21 citation statements)
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“…The photoluminescence excitation and emission spectra of these compounds are plotted in Figure b,c, respectively. The excitation spectra present two intense bands with peaks located in blue and red regions, which can be assigned to 4 A 2 ( 4 F) → 4 T 1 ( 4 F) and 4 A 2 ( 4 F) → 4 T 2 ( 4 F) transitions of Cr 3+ , respectively . Upon 450 nm excitation, a broadband NIR emission covering 700–1100 nm with emission peaks ranging from 730 to 830 nm can be observed in this family.…”
Section: Resultsmentioning
confidence: 87%
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“…The photoluminescence excitation and emission spectra of these compounds are plotted in Figure b,c, respectively. The excitation spectra present two intense bands with peaks located in blue and red regions, which can be assigned to 4 A 2 ( 4 F) → 4 T 1 ( 4 F) and 4 A 2 ( 4 F) → 4 T 2 ( 4 F) transitions of Cr 3+ , respectively . Upon 450 nm excitation, a broadband NIR emission covering 700–1100 nm with emission peaks ranging from 730 to 830 nm can be observed in this family.…”
Section: Resultsmentioning
confidence: 87%
“…The excitation spectra present two intense bands with peaks located in blue and red regions, which can be assigned to 4 A 2 ( 4 F) → 4 T 1 ( 4 F) and 4 A 2 ( 4 F) → 4 T 2 ( 4 F) transitions of Cr 3+ , respectively. 42 Upon 450 nm excitation, a broadband NIR emission covering 700−1100 nm with emission peaks ranging from 730 to 830 nm can be observed in this family. Comparing the relative emission peak intensity (Figure 1d) indicates that the Y 3 In 1.94 Cr 0.06 Ga 3 O 12 has the highest emission intensity in this family.…”
Section: Computationmentioning
confidence: 89%
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“…There is no apparent absorption from the visible to the NIR for the undoped CLSAS. The optical band gap of the CLSAS host can be calculated according to the Kubelka–Munk equation: [ 32,33 ] F(R)badbreak=(1R)22R\[ \begin{array}{*{20}{c}}{F\left( R \right) = \frac{{{{\left( {1 - R} \right)}^2}}}{{2R}}}\end{array} \] [F(R)×hν]2badbreak=c(hνbadbreak−Eg)\[ \begin{array}{*{20}{c}}{{{\left[ {F\left( R \right) \times h\nu } \right]}^2} = c\left( {h\nu - {E_{\rm{g}}}} \right)}\end{array} \] …”
Section: Resultsmentioning
confidence: 99%
“…There is no apparent absorption from the visible to the NIR for the undoped CLSAS. The optical band gap of the CLSAS host can be calculated according to the Kubelka-Munk equation: [32,33] 1 2…”
Section: Pl Properties Of Clsas:cr 3+mentioning
confidence: 99%