2020
DOI: 10.1016/j.jallcom.2020.154964
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Silicon-based electroluminescent polycrystalline Er-doped Yb3Al5O12 nanofilms fabricated by atomic layer deposition

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Cited by 15 publications
(17 citation statements)
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“…The higher Lu/Ga ratios equate to lower Er/Lu concentrations, which further disperse Er dopants in the nanolaminates and contribute to the suppression of cross-relaxation among Er 3+ ions. Additionally, the values of EL lifetime and efficiencies are close to that of YGG:Er MOSLEDs in our previous work, and the optimal EL decay lifetime for the gallium garnet nanofilms (2.2–2.5 ms) is much longer than that for the aluminum garnets (1.2–1.8 ms), beneficial for laser applications. …”
Section: Resultssupporting
confidence: 82%
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“…The higher Lu/Ga ratios equate to lower Er/Lu concentrations, which further disperse Er dopants in the nanolaminates and contribute to the suppression of cross-relaxation among Er 3+ ions. Additionally, the values of EL lifetime and efficiencies are close to that of YGG:Er MOSLEDs in our previous work, and the optimal EL decay lifetime for the gallium garnet nanofilms (2.2–2.5 ms) is much longer than that for the aluminum garnets (1.2–1.8 ms), beneficial for laser applications. …”
Section: Resultssupporting
confidence: 82%
“…The compositions and doping levels of these LuGG:Er MOSLEDs are adjusted by tuning the deposition cycle of Lu 2 O 3 interlayers to optimize the EL performance. Each Lu 2 O 3 interlayer was inserted with two Er 2 O 3 cycles, which has been certified to be the optimal recipe in previous reports. Figure shows the EL spectra under different injection currents, from the amorphous and crystalline LuGG:Er MOSLEDs (Lu/Ga = 0.59, 1.0 nm Ga 2 O 3 interlayers) after annealing at 700 and 800 °C, respectively. The peak of the main emissions from the crystallized LuGG:Er device is located at 1529 nm, accompanied with several discrete peaks at ∼1465, 1569, and 1624 nm.…”
Section: Resultsmentioning
confidence: 99%
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“…Similar phenomena corresponding to the crystallinity of other garnets have been reported previously, which also results from the modification on the crystal field around the doped RE ions by changes in the local lattice structure. [40][41][42][43] The broad EL peaks at 1466 and 1620 nm are assigned to 3 H 11/2 → 4 I 9/2 and 3 I 9/2 → 4 I 13/2 electric-dipole transitions, while the sharp bands at 1530 and 1566 nm are regarded as the 3 I 13/2 → 4 I 15/2 and 3 S 3/2 → 4 I 9/2 magnetic-dipole transitions of Er 3+ ions, respectively. [44][45][46][47] Fig.…”
Section: Resultsmentioning
confidence: 99%