2017
DOI: 10.1364/prj.5.000567
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154  μm photoluminescence enhancenment of Er^3+-doped ZnO films containing nc-Ge: joint effect from Er^3+ local environment changing and energy transfer of nc-Ge

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“…Electroluminescence (EL) from light-emitting devices (LEDs) with erbium (Er)-doped wide band gap semiconductors has been subjected to great effort for years since the emission at ∼1540 nm, which results from the 4 I 13/2 → 4 I 15/2 transition of the Er 3+ ion, is located within the minimum-loss window of silica optical fibers. With a wide band gap of 3.37 eV at 300 K, ZnO is believed to be a desirable matrix for accommodating rare-earth ions that act as luminescent centers. , Over the years, photoluminescence (PL) from diverse Er-doped ZnO (ZnO:Er) materials has been extensively reported. By comparison, the ZnO:Er-related EL has been much less realized. Harako et al realized the visible and ∼1.54 μm EL from a LED based on the n-ZnO:Er/p-Si structure, which arose from the impact-excitation of Er 3+ ions .…”
Section: Introductionmentioning
confidence: 99%
“…Electroluminescence (EL) from light-emitting devices (LEDs) with erbium (Er)-doped wide band gap semiconductors has been subjected to great effort for years since the emission at ∼1540 nm, which results from the 4 I 13/2 → 4 I 15/2 transition of the Er 3+ ion, is located within the minimum-loss window of silica optical fibers. With a wide band gap of 3.37 eV at 300 K, ZnO is believed to be a desirable matrix for accommodating rare-earth ions that act as luminescent centers. , Over the years, photoluminescence (PL) from diverse Er-doped ZnO (ZnO:Er) materials has been extensively reported. By comparison, the ZnO:Er-related EL has been much less realized. Harako et al realized the visible and ∼1.54 μm EL from a LED based on the n-ZnO:Er/p-Si structure, which arose from the impact-excitation of Er 3+ ions .…”
Section: Introductionmentioning
confidence: 99%