1995
DOI: 10.1063/1.360175
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Visible electroluminescence from semitransparent Au film/extra thin Si-rich silicon oxide film/p-Si structure

Abstract: Visible electroluminescence (EL) has been reported from semitransparent Au film/extra thin Si-rich silicon oxide film/p-Si diodes at room temperature. The Si-rich silicon oxide films, with thickness of about 40 Å, were grown using the magnetron sputtering technique. At forward bias of 4 V, EL spectra with peak energy of 1.9 eV and full width at half maximum of 0.5 eV can be observed from diodes with such extra thin Si-rich oxide films having not been annealed. EL peak energy shows a small red shift under low f… Show more

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Cited by 128 publications
(22 citation statements)
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“…20 It is more likely originated from luminescent defect centers. [21][22][23] Figure 7 shows the evolution of the integrated PL intensity as a function of the particle density of the Si nanostructures, the PL intensity has a minimum for the sample SO-10 (5 % O 2 ), which corresponds to the lowest particle density (Table 2), the maximum integrated intensity is observed for the sample SO-0 of the highest particle density. This behavior of PL intensity is probably due to the enhancement of the light harvesting efficiency of prepared Si nanostructures with the increase of their particle density.…”
Section: Etching Ratementioning
confidence: 99%
“…20 It is more likely originated from luminescent defect centers. [21][22][23] Figure 7 shows the evolution of the integrated PL intensity as a function of the particle density of the Si nanostructures, the PL intensity has a minimum for the sample SO-10 (5 % O 2 ), which corresponds to the lowest particle density (Table 2), the maximum integrated intensity is observed for the sample SO-0 of the highest particle density. This behavior of PL intensity is probably due to the enhancement of the light harvesting efficiency of prepared Si nanostructures with the increase of their particle density.…”
Section: Etching Ratementioning
confidence: 99%
“…The presence of Ge nanoclusters provides high high-energy excitons, higher than the bulk Ge bandgap energy, and a high density of interface states that lead to PL with band energies higher than the bulk Ge bandgap. This model has been extensively used to explain luminescence properties from Si and Ge nanocluster systems [25][26][27][28][29]. We have noticed that our observed P1 and P2 bands are in similar energy positions to the dislocation centers D1 and D2, to which are attributed the emission lines of 0.808 (D1) and 0.875 (D2) meV [20,30,31].…”
Section: Photoluminescence Of Ge Nanoclustersmentioning
confidence: 67%
“…In the previous work [10,11], it has been suggested that the PL from a-SiNx:H is mainly in three process, i.e., the luminescence from Si nanoparticles, the interface luminescence between silicon and silicon nitride, and gap states luminescence from the imperfection of silicon nitride matrix. Three origins are inherently coexisting in the a-SiNx: H films and the photoluminescence spectrum depends on the contribution of each part.…”
Section: Resultsmentioning
confidence: 99%