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Enhancement of photoluminescence intensity by photoinduced interdiffusion in nanolayered a-Se∕As2S3 films

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Optical parameters of chalcogenide glass multilayers with 12–15nm modulation lengths prepared by thermal evaporation can be changed by laser irradiation. Photoluminescence (PL) studies were carried out on such nonirradiated and irradiated multilayered samples of a-Se∕As2S3 (sublayer thickness of a-Se is 4–5nm for one set of samples and 1–2nm for the other set. However As2S3 sublayer thickness is 11–12nm for both sets of samples.) PL intensity can be increased by several orders of magnitude by reducing the Se well layer (lower band gap) thickness and can be further increased by irradiating the samples with appropriate wavelengths in the range of the absorption edge. The broadening of luminescence bands takes place either with a decrease in Se layer thickness or with irradiation. The former is due to the change in interface roughness and defects because of the enhanced structural disorder while the latter is due to photoinduced interdiffusion. The photoinduced interdiffusion creates defects at the interface between Se and As2S3 by forming an As–Se–S solid solution. From the deconvoluted PL spectrum, it is shown that the peak PL intensity, full width half maximum, and the PL quantum efficiency of particular defects giving rise to PL, can be tuned by changing the sublayer thickness or by interdiffusion.
Title: Enhancement of photoluminescence intensity by photoinduced interdiffusion in nanolayered a-Se∕As2S3 films
Description:
Optical parameters of chalcogenide glass multilayers with 12–15nm modulation lengths prepared by thermal evaporation can be changed by laser irradiation.
Photoluminescence (PL) studies were carried out on such nonirradiated and irradiated multilayered samples of a-Se∕As2S3 (sublayer thickness of a-Se is 4–5nm for one set of samples and 1–2nm for the other set.
However As2S3 sublayer thickness is 11–12nm for both sets of samples.
) PL intensity can be increased by several orders of magnitude by reducing the Se well layer (lower band gap) thickness and can be further increased by irradiating the samples with appropriate wavelengths in the range of the absorption edge.
The broadening of luminescence bands takes place either with a decrease in Se layer thickness or with irradiation.
The former is due to the change in interface roughness and defects because of the enhanced structural disorder while the latter is due to photoinduced interdiffusion.
The photoinduced interdiffusion creates defects at the interface between Se and As2S3 by forming an As–Se–S solid solution.
From the deconvoluted PL spectrum, it is shown that the peak PL intensity, full width half maximum, and the PL quantum efficiency of particular defects giving rise to PL, can be tuned by changing the sublayer thickness or by interdiffusion.

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