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Ga(2)Se(3) Defect Semiconductors: The Study of Direct Band Edge and Optical Properties
[Image: see text] Direct band edge is a crucial factor for a functional chalcogenide to be applied in luminescence devices, photodetectors, and solar-energy devices. In this work, the room-temperature band-edge emission of III–VI Ga(2)Se(3) has been first observed by micro-photoluminescence (μPL) me...
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2020
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7392520/ https://www.ncbi.nlm.nih.gov/pubmed/32743231 http://dx.doi.org/10.1021/acsomega.0c02623 |
Sumario: | [Image: see text] Direct band edge is a crucial factor for a functional chalcogenide to be applied in luminescence devices, photodetectors, and solar-energy devices. In this work, the room-temperature band-edge emission of III–VI Ga(2)Se(3) has been first observed by micro-photoluminescence (μPL) measurement. The emission peak is at 1.85 eV, which matches well with the band-edge transition that is measured by micro-thermoreflectance (μTR) and micro-transmittance (μTransmittance) for verification of the direct band edge of Ga(2)Se(3). The temperature-dependent μTR spectra of Ga(2)Se(3) show a general semiconductor behavior with its temperature-energy shift following Varshni-type variation. With the well-evident direct band edge, the peak responsivities of photovoltaic response (∼6.2 mV/μW) and photocurrent (∼2.25 μA/μW at f = 30 Hz) of defect zincblende Ga(2)Se(3) can be, respectively, detected at ∼2.22 and ∼1.92 eV from a Cu/Ga(2)Se(3) Schottky solar cell and a Ga(2)Se(3) photoconductor. On the basis of experimental analysis, the optical band edge and photoresponsivity properties of a III–VI Ga(2)Se(3) defect semiconductor are thus realized. |
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