2021
DOI: 10.35848/1347-4065/ac25da
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Photoluminescence properties of heavily Sb doped Ge1−x Sn x and heterostructure design favorable for n+-Ge1−x Sn x active layer

Abstract: We investigated the photoluminescence (PL) properties of heavily Sb doped n+-Ge1−x Sn x layers and demonstrated the formation of a double heterostructure (DHS) for the n+-Ge1−x Sn x active layer. A single PL peak was observed for n+-Ge1−x Sn x layers thicker than 80 nm with increasing the Sb concentration up to 1020 cm−3, attributed to the… Show more

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Cited by 2 publications
(2 citation statements)
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“…This suggests the carrier confinement and/or the defect termination of Ge 1−x Sn x QDs surface by SiO 2 layer is important to cause the PL emission of the Ge 1−x Sn x QDs as so far reported. 2) Next, we performed PDA for some samples. Figure 8(b) shows the PL spectra of the prepared samples with T PDA of 300 °C-500 °C measured at RT.…”
Section: Optoelectronic Property Of Ge 1−x Snmentioning
confidence: 99%
See 1 more Smart Citation
“…This suggests the carrier confinement and/or the defect termination of Ge 1−x Sn x QDs surface by SiO 2 layer is important to cause the PL emission of the Ge 1−x Sn x QDs as so far reported. 2) Next, we performed PDA for some samples. Figure 8(b) shows the PL spectra of the prepared samples with T PDA of 300 °C-500 °C measured at RT.…”
Section: Optoelectronic Property Of Ge 1−x Snmentioning
confidence: 99%
“…1) However, the E gΓ of the direct transition Ge 1−x Sn x bulk is less than 0.6 eV. To achieve luminescence preferable for the optical interconnect of LSIs, using quantum levels formed by lowering the dimensions of the light-emitting layers such as multi-quantum-wells (MQWs), 2,3) nanowires, 4,5) and QDs [6][7][8] is a feasible approach to realizing high E gΓ . Light sources based on high-density (>10 10 cm −2 ) QDs are particularly promising because of their lower power consumption and greater operational temperature stability compared to MQWs.…”
Section: Introductionmentioning
confidence: 99%