2016
DOI: 10.1016/j.spmi.2016.09.035
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Electronic transport mechanism in intrinsic and doped nanocrystalline silicon films deposited by RF-magnetron sputtering at low temperature

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Cited by 5 publications
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“…The unusual phenomenon where n h and µ h both increase simultaneously can be attributed to the fact that, in polycrystalline samples with high concentration of impurities, the mobility of carrier follows either the percolation model or the variable range hopping model. [ 48 , 49 , 50 ] Furthermore, doping of S atoms is more spontaneous to passivate I − vacancies rather than exchanging I − with S 2− . Nevertheless, doping concentration exceeding 1.5% exhibited µ h decrease to 8.22 cm 2 V −1 s −1 owing to the increase in residual C. Finally, to optimize the annealing temperature, 1.5% NET doped CuI:S thin‐films were annealed at different temperatures (25–200 °C), as shown in Figure 4d .…”
Section: Resultsmentioning
confidence: 99%
“…The unusual phenomenon where n h and µ h both increase simultaneously can be attributed to the fact that, in polycrystalline samples with high concentration of impurities, the mobility of carrier follows either the percolation model or the variable range hopping model. [ 48 , 49 , 50 ] Furthermore, doping of S atoms is more spontaneous to passivate I − vacancies rather than exchanging I − with S 2− . Nevertheless, doping concentration exceeding 1.5% exhibited µ h decrease to 8.22 cm 2 V −1 s −1 owing to the increase in residual C. Finally, to optimize the annealing temperature, 1.5% NET doped CuI:S thin‐films were annealed at different temperatures (25–200 °C), as shown in Figure 4d .…”
Section: Resultsmentioning
confidence: 99%