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Influences of Low Intensity on Diode Parameters of CdTe Solar Cells

This study deals with the CdS/CdTe solar cells under low illumination intensity, with cell #1 for the shunt resistance exceeding 100,000 Ω·cm(2) and cell #2 for the shunt resistance above 1000 Ω·cm(2). The diode parameter variations with the decline of the irradiance intensity are illustrated by div...

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Detalles Bibliográficos
Autores principales: Xu, Xiaobo, Gu, Wenping, Wang, Xiaoyan, Zhu, Wei, Zhang, Lin, Zhang, Zan
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7254389/
https://www.ncbi.nlm.nih.gov/pubmed/32397646
http://dx.doi.org/10.3390/ma13092194
Descripción
Sumario:This study deals with the CdS/CdTe solar cells under low illumination intensity, with cell #1 for the shunt resistance exceeding 100,000 Ω·cm(2) and cell #2 for the shunt resistance above 1000 Ω·cm(2). The diode parameter variations with the decline of the irradiance intensity are illustrated by dividing 0–100 mW/cm(−2) into a number of small intensity ranges for J–V measurements and assuming the diode parameters to be constant within each range, the diode parameters of each range including the series resistance, the shunt resistance, the reverse saturation current density and the ideality factor are then extracted by employing an analytical approach. The mechanism of the cell performance deviations are also investigated by basic theories, reports and experiments. For cell #1 with higher R(sh) corresponding to less traps, R(sh) shows a upward tendency as the irradiance declines, n and J(0) exhibit a rise with the irradiance and keep nearly unchanged at the low irradiance values mainly due to recombination and carrier contributions, R(s) shows a slight increase when the irradiance intensity goes down because of the resistance of CdTe absorption layer. For cell #2 with lower R(sh) corresponding to more traps, with the decrease of the illumination intensity, R(sh) increases sharply only for captured carrier reduction, R(s) goes steadily up similarly, n and J(0) exhibit a decline with the irradiance due to recombination shift. It should be pointed out that R(s) varies much smoother than the traditional approximation of a reciprocal of differential at short circuit, and the distribution of R(sh) is diverse, and an average R(sh) of for each intensity range can reflect the variation trend.