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Defect visualization of Cu(InGa)(SeS)(2) thin films using DLTS measurement

Defect depth profiles of Cu (In(1−x),Ga(x))(Se(1−y)S(y))(2) (CIGSS) were measured as functions of pulse width and voltage via deep-level transient spectroscopy (DLTS). Four defects were observed, i.e., electron traps of ~0.2 eV at 140 K (E1 trap) and 0.47 eV at 300 K (E2 trap) and hole traps of ~0.1...

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Detalles Bibliográficos
Autores principales: Heo, Sung, Chung, JaeGwan, Lee, Hyung-Ik, Lee, Junho, Park, Jong-Bong, Cho, Eunae, Kim, KiHong, Kim, Seong Heon, Park, Gyeong Su, Lee, Dongho, Lee, Jaehan, Nam, Junggyu, Yang, JungYup, Lee, Dongwha, Cho, Hoon Young, Kang, Hee Jae, Choi, Pyung-Ho, Choi, Byoung-Deog
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4967860/
https://www.ncbi.nlm.nih.gov/pubmed/27476672
http://dx.doi.org/10.1038/srep30554
Descripción
Sumario:Defect depth profiles of Cu (In(1−x),Ga(x))(Se(1−y)S(y))(2) (CIGSS) were measured as functions of pulse width and voltage via deep-level transient spectroscopy (DLTS). Four defects were observed, i.e., electron traps of ~0.2 eV at 140 K (E1 trap) and 0.47 eV at 300 K (E2 trap) and hole traps of ~0.1 eV at 100 K (H1 trap) and ~0.4 eV at 250 K (H2 trap). The open circuit voltage (V(OC)) deteriorated when the trap densities of E2 were increased. The energy band diagrams of CIGSS were also obtained using Auger electron spectroscopy (AES), X-ray photoelectron spectroscopy (XPS), and DLTS data. These results showed that the valence band was lowered at higher S content. In addition, it was found that the E2 defect influenced the V(OC) and could be interpreted as an extended defect. Defect depth profile images provided clear insight into the identification of defect state and density as a function of depth around the space charge region.