| Article ID | Journal | Published Year | Pages | File Type |
|---|---|---|---|---|
| 77924 | Solar Energy Materials and Solar Cells | 2015 | 5 Pages |
•The CdTe/Sb2Te3 interface was prepared by co-evaporation on an ultra-thin glass substrate and studied “in-situ” in an ultra-high vacuum using the synchrotron radiation technology.•Band diagrams before and after annealing indicate a thin layer of Sb2Te3 plays a crucial role in forming an ohmic contact to CdTe.•From the point of view of the band diagram of CdTe/Sb2Te3, we proposed a modified CdTe/Sb2Te3 interface, and enhanced device performance on the ultra-thin glass substrates.
The CdTe/Sb2Te3 interface was prepared by co-evaporation on an ultra-thin glass substrate and studied “in-situ” by photoelectron spectroscopy using a tunable synchrotron radiation photon source. The results indicated that the as-deposited antimony telluride was a mixture of Sb–Te phase and Sb2Te3 structure. The band diagram showed a conduction band offset (ΔECB) of 0.65 eV at the interface. A thin layer of Sb2Te3 came into being on the surface of CdTe with a subsequent 300 °C anneal. The sputter depth profile suggested that the annealed interface was actually constituted by the “substrate CdTe/interface Sb+Cd donors/inner Sb–Te mixture/surface Sb2Te3” structure. The band diagram gave ΔECB=1.35 eV for the annealed interface. It was found that there was a thin barrier of 0.2 eV induced by Sb+Cd donors for the hole transportation at the interface. To create a thin p+ layer between CdTe and the back electrode, a 50 Å thick Sb2Te3 layer was used for the back contact to CdTe thin film solar cells. J–V characteristic showed that this thin p+ back contact greatly enhanced the cell performance.
