TY - JOUR
T1 - Distribution of Copper States, Phases, and Defects across the Depth of a Cu-Doped CdTe Solar Cell
AU - Rojsatien, Srisuda
AU - Mannodi-Kanakkithodi, Arun
AU - Walker, Trumann
AU - Kumar, Niranjana
AU - Nietzold, Tara
AU - Colegrove, Eric
AU - Mao, Dan
AU - Stuckelberger, Michael
AU - Lai, Barry
AU - Cai, Zhonghou
AU - Chan, Maria
AU - Bertoni, Mariana
PY - 2023
Y1 - 2023
N2 - Copper has been used as a p-type dopant in cadmium telluride (CdTe) for decades. However, the density of Cu atoms in the finished device is much higher than that of holes, which means that most Cu atoms are not activated as acceptors during incorporation. Furthermore, studies have demonstrated that the distribution of copper (Cu) atoms across the device is highly inhomogeneous, with reports citing Cu substitution on Cd sites and segregation to grain boundaries. Fast diffusion along these boundaries and Cu accumulation at the CdTe/CdS interface have also been observed and validated computationally. These levels of inhomogeneity make it difficult to accurately characterize and correlate the performance with the nature of the Cu atomic species present. To address this challenge, we utilize X-ray microscopy and, specifically, nanoscale fluorescence-mode X-ray absorption near-edge structure to resolve the atomic Cu environment throughout the depth of the CdTe layer. Our results suggest that the majority of Cu atoms are in the form of CuxTe phases (or similar local environments) near the ZnTe|CdTe interface, CuxO phases in the CdTe absorber, and present in various oxidation states, including Cu1+ and Cu2+, near the CdS/CdTe junction. This work also provides experimental evidence for the first time of the presence of CuS around the ZnTe|CdTe interface and the hypothesized CuCd-Cli complex in the CdTe absorber.
AB - Copper has been used as a p-type dopant in cadmium telluride (CdTe) for decades. However, the density of Cu atoms in the finished device is much higher than that of holes, which means that most Cu atoms are not activated as acceptors during incorporation. Furthermore, studies have demonstrated that the distribution of copper (Cu) atoms across the device is highly inhomogeneous, with reports citing Cu substitution on Cd sites and segregation to grain boundaries. Fast diffusion along these boundaries and Cu accumulation at the CdTe/CdS interface have also been observed and validated computationally. These levels of inhomogeneity make it difficult to accurately characterize and correlate the performance with the nature of the Cu atomic species present. To address this challenge, we utilize X-ray microscopy and, specifically, nanoscale fluorescence-mode X-ray absorption near-edge structure to resolve the atomic Cu environment throughout the depth of the CdTe layer. Our results suggest that the majority of Cu atoms are in the form of CuxTe phases (or similar local environments) near the ZnTe|CdTe interface, CuxO phases in the CdTe absorber, and present in various oxidation states, including Cu1+ and Cu2+, near the CdS/CdTe junction. This work also provides experimental evidence for the first time of the presence of CuS around the ZnTe|CdTe interface and the hypothesized CuCd-Cli complex in the CdTe absorber.
KW - cadmium telluride
KW - copper
KW - photovoltaics
KW - X-ray absorption near-edge structure
KW - XANES
U2 - 10.1021/acs.chemmater.3c01688
DO - 10.1021/acs.chemmater.3c01688
M3 - Article
SN - 0897-4756
VL - 35
SP - 9935
EP - 9944
JO - Chemistry of Materials
JF - Chemistry of Materials
IS - 23
ER -