Abstract:Toward suppressing the formation of anti-site defects and related defect clusters in kesterite Cu 2 ZnSnS 4−x Se x (CZTS) absorber films, Cu 2 −II−IV−X 4 (II = Sr, Ba; IV = Ge, Sn; X = S, Se) compounds have recently been introduced. Cu 2 BaGe 1−x Sn x Se 4 (CBGTSe) is one of the materials that belongs to this chalcogenide family, with a tunable band gap (1.6 eV ≤ E g ≤ 1.9 eV, based on the x value) having been demonstrated for bulk samples. In this report, we demonstrate the deposition of CBGTSe films and repo… Show more
“…It is noteworthy that such improvement with annealing has also been reported for other copper chalcogenidebased solar cells-that is, CZTS, [40][41][42] CBTSSe, [8] CBGSe, [10] and CBGTSe. [11] The improvement has been attributed to modification of heterojunction properties [40,41] and the passivation of grain boundaries by oxides (e.g., SnO x ). [8,42] J-V and EQE curves for the best-performing postannealed ACBGTSe solar cells are shown in Figure 6, with the corresponding solar cell performance parameters summarized in Table 1.…”
Kesterite Cu 2 ZnSnS 4Àx Se x (CZTS) compounds have been considered as an alternative absorber material for conventional thin-film photovoltaic (PV) materials, CIGS and CdTe. However, substantial concentrations of antisite defects and related defect clusters in CZTS (e.g.
“…It is noteworthy that such improvement with annealing has also been reported for other copper chalcogenidebased solar cells-that is, CZTS, [40][41][42] CBTSSe, [8] CBGSe, [10] and CBGTSe. [11] The improvement has been attributed to modification of heterojunction properties [40,41] and the passivation of grain boundaries by oxides (e.g., SnO x ). [8,42] J-V and EQE curves for the best-performing postannealed ACBGTSe solar cells are shown in Figure 6, with the corresponding solar cell performance parameters summarized in Table 1.…”
Kesterite Cu 2 ZnSnS 4Àx Se x (CZTS) compounds have been considered as an alternative absorber material for conventional thin-film photovoltaic (PV) materials, CIGS and CdTe. However, substantial concentrations of antisite defects and related defect clusters in CZTS (e.g.
“…CBGTSe films ( x = 0.5–0.6) have been prepared by selenizing Cu–Ba–Ge–Sn precursor multilayers that were sequentially deposited using vacuum-based techniques, including both sputtering (for Cu, Ge and Sn) and evaporation (for Ba). 137 Vacuum-deposition of related Cu 2 –II–IV–X 4 films ( i.e. , CBTS, 106,132,138 CBTSSe, 105,139,140 and CSTS 141 ) to yield functioning solar cells has only been demonstrated using the co-sputtering approach.…”
Section: Moving Beyond Cbtssementioning
confidence: 99%
“…, Ba). 142 Kim and Mitzi’s study 137 showed that such issues can be prevented using a high temperature vacuum pre-annealing step to partially homogenize the metallic precursor layer. The CBGTSe films exhibit a PL peak centered at 1.67 eV at room temperature, which is at a lower energy than for CBGSe (1.96 eV), reflecting an ∼0.3 eV bandgap reduction via partial substitution of Ge with Sn.…”
Section: Moving Beyond Cbtssementioning
confidence: 99%
“…CBGTSe lms (x ¼ 0.5-0.6) have been prepared by selenizing Cu-Ba-Ge-Sn precursor multilayers that were sequentially deposited using vacuumbased techniques, including both sputtering (for Cu, Ge and Sn) and evaporation (for Ba). 137 Vacuum-deposition of related Cu 2 -II-IV-X 4 lms (i.e., CBTS, 106,132,138 CBTSSe, 105,139,140 and CSTS 141 ) to yield functioning solar cells has only been demonstrated using the co-sputtering approach. The challenges associated with high quality lm growth from sequential deposition of elemental layers have been attributed in part to issues related to the alkaline earth element (e.g., Ba).…”
Section: Moving Beyond Cbtssementioning
confidence: 99%
“…The challenges associated with high quality lm growth from sequential deposition of elemental layers have been attributed in part to issues related to the alkaline earth element (e.g., Ba). 142 Kim and Mitzi's study 137 showed that such issues can be prevented using a high temperature vacuum pre-annealing step to partially homogenize the metallic precursor layer. The CBGTSe lms exhibit a PL peak centered at 1.67 eV at room temperature, which is at a lower energy than for CBGSe (1.96 eV), reecting an $0.3 eV bandgap reduction via partial substitution of Ge with Sn.…”
The lecture focuses on emerging chalcogenide-based thin-film photovoltaics and provides both an overview of selected absorber candidates that are of recent interest, and a deeper dive into an exemplary Cu2BaSn(S,Se)4-related family.
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