2013
DOI: 10.1016/j.matlet.2013.08.042
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Deposition of earth-abundant p-type CuBr films with high hole conductivity and realization of p-CuBr/n-Si heterojunction solar cell

Abstract: We present details of the deposition of transparent and earth-abundant p-type CuBr films with high hole conductivity and the fabrication and characterization of a prototype solar cell based on p-CuBr/n-Si

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Cited by 24 publications
(17 citation statements)
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“…Therefore, it is important to develop a low‐cost and high‐performance wide‐bandgap material without the lattice mismatch. The earth‐abundant γ‐CuBr with zinc blende structure is naturally a p‐type semiconductor with a wide direct bandgap of ≈3.0 eV, which can be synthesized at a low temperature environment . In addition, the large excitonic binding energy of 108 meV of CuBr, much higher than that of GaN (≈23 meV) and ZnO (≈60 meV), indicates a strong room‐temperature exciton emission and great potential in constructing short wavelength luminescence devices .…”
Section: Comparison Of the Critical Parameters Of Short Wavelength Phmentioning
confidence: 99%
“…Therefore, it is important to develop a low‐cost and high‐performance wide‐bandgap material without the lattice mismatch. The earth‐abundant γ‐CuBr with zinc blende structure is naturally a p‐type semiconductor with a wide direct bandgap of ≈3.0 eV, which can be synthesized at a low temperature environment . In addition, the large excitonic binding energy of 108 meV of CuBr, much higher than that of GaN (≈23 meV) and ZnO (≈60 meV), indicates a strong room‐temperature exciton emission and great potential in constructing short wavelength luminescence devices .…”
Section: Comparison Of the Critical Parameters Of Short Wavelength Phmentioning
confidence: 99%
“…Other interesting works on GICS devices may be found in the literature (Sobayel et al [20], Li et al [21], Farooq et al [22], Sharbati et al [23], Bouchama et al [24], Saifullah et al [25], Mallem et al [26], Ding et al [27], Procel et al [28], Richter et al [29], Tao et al [30], Ok et al [31], Rajani et al [32], Singh et al [33], and Jay et al [34]). They also presented in Table 1.…”
Section: Introductionmentioning
confidence: 99%
“…This configuration is used for a CIGS solar cell. [20] CIGS cell with LDS layer on top [21] CIGS Cell with vs. effective layers [22] AlxGa1-xAs/CIGS tandem cell [23] Superstrate CIGS cell [24] Completed CIGS cell [25] TMO/Si heterojunction solar cell [26] n-type Si PERT bifacial cell [27] p-type c-Si solar cell [28] n-type silicon solar cell [29] TOP-Con silicon solar cell [30] N-type front junction Si solar cell [31] p-CuBr/n-Si heterojunction cell [32] n-type mc-Si screen-printed cell [33] n-type a-Si:H/c-Si heterojunctions [34]…”
Section: Introductionmentioning
confidence: 99%
“…However, the cell still exhibits a high process cost and technical barriers because of its complex structure, despite the fact that it can be fabricated at a rather low temperature (<250 ∘ C) [1,2]. By comparison, the low cost transparent conducting oxide (TCO)/n-Si heterojunction solar cells (HJSCs) are more promising as high-conversion-efficiency and low cost SCs because of the advantages they offer, including a simpler device structure and a lower processing temperature (<250 ∘ C) [3][4][5][6][7][8][9][10][11][12][13]. In 2013, our study [14] proposed that low cost p-type Ni 1− O:Li thin film was a promising material candidate for other TCO materials (such as n-ZnO-base or n-type indium tin oxide (n-ITO)) in HJSCs applications due to the higher work function (>5 eV), which can directly increase the built-in potential ( bi ) and further increase the oc .…”
Section: Introductionmentioning
confidence: 99%