Abstract:A method for in situ Al 2 O 3 incorporation into a Cu 2 ZnSn(S,Se) 4 (CZTSSe) absorber and its effect on solar cell performance is reported. Al 2 O 3 -incorporated CZTSSe films can be prepared by spraying a precursor solution containing Al metal salt dissolved together with Cu, Zn, and Sn metal salts and thiourea. X-ray photoemission spectroscopy (XPS) and field-emission transmission electron microscopy (FESEM) reveal the existence of an Al 2 O 3 phase in the CZTSSe film. X-ray diffraction (XRD) and Raman spec… Show more
“…[ 17 ] The O 2− induced by Al 2 O 3 on the surface could attract positively charged interstitial Na + . [ 12 ] After AS treatment, the peak intensity of O 2− and Se 4+ decreased significantly, which indicates the further cleaning effect of the CZTSSe surface by the AS treatment. The increased intensity of the S 2p peak after AS treatment indicates S incorporation and/or adsorption on the surface of the absorber (Figure 5f), which is considered as further passivation of the film surface.…”
Section: Resultsmentioning
confidence: 99%
“…With such method, the defect level and defect density were tailored. [ 12 ] Furthermore, our group prepared ultrathin Al 2 O 3 by the ALD on the precursor film before the selenization process. After optimizing the thickness of the Al 2 O 3 , the V OC deficit was reduced from 0.621 to 0.577 V. [ 13 ] Additionally, Hao's group systematically clarified the relationship between ALD‐Al 2 O 3 on the absorber layer and the improvement in V OC , which is accredited to the hydrogen from the ALD process and the homogeneous passivation layer on the surface of CZTS absorber.…”
Increasing the fill factor (FF) and the open‐circuit voltage (VOC) simultaneously together with non‐decreased short‐circuit current density (JSC) are a challenge for highly efficient Cu2ZnSn(S,Se)4 (CZTSSe) solar cells. Aimed at such target in CZTSSe solar cells, a synergistic strategy to tailor the recombination in the bulk and at the heterojunction interface has been developed, consisting of atomic‐layer deposited aluminum oxide (ALD‐Al2O3) and (NH4)2S treatment. With this strategy, deep‐level CuZn defects are converted into shallower VCu defects and improved crystallinity, while the surface of the absorber is optimized by removing Zn‐ and Sn‐related impurities and incorporating S. Consequently, the defects responsible for recombination in the bulk and at the heterojunction interface are effectively passivated, thereby prolonging the minority carrier lifetime and increasing the depletion region width, which promote carrier collection and reduce charge loss. As a consequence, the VOC deficit decreases from 0.607 to 0.547 V, and the average FF increases from 64.2% to 69.7%, especially, JSC does not decrease. Thus, the CZTSSe solar cell with the remarkable efficiency of 13.0% is fabricated. This study highlights the increased FF together with VOC simultaneously to promote the efficiency of CZTSSe solar cells, which could also be applied to other photoelectronic devices.
“…[ 17 ] The O 2− induced by Al 2 O 3 on the surface could attract positively charged interstitial Na + . [ 12 ] After AS treatment, the peak intensity of O 2− and Se 4+ decreased significantly, which indicates the further cleaning effect of the CZTSSe surface by the AS treatment. The increased intensity of the S 2p peak after AS treatment indicates S incorporation and/or adsorption on the surface of the absorber (Figure 5f), which is considered as further passivation of the film surface.…”
Section: Resultsmentioning
confidence: 99%
“…With such method, the defect level and defect density were tailored. [ 12 ] Furthermore, our group prepared ultrathin Al 2 O 3 by the ALD on the precursor film before the selenization process. After optimizing the thickness of the Al 2 O 3 , the V OC deficit was reduced from 0.621 to 0.577 V. [ 13 ] Additionally, Hao's group systematically clarified the relationship between ALD‐Al 2 O 3 on the absorber layer and the improvement in V OC , which is accredited to the hydrogen from the ALD process and the homogeneous passivation layer on the surface of CZTS absorber.…”
Increasing the fill factor (FF) and the open‐circuit voltage (VOC) simultaneously together with non‐decreased short‐circuit current density (JSC) are a challenge for highly efficient Cu2ZnSn(S,Se)4 (CZTSSe) solar cells. Aimed at such target in CZTSSe solar cells, a synergistic strategy to tailor the recombination in the bulk and at the heterojunction interface has been developed, consisting of atomic‐layer deposited aluminum oxide (ALD‐Al2O3) and (NH4)2S treatment. With this strategy, deep‐level CuZn defects are converted into shallower VCu defects and improved crystallinity, while the surface of the absorber is optimized by removing Zn‐ and Sn‐related impurities and incorporating S. Consequently, the defects responsible for recombination in the bulk and at the heterojunction interface are effectively passivated, thereby prolonging the minority carrier lifetime and increasing the depletion region width, which promote carrier collection and reduce charge loss. As a consequence, the VOC deficit decreases from 0.607 to 0.547 V, and the average FF increases from 64.2% to 69.7%, especially, JSC does not decrease. Thus, the CZTSSe solar cell with the remarkable efficiency of 13.0% is fabricated. This study highlights the increased FF together with VOC simultaneously to promote the efficiency of CZTSSe solar cells, which could also be applied to other photoelectronic devices.
“…The full device structure was then completed with the deposition of i-ZnO (∼50 nm) and tin-doped indium oxide (ITO) (∼300 nm) layers by radio frequency (RF) magnetron sputtering. Detailed information on the buffer and window layer fabrication processes can be found elsewhere. ,,− No additional antireflection coatings were applied to the fabricated devices. For measurement of device performance, we mechanically scribed the cell with an area of 0.20 cm 2 .…”
Section: Methodsmentioning
confidence: 99%
“…With air annealing, they obtained improved crystallinity of the CISSe absorber without carbon residue near the bottom electrode, which enabled a PCE of more than ∼14%. But, all device parameters, V oc , short-circuit current density ( J sc ), and fill factor ( FF ), were lower compared to the devices made by using a vacuum-based process. ,, We have developed spray pyrolysis with deionized water (DIW) for Cu(In,Ga)(S,Se) 2 (CIGSSe) solar cells. ,,− DIW is the most eco-friendly, low-cost solvent, and it does not retain any kind of carbon residue in the fabricated absorber, which is usually observed when using organic solvents and can be a possible limitation to device performance. In addition, alkali doping/alloying is easily achievable by spraying an alkali-dissolved aqueous solution. , For the narrow band gap solar cells ( E g = ∼1.1 eV) on a flexible SUS substrate, spraying Na/K codissolved Cu-In-Ga-S precursor solution in an air environment (in situ alkali doping/alloying) provides a PCE of 11.45% …”
The chalcopyrite Cu(In,Ga)(S,Se) 2 (CIGSSe) solar cell with a low band gap is a promising candidate for use as the bottom cell in high-efficiency tandem solar cells. In this study, we investigated narrow band gap CIGSSe solar cells, both with and without alkali treatment. The CIGSSe absorbers were fabricated using aqueous spray pyrolysis in an air environment, with the precursor solution prepared by dissolving constituent metal salts. We found that the power conversion efficiency (PCE) of the fabricated solar cell was significantly enhanced when rubidium postdeposition treatment (PDT) was applied to the CIGSSe absorber. The Rb-PDT facilitates defect passivation and a downshift of the valence band maximum of the CIGSSe absorber, thereby improving the power conversion efficiency and all device parameters. Due to these beneficial effects, a PCE of ∼15% was obtained with an energy band gap of less than 1.1 eV, making it suitable for use as the bottom cell in a highly efficient tandem solar cell.
“…Furthermore, the HCell-MoSe 2 :V exhibits nonlinear V OC -T characteristics from %110 K, which is much lower than HCell-Ref (%160 K), which implies HCell-MoSe 2 :V has a lower back contact barrier. [45,46] Meanwhile, it is well known that the presence of a cross-over point between the light and dark J-V curves indicates the presence of a back contact barrier [47,48] and the higher current density corresponding to the intersection points means the lower back contact barrier height. From Figure 9d, the current density corresponding to the cross-over point is increased from 65.03 to 123.99 mA cm À2 after V is incorporated into Mo and MoSe 2 films, indicating that HCell-MoSe 2 :V has a lower back contact barrier.…”
Section: Device Performances and Carrier Transport Mechanism At Back ...mentioning
One of the key issues impeding the enhancement of power conversion efficiency (PCE) of Cu2ZnSn(S,Se)4 (CZTSSe) solar cells is the severe carrier recombination at CZTSSe/MoSe2 back interface, primarily arising from the reverse electric field formed between CZTSSe and n‐type MoSe2 produced after selenization. To inhibit recombination at back interface, herein, the MoSe2 layer is converted from n‐type to p‐type by V doping in site through reaction of V‐alloyed Mo (Mo:V) back electrode with Se during selenization, and CZTSSe solar cells with p+‐type V‐doped MoSe2 (MoSe2:V) interface layer are fabricated. It is found that the PCE of the device rises from 8.34% to 9.63% as back contact changes from soda lime glass (SLG)/Mo/n‐MoSe2 to SLG/Mo:V/p+‐MoSe2:V. The quantitative analysis demonstrates that the increased PCE predominantly originated from the decreased reverse saturated current density (J0), followed by the decreased series resistance (RS), and lastly by the increased photogenerated current density (JL). The influence mechanism of the SLG/Mo:V/MoSe2:V back contact on device performance is suggested by studying the properties of Mo:V and MoSe2:V films and CZTSSe/MoSe2:V heterojunction. This work emphasizes the vital significance of the back surface passivation field induced by p+‐MoSe2:V/p‐CZTSSe heterojunction, which is enlightening for optimizing the back contact in kesterite photovoltaics.
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