Abstract:The selenization of metallic Cu−Zn−Sn−Ge precursors is a promising route for the fabrication of low-cost and efficient kesterite thin-film solar cells. Nowadays, efficiencies of kesterite solar cells are still below 13%. For Cu(In,Ga)Se 2 solar cells, the formation of compositional gradients along the depth of the absorber layer has been demonstrated to be a key requirement for producing thin-film solar cells with conversion efficiencies above the 22% level. No clear understanding has been reached so far about… Show more
“…The in‐depth compositional grading of group‐III elements (Ga, In) is one of the most useful techniques for high‐performance solar cells with CIGSe, and similar to cation grading of group‐IV elements (Sn, Ge), is expected for CZTGSe under the same analogy . Accordingly, we expect that the solar cell performance of CZTGSe can be further improved by the potential grading of the CBM in CZTGSe by controlling x in depth because the electron affinity of CZTGSe continuously varies with x .…”
mentioning
confidence: 92%
“…Ge‐incorporated Cu 2 Zn(Sn 1– x Ge x )Se 4 (CZTGSe) with kesterite crystal structure has attracted attention as a material for p‐type light absorbers in heterojunction solar cells . This is because the bandgap energy ( E g ) can be tuned from 1.0 to 1.4 eV by adjusting the cationic mixing ratios {Ge/(Ge + Sn) = x } from 0 to 1 .…”
mentioning
confidence: 99%
“…In spite of the importance of developing high‐performance solar cells, the origin of the V OC deficit in kesterite is not yet clear. Especially, although V OC is expected to be affected by the electronic structures at the surface and heterointerface, only a few studies have reported on the band alignment of the CdS/Ge‐incorporated CZTGSe interface and electronic properties of the CZGSe surface . Thus, their systematic accumulation is significantly important for the further improvement of CZTGSe solar cells.…”
This study analyzes the electronic structure of Cu2ZnSn1–xGexSe4 (CZTGSe) surface and band alignments of CdS and CZTGSe using the Ge/(Sn + Ge) composition ratios of x = 0–1 based on inversed, ultraviolet, and X‐ray photoemission spectroscopy. The conduction band offsets of the CdS/CZTGSe interface linearly decrease with increasing x, which are so‐called spike conduction band connections, whereas the valence band offsets are observed to be independent of x. Moreover, the hole density near the CZTGSe surface increases with an increase in x; this corresponds to the increase in the measured built‐in‐potential with x. However, the open circuit voltage (VOC) saturates to ≈0.5 V for x over 0.2 in spite of the favorable band alignment and larger built‐in‐potential of x at the interface. External‐quantum‐efficiency spectral analysis shows that the carrier recombination in CZTGSe bulk is suppressed with an increase in x, whereas the recombination near the CZTGSe surface is enhanced. The relationship between these recombination centers, electronic structure, and saturation of VOC is discussed.
“…The in‐depth compositional grading of group‐III elements (Ga, In) is one of the most useful techniques for high‐performance solar cells with CIGSe, and similar to cation grading of group‐IV elements (Sn, Ge), is expected for CZTGSe under the same analogy . Accordingly, we expect that the solar cell performance of CZTGSe can be further improved by the potential grading of the CBM in CZTGSe by controlling x in depth because the electron affinity of CZTGSe continuously varies with x .…”
mentioning
confidence: 92%
“…Ge‐incorporated Cu 2 Zn(Sn 1– x Ge x )Se 4 (CZTGSe) with kesterite crystal structure has attracted attention as a material for p‐type light absorbers in heterojunction solar cells . This is because the bandgap energy ( E g ) can be tuned from 1.0 to 1.4 eV by adjusting the cationic mixing ratios {Ge/(Ge + Sn) = x } from 0 to 1 .…”
mentioning
confidence: 99%
“…In spite of the importance of developing high‐performance solar cells, the origin of the V OC deficit in kesterite is not yet clear. Especially, although V OC is expected to be affected by the electronic structures at the surface and heterointerface, only a few studies have reported on the band alignment of the CdS/Ge‐incorporated CZTGSe interface and electronic properties of the CZGSe surface . Thus, their systematic accumulation is significantly important for the further improvement of CZTGSe solar cells.…”
This study analyzes the electronic structure of Cu2ZnSn1–xGexSe4 (CZTGSe) surface and band alignments of CdS and CZTGSe using the Ge/(Sn + Ge) composition ratios of x = 0–1 based on inversed, ultraviolet, and X‐ray photoemission spectroscopy. The conduction band offsets of the CdS/CZTGSe interface linearly decrease with increasing x, which are so‐called spike conduction band connections, whereas the valence band offsets are observed to be independent of x. Moreover, the hole density near the CZTGSe surface increases with an increase in x; this corresponds to the increase in the measured built‐in‐potential with x. However, the open circuit voltage (VOC) saturates to ≈0.5 V for x over 0.2 in spite of the favorable band alignment and larger built‐in‐potential of x at the interface. External‐quantum‐efficiency spectral analysis shows that the carrier recombination in CZTGSe bulk is suppressed with an increase in x, whereas the recombination near the CZTGSe surface is enhanced. The relationship between these recombination centers, electronic structure, and saturation of VOC is discussed.
“…CZTS has a high absorption coefficient ( α > 10 4 cm −1 ), direct band gap ( E g ~ 1.5 eV), and p‐type conductivity, which allows for effective absorption of the most incident photons in absorbers with thicknesses of 1 to 2 μm. However, the current efficiency of CZTS‐based solar cells does not exceed 12.6%, because of the short lifetimes of minority charge carriers in the sub‐nanosecond regime . Despite the fact that the maximum possible efficiency of 32% (Shockley‐Queisser limit) for CZTS‐based solar cells has not been reached yet, the significant advances in understanding the functioning problems of photovoltaic devices were achieved.…”
Section: Introductionmentioning
confidence: 99%
“…However, the current efficiency of CZTS-based solar cells does not exceed 12.6%, 4 because of the short lifetimes of minority charge carriers in the sub-nanosecond regime. 5 Despite the fact that the maximum possible efficiency of 32% (Shockley-Queisser limit) for CZTS-based solar cells has not been reached yet, the significant advances in understanding the functioning problems of photovoltaic devices were achieved.…”
The Cu2ZnSnGeS4 (CZTGeS) thin films were deposited by the spray pyrolysis method at different substrate temperatures without further sulfurization. The influence of various deposition temperatures on the surface morphology, microstructure, optical properties, chemical, and phase composition were investigated. The substitution mechanism of Sn/Ge in the crystal lattice of CZTGeS depending on deposition temperatures was studied. It was shown that a variation in substrate temperature has a strong effect on the surface morphology of the films. The X‐ray diffractometer (XRD), transmission electron microscope (TEM), and Raman spectroscopy (RS) analysis showed that CZTGeS films were polycrystalline with a kesterite‐type single‐phase structure and a preferential orientation of (112). The RS‐mapping analysis showed the distribution of intensities on the surfaces of the films. Optical measurements showed that CZTGeS films are highly absorbing in the visible region, and the optical band gap is shifted from 1.89 to 1.84 eV.
Kesterite Cu 2 ZnSn(S,Se) 4 (CZTSSe) has emerged as a promising photovoltaic material not only because of its environmentally benign and earth-abundant constituents, but also its outstanding photoelectronic properties. Unfortunately, the significant open-circuit voltage (V oc ) loss and inferior fill factor (FF) resulting from abundant nonradiative carrier recombination at depletion region has become a major obstacle for further improving device performance. Here, an effective strategy to passivate the deep trap and band-tail states in the heterojunction is proposed, by modifying the CZTSSe absorber layer with GeSe 2 post-deposition treatment. The results reveal that the Ge 4+ can migrate into the front surface of the absorber, which plays an active role in suppressing the Cu Sn deep defects and [2Cu Zn +Sn Zn ] defect clusters, accordingly dramatically reducing severe interfacial nonradiative carrier recombination of CZTSSe photovoltaic device. Under optimal treatment conditions, the CZTSSe solar cell efficiency increases from 10.36% to 12.22%, mainly benefitting from the increasement of V oc and FF.
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