ISSN 0253-2778

CN 34-1054/N

open
Free to Publish. Free to Read.
Open AccessOpen Access JUSTC Chemistry；Engineering & Materials 15 July 2024

Effect of substrate temperature and oxygen plasma treatment on the properties of magnetron-sputtered CdS for solar cell applications

  • Department of Materials Science and Engineering, School of Chemistry and Materials Science, University of Science and Technology of China, Hefei 230026, China

Cite this:
https://doi.org/10.52396/JUSTC-2024-0048
More Information
  • Author Bio:

    Runxuan Zang is currently a master’s student at the University of Science and Technology of China under the supervision of Prof. Tao Chen. His research mainly focuses on the application of magnetron sputtered CdS in antimony chalcogenide solar cells

    Tao Chen is a Professor in the Department of Materials Science and Engineering, University of Science and Technology of China. He received his Ph.D. degree in Chemistry from Nanyang Technological University in 2010. His research mainly focuses on metal chalcogenide solar cells and energy storage materials and devices

  • Corresponding author: E-mail: tchenmse@ustc.edu.cn
  • Received Date: 26 March 2024
  • Accepted Date: 14 May 2024
    • Available Online: 15 July 2024
    Abstract

  • Abstract

    Cadmium sulfide (CdS) is an n-type semiconductor with excellent electrical conductivity that is widely used as an electron transport material (ETM) in solar cells. At present, numerous methods for preparing CdS thin films have emerged, among which magnetron sputtering (MS) is one of the most commonly used vacuum techniques. For this type of technique, the substrate temperature is one of the key deposition parameters that affects the interfacial properties between the target film and substrate, determining the specific growth habits of the films. Herein, the effect of substrate temperature on the microstructure and electrical properties of magnetron-sputtered CdS (MS-CdS) films was studied and applied for the first time in hydrothermally deposited antimony selenosulfide (Sb2(S,Se)3) solar cells. Adjusting the substrate temperature not only results in the design of the flat and dense film with enhanced crystallinity but also leads to the formation of an energy level arrangement with a Sb2(S,Se)3 layer that is more favorable for electron transfer. In addition, we developed an oxygen plasma treatment for CdS, reducing the parasitic absorption of the device and resulting in an increase in the short-circuit current density of the solar cell. This study demonstrates the feasibility of MS-CdS in the fabrication of hydrothermal Sb2(S,Se)3 solar cells and provides interface optimization strategies to improve device performance.

    Graphical abstract

    Under substrate heating conditions, the CdS thin film prepared by magnetron sputtering has a flat and dense morphology with enhanced crystallinity.

    Abstract

    Cadmium sulfide (CdS) is an n-type semiconductor with excellent electrical conductivity that is widely used as an electron transport material (ETM) in solar cells. At present, numerous methods for preparing CdS thin films have emerged, among which magnetron sputtering (MS) is one of the most commonly used vacuum techniques. For this type of technique, the substrate temperature is one of the key deposition parameters that affects the interfacial properties between the target film and substrate, determining the specific growth habits of the films. Herein, the effect of substrate temperature on the microstructure and electrical properties of magnetron-sputtered CdS (MS-CdS) films was studied and applied for the first time in hydrothermally deposited antimony selenosulfide (Sb2(S,Se)3) solar cells. Adjusting the substrate temperature not only results in the design of the flat and dense film with enhanced crystallinity but also leads to the formation of an energy level arrangement with a Sb2(S,Se)3 layer that is more favorable for electron transfer. In addition, we developed an oxygen plasma treatment for CdS, reducing the parasitic absorption of the device and resulting in an increase in the short-circuit current density of the solar cell. This study demonstrates the feasibility of MS-CdS in the fabrication of hydrothermal Sb2(S,Se)3 solar cells and provides interface optimization strategies to improve device performance.

    • Public Summary

    • Substrate heating was used during the sputtering process to improve the quality of the CdS thin film.
    • A higher crystallinity and smoother surface as well as a good energy level matching between the CdS and Sb2(S,Se)3 absorber layers are achieved.
    • Oxygen plasma treatment was used to treat the CdS layer to reduce Se diffusion during the annealing process, which improves the JSC and power conversion efficiency of solar cells.
    • A solar cell device with a power conversion efficiency of 8.09% is achieved, which is the highest among all antimony chalcogenide solar cells based on a sputtered CdS window layer.

    FullText(HTML)
  • loading
    • References(50)
  • [1]
    Yan C, Huang J, Sun K, et al. Cu2ZnSnS4 solar cells with over 10% power conversion efficiency enabled by heterojunction heat treatment. Nature Energy, 2018, 3 (9): 764–772. doi: 10.1038/s41560-018-0206-0
    [2]
    Yang S C, Lin T Y, Ochoa M, et al. Efficiency boost of bifacial Cu(In, Ga)Se2 thin-film solar cells for flexible and tandem applications with silver-assisted low-temperature process. Nature Energy, 2023, 8 (1): 40–51. doi: 10.1038/s41560-022-01157-9
    [3]
    Burst J M, Duenow J N, Albin D S, et al. CdTe solar cells with open-circuit voltage breaking the 1 V barrier. Nature Energy, 2016, 1 (3): 16015. doi: 10.1038/nenergy.2016.15
    [4]
    Tang R F, Wang X M, Lian W T, et al. Hydrothermal deposition of antimony selenosulfide thin films enables solar cells with 10% efficiency. Nature Energy, 2020, 5 (8): 587–595. doi: 10.1038/s41560-020-0652-3
    [5]
    Chen G J, Luo Y D, Abbas M, et al. Suppressing buried interface nonradiative recombination losses toward high-efficiency antimony triselenide solar cells. Advanced Materials, 2024, 36 (5): 2308522. doi: 10.1002/adma.202308522
    [6]
    Chen S, Fu Y, Ishaq M, et al. Carrier recombination suppression and transport enhancement enable high-performance self-powered broadband Sb2Se3 photodetectors. InfoMat, 2023, 5 (4): e12400. doi: 10.1002/inf2.12400
    [7]
    Tang R, Chen S, Zheng Z H, et al. Heterojunction annealing enabling record open-circuit voltage in antimony triselenide solar cells. Advanced Materials, 2022, 34 (14): 2109078. doi: 10.1002/adma.202109078
    [8]
    Luo Y D, Chen G J, Chen S, et al. Carrier transport enhancement mechanism in highly efficient antimony selenide thin-film solar cell. Advanced Functional Materials, 2023, 33 (14): 2213941. doi: 10.1002/adfm.202213941
    [9]
    Chen X L, Che B, Zhao Y Q, et al. Solvent-assisted hydrothermal deposition approach for highly-efficient Sb2(S, Se)3 thin-film solar cells. Advanced Energy Materials, 2023, 13 (21): 2300391. doi: 10.1002/aenm.202300391
    [10]
    Li G, Dong J B, Xiao P, et al. Dual effect of NH4F additive in the hydrothermal deposition of antimony selenosulfide thin film for high-performance solar cells. Science China Materials, 2022, 65 (12): 3411–3417. doi: 10.1007/s40843-022-2066-5
    [11]
    Wang X M, Tang R F, Jiang C H, et al. Manipulating the electrical properties of Sb2(S, Se)3 film for high-efficiency solar cell. Advanced Energy Materials, 2020, 10 (40): 2002341. doi: 10.1002/aenm.202002341
    [12]
    Pan X Y, Pan Y L, Shen L Y, et al. All-vacuum-processed Sb2(S, Se)3 thin film photovoltaic devices via controllable tuning seed orientation. Advanced Functional Materials, 2023, 33 (22): 2214511. doi: 10.1002/adfm.202214511
    [13]
    Liu J J, Cao M S, Feng Z D, et al. Thermal evaporation–deposited hexagonal CdS buffer layer with improved quality, enlarged band gap, and reduced band gap offset to boost performance of Sb2(S, Se)3 solar cells. Journal of Alloys and Compounds, 2022, 920 (1): 165885. doi: 10.1016/j.jallcom.2022.165885
    [14]
    Cheng J, Zhang Z, Zhao M H, et al. High-efficiency Sb2Se3 thin-film solar cells based on Cd(S, O) buffer layers prepared via spin-coating. Materials Chemistry and Physics, 2023, 303 (1): 127794. doi: 10.1016/j.matchemphys.2023.127794
    [15]
    Li K, Cai Z Y, Yang J J, et al. Molecular beam epitaxy deposition of in situ O-doped CdS films for highly efficient Sb2(S, Se)3 solar cells. Advanced Functional Materials, 2023, 33 (48): 2304141. doi: 10.1002/adfm.202304141
    [16]
    Schwartz C, Nordlund D, Weng T C, et al. Electronic structure study of the CdS buffer layer in CIGS solar cells by X-ray absorption spectroscopy: experiment and theory. Solar Energy Materials and Solar Cells, 2016, 149 (1): 275–283. doi: 10.1016/j.solmat.2016.01.043
    [17]
    Ge J, Koirala P, Grice C R, et al. Oxygenated CdS buffer layers enabling high open-circuit voltages in earth-abundant Cu2BaSnS4 thin-film solar cells. Advanced Energy Materials, 2017, 7 (6): 1601803. doi: 10.1002/aenm.201601803
    [18]
    Guo L, Zhang B, Ranjit S, et al. Interface engineering via sputtered oxygenated CdS: O window layer for highly efficient Sb2Se3 thin-film solar cells with efficiency above 7%. Solar RRL, 2019, 3 (10): 1900225. doi: 10.1002/solr.201900225
    [19]
    Hu X B, Tao J H, Wang Y Y, et al. 5.91%-efficient Sb2Se3 solar cells with a radio-frequency magnetron-sputtered CdS buffer layer. Applied Materials Today, 2019, 16 (1): 367–374. doi: 10.1016/j.apmt.2019.06.001
    [20]
    Kephart J M, Geisthardt R M, Sampath W S. Optimization of CdTe thin-film solar cell efficiency using a sputtered, oxygenated CdS window layer. Progress in Photovoltaics: Research and Applications, 2015, 23 (11): 1484–1492. doi: 10.1002/pip.2578
    [21]
    Liu Y F, Li B, Liang X Y, et al. Reactively sputtered CdS: O buffer layers for substrate Sb2Se3 solar cells. Journal of Alloys and Compounds, 2023, 932 (1): 167313. doi: 10.1016/j.jallcom.2022.167313
    [22]
    Ou C Z, Shen K, Li Z Q, et al. Bandgap tunable CdS: O as efficient electron buffer layer for high-performance Sb2Se3 thin film solar cells. Solar Energy Materials and Solar Cells, 2019, 194: 47–53. doi: 10.1016/j.solmat.2019.01.043
    [23]
    Paudel N R, Poplawsky J D, Moore K L, et al. Current enhancement of CdTe-based solar cells. IEEE Journal of Photovoltaics, 2015, 5 (5): 1492–1496. doi: 10.1109/JPHOTOV.2015.2458040
    [24]
    Shiel H, Hutter O S, Phillips L J, et al. Natural band alignments and band offsets of Sb2Se3 solar cells. ACS Applied Energy Materials, 2020, 3 (12): 11617–11626. doi: 10.1021/acsaem.0c01477
    [25]
    Stoner J. What is Magnetron Sputtering and How Does it Work. 2022 . https://korvustech.com/magnetron-sputtering/#:~:text=The%20advantages%20of%20magnetron%20sputtering%20include%3A%201%20High,5%20Uniformity%20on%20large-area%20substrates%206%20Low%20temperature. Accessed December 26, 2023.
    [26]
    Mchugh L F, Kumar P, Meendering D, et al. Method of making high-purity (>99%) MoO2 powders, products made from MoO2 powders, deposition of MoO2 thin films, and methods of using such materials. Patent WO2005040044, 2005 .
    [27]
    Wang K C, Shen P S, Li M H, et al. Low-temperature sputtered nickel oxide compact thin film as effective electron blocking layer for mesoscopic NiO/CH3NH3PbI3 perovskite heterojunction solar cells. ACS Applied Materials & Interfaces, 2014, 6 (15): 11851–11858. doi: 10.1021/am503610u
    [28]
    Wan L, Bai Z Z, Hou Z R, et al. Effect of CdCl2 annealing treatment on thin CdS films prepared by chemical bath deposition. Thin Solid Films, 2010, 518 (23): 6858–6865. doi: 10.1016/j.tsf.2010.07.011
    [29]
    Cai H L, Cao R, Gao J X, et al. Interfacial engineering towards enhanced photovoltaic performance of Sb2Se3 solar cell. Advanced Functional Materials, 2022, 32 (46): 2208243. doi: 10.1002/adfm.202208243
    [30]
    Yu M, Kenny S D. Using atomistic simulations to model cadmium telluride thin film growth. Journal of Physics: Condensed Matter, 2016, 28 (10): 105002. doi: 10.1088/0953-8984/28/10/105002
    [31]
    de Assis T A, Aarão Reis F D A. Thin film deposition with time-varying temperature. Journal of Statistical Mechanics: Theory and Experiment, 2013, 2013 (10): P10008. doi: 10.1088/1742-5468/2013/10/P10008
    [32]
    Blackwell S, Smith R, Kenny S D, et al. Modelling the growth of ZnO thin films by PVD methods and the effects of post-annealing. Journal of Physics: Condensed Matter, 2013, 25 (13): 135002. doi: 10.1088/0953-8984/25/13/135002
    [33]
    Liu M, Man B Y, Lin X C, et al. Effect of temperature on pulsed laser deposition of HgCdTe films. Applied Surface Science, 2007, 253 (24): 9291–9294. doi: 10.1016/j.apsusc.2007.05.070
    [34]
    Kephart J M, McCamy J W, Ma Z, et al. Band alignment of front contact layers for high-efficiency CdTe solar cells. Solar Energy Materials and Solar Cells, 2016, 157 (1): 266–275. doi: 10.1016/j.solmat.2016.05.050
    [35]
    Wetzelaer G A H, Kuik M, Nicolai H T, et al. Trap-assisted and Langevin-type recombination in organic light-emitting diodes. Physical Review B, 2011, 83 (16): 165204. doi: 10.1103/PhysRevB.83.165204
    [36]
    Wetzelaer G J A H, Scheepers M, Sempere A M, et al. Trap-assisted non-radiative recombination in organic–inorganic perovskite solar cells. Advanced Materials, 2015, 27 (11): 1837–1841. doi: 10.1002/adma.201405372
    [37]
    Woo J C S, Plummer J D, Stork J M C. Non-ideal base current in bipolar transistors at low temperatures. IEEE Transactions on Electron Devices, 1987, 34 (1): 130–138. doi: 10.1109/T-ED.1987.22895
    [38]
    Kaminski A, Marchand J J, Laugier A. Non ideal dark I–V curves behavior of silicon solar cells. Solar Energy Materials and Solar Cells, 1998, 51 (3/4): 221–231. doi: 10.1016/S0927-0248(97)00216-X
    [39]
    Liang G X, Chen M D, Ishaq M, et al. Crystal growth promotion and defects healing enable minimum open-circuit voltage deficit in antimony selenide solar cells. Advanced Science, 2022, 9 (9): 2105142. doi: 10.1002/advs.202105142
    [40]
    Ishaq M, Deng H, Yuan S J, et al. Efficient double buffer layer Sb2(SexS1–x)3 thin film solar cell via single source evaporation. Solar RRL, 2018, 2 (10): 1800144. doi: 10.1002/solr.201800144
    [41]
    Zhao J, Li X R, Lin J H, et al. Unveiling the influence of absorber thickness on efficient Sb2(S, Se)3 solar cells through controlled chemical bath deposition. Surfaces and Interfaces, 2023, 42 (1): 103411. doi: 10.1016/j.surfin.2023.103411
    [42]
    Li J M, Zhao Y Q, Li C, et al. Hydrazine hydrate-induced surface modification of CdS electron transport layer enables 10.30%-efficient Sb2(S, Se)3 planar solar cells. Advanced Science, 2022, 9 (25): 2202356. doi: 10.1002/advs.202202356
    [43]
    Sites J R, Mauk P H. Diode quality factor determination for thin-film solar cells. Solar Cells, 1989, 27 (1): 411–417. doi: 10.1016/0379-6787(89)90050-1
    [44]
    Deng B Z, Lian H, Xue B T, et al. Niobium-carbide MXene modified hybrid hole transport layer enabling high-performance organic solar cells over 19%. Small, 2023, 19 (23): 2207505. doi: 10.1002/smll.202207505
    [45]
    Lin Y R, Tunuguntla V, Wei S Y, et al. Bifacial sodium-incorporated treatments: Tailoring deep traps and enhancing carrier transport properties in Cu2ZnSnS4 solar cells. Nano Energy, 2015, 16 (1): 438–445. doi: 10.1016/j.nanoen.2015.07.022
    [46]
    Christians J A, Kamat P V. Trap and transfer. Two-step hole injection across the Sb2S3/CuSCN interface in solid-state solar cells. ACS Nano, 2013, 7 (9): 7967–7974. doi: 10.1021/nn403058f
    [47]
    Yang Z L, Wang X M, Chen Y Z, et al. Ultrafast self-trapping of photoexcited carriers sets the upper limit on antimony trisulfide photovoltaic devices. Nature Communications, 2019, 10 (1): 4540. doi: 10.1038/s41467-019-12445-6
    [48]
    Guo H F, Chen Z W, Wang X, et al. Enhancement in the efficiency of Sb2Se3 thin-film solar cells by increasing carrier concertation and inducing columnar growth of the grains. Solar RRL, 2018, 3 (3): 1800224. doi: 10.1002/solr.201800224
    [49]
    Li Z Q, Liang X Y, Li G, et al. 9.2%-efficient core-shell structured antimony selenide nanorod array solar cells. Nature Communications, 2019, 10 (1): 125. doi: 10.1038/s41467-018-07903-6
    [50]
    Wu Q C, Lin X L, Mahabaduge H, et al. Effect of oxygen on the properties of CdSe thin films prepared by RF-sputtering. Chemical Physics Letters, 2022, 799 (1): 139633. doi: 10.1016/j.cplett.2022.139633
    • Supplements(1)
  • JUSTC-2024-0048 Supporting information.docx
    • Related Articles
    • Track Citations
  • 加载中

Catalog

    |
    Get Citation
    PDF
    XML

    Figure  1.  X-ray diffraction (XRD) pattern of the sputtered CdS thin film. The deposition time was 2 h, four times the standard CdS growth time. (a) CdS sputtered on a glass substrate at different temperatures. (b) CdS sputtered on an FTO substrate. The positions of the FTO diffraction peaks are labeled with asterisks. (c) Grazing incidence XRD (GIXRD) result of CdS sputtered on an FTO substrate. The incident angle is 0.4°, and no FTO substrate peaks are found.

    Figure  2.  SEM image of sputtered CdS. The first row shows sputtered CdS without ambient air annealing. The second row shows sputtered CdS with CdCl2 spin coating and ambient air annealing posttreatment. The four columns show CdS sputtered at RT, 150 °C, 200 °C and 250 °C from left to right.

    Figure  3.  Characterization of Sb2(S,Se)3 thin films grown on sputtered CdS. (a) XRD pattern of the Sb2(S,Se)3 thin film. (b) Statistics on the grain size of the Sb2(S,Se)3 thin film. SEM image of a Sb2(S,Se)3 thin film (c) grown on RT-sputtered CdS and (d) grown on 200 °C-sputtered CdS.

    Figure  4.  UPS spectra of (a) RT-sputtered CdS, (b) substrate heat-sputtered CdS and (c) Sb2(S,Se)3 thin films. (d, e) Band alignment diagram of the Sb2(S,Se)3 solar cell devices.

    Figure  5.  Photovoltaic performance of the devices. (a) Current density–voltage (J–V) curves of Sb2(S,Se)3 solar cell devices grown on sputtered CdS under different substrate heating conditions. Statistical boxplots of the photovoltaic parameters (b) power conversion efficiency (PCE), (c) short-circuit current density (JSC), (e) open-circuit voltage (VOC), and (f) fill factor (FF) of the corresponding devices. (d) External quantum efficiency (EQE) spectra of the corresponding devices.

    Figure  6.  Characterization of Sb2(S,Se)3 solar cell devices grown on sputtered CdS under different substrate heating conditions. Dark current results are shown in the first row with (a) J–V curve, (b) dJ/dV versus voltage plot, and (c) dV/dJ versus (J+JSC)−1 plot. Here, the dark J–V data were measured starting at +3 V, so that (J+JSC)−1 increased to approximately 0.002 mA−1·cm2. Under very high voltage conditions, the derivative increases, forming a tail at the end of the curve. However, this does not influence the analysis by using the well-defined linear part of the curve. The light intensity, electrochemical characterization and carrier transport kinetics of the devices are shown next. (d) Relation between VOC and the logarithm of the incident light intensity. (e) Relation between JSC and the incident light intensity. (f) Nyquist plots (under dark conditions at −0.60 V) of the devices. (g) Original data and fitted curves of transient decay kinetics monitored at 665 nm for Sb2(S,Se)3 films grown on sputtered CdS at RT and at 200 °C.

    Figure  7.  Characterization related to oxygen plasma treatment of sputtered CdS. (a) Full-wavelength EQE spectra of devices with (15 min) and without oxygen plasma treatment (OPT). (b) Champion device efficiency with and without oxygen plasma treatment. (c) Oxygen content and Cd∶S ratio under different oxygen plasma treatment conditions. The results are based on EDS data. (d) The 1/C2–V curves of the devices recorded at a frequency of 100 kHz at RT in the dark.

    [1]
    Yan C, Huang J, Sun K, et al. Cu2ZnSnS4 solar cells with over 10% power conversion efficiency enabled by heterojunction heat treatment. Nature Energy, 2018, 3 (9): 764–772. doi: 10.1038/s41560-018-0206-0
    [2]
    Yang S C, Lin T Y, Ochoa M, et al. Efficiency boost of bifacial Cu(In, Ga)Se2 thin-film solar cells for flexible and tandem applications with silver-assisted low-temperature process. Nature Energy, 2023, 8 (1): 40–51. doi: 10.1038/s41560-022-01157-9
    [3]
    Burst J M, Duenow J N, Albin D S, et al. CdTe solar cells with open-circuit voltage breaking the 1 V barrier. Nature Energy, 2016, 1 (3): 16015. doi: 10.1038/nenergy.2016.15
    [4]
    Tang R F, Wang X M, Lian W T, et al. Hydrothermal deposition of antimony selenosulfide thin films enables solar cells with 10% efficiency. Nature Energy, 2020, 5 (8): 587–595. doi: 10.1038/s41560-020-0652-3
    [5]
    Chen G J, Luo Y D, Abbas M, et al. Suppressing buried interface nonradiative recombination losses toward high-efficiency antimony triselenide solar cells. Advanced Materials, 2024, 36 (5): 2308522. doi: 10.1002/adma.202308522
    [6]
    Chen S, Fu Y, Ishaq M, et al. Carrier recombination suppression and transport enhancement enable high-performance self-powered broadband Sb2Se3 photodetectors. InfoMat, 2023, 5 (4): e12400. doi: 10.1002/inf2.12400
    [7]
    Tang R, Chen S, Zheng Z H, et al. Heterojunction annealing enabling record open-circuit voltage in antimony triselenide solar cells. Advanced Materials, 2022, 34 (14): 2109078. doi: 10.1002/adma.202109078
    [8]
    Luo Y D, Chen G J, Chen S, et al. Carrier transport enhancement mechanism in highly efficient antimony selenide thin-film solar cell. Advanced Functional Materials, 2023, 33 (14): 2213941. doi: 10.1002/adfm.202213941
    [9]
    Chen X L, Che B, Zhao Y Q, et al. Solvent-assisted hydrothermal deposition approach for highly-efficient Sb2(S, Se)3 thin-film solar cells. Advanced Energy Materials, 2023, 13 (21): 2300391. doi: 10.1002/aenm.202300391
    [10]
    Li G, Dong J B, Xiao P, et al. Dual effect of NH4F additive in the hydrothermal deposition of antimony selenosulfide thin film for high-performance solar cells. Science China Materials, 2022, 65 (12): 3411–3417. doi: 10.1007/s40843-022-2066-5
    [11]
    Wang X M, Tang R F, Jiang C H, et al. Manipulating the electrical properties of Sb2(S, Se)3 film for high-efficiency solar cell. Advanced Energy Materials, 2020, 10 (40): 2002341. doi: 10.1002/aenm.202002341
    [12]
    Pan X Y, Pan Y L, Shen L Y, et al. All-vacuum-processed Sb2(S, Se)3 thin film photovoltaic devices via controllable tuning seed orientation. Advanced Functional Materials, 2023, 33 (22): 2214511. doi: 10.1002/adfm.202214511
    [13]
    Liu J J, Cao M S, Feng Z D, et al. Thermal evaporation–deposited hexagonal CdS buffer layer with improved quality, enlarged band gap, and reduced band gap offset to boost performance of Sb2(S, Se)3 solar cells. Journal of Alloys and Compounds, 2022, 920 (1): 165885. doi: 10.1016/j.jallcom.2022.165885
    [14]
    Cheng J, Zhang Z, Zhao M H, et al. High-efficiency Sb2Se3 thin-film solar cells based on Cd(S, O) buffer layers prepared via spin-coating. Materials Chemistry and Physics, 2023, 303 (1): 127794. doi: 10.1016/j.matchemphys.2023.127794
    [15]
    Li K, Cai Z Y, Yang J J, et al. Molecular beam epitaxy deposition of in situ O-doped CdS films for highly efficient Sb2(S, Se)3 solar cells. Advanced Functional Materials, 2023, 33 (48): 2304141. doi: 10.1002/adfm.202304141
    [16]
    Schwartz C, Nordlund D, Weng T C, et al. Electronic structure study of the CdS buffer layer in CIGS solar cells by X-ray absorption spectroscopy: experiment and theory. Solar Energy Materials and Solar Cells, 2016, 149 (1): 275–283. doi: 10.1016/j.solmat.2016.01.043
    [17]
    Ge J, Koirala P, Grice C R, et al. Oxygenated CdS buffer layers enabling high open-circuit voltages in earth-abundant Cu2BaSnS4 thin-film solar cells. Advanced Energy Materials, 2017, 7 (6): 1601803. doi: 10.1002/aenm.201601803
    [18]
    Guo L, Zhang B, Ranjit S, et al. Interface engineering via sputtered oxygenated CdS: O window layer for highly efficient Sb2Se3 thin-film solar cells with efficiency above 7%. Solar RRL, 2019, 3 (10): 1900225. doi: 10.1002/solr.201900225
    [19]
    Hu X B, Tao J H, Wang Y Y, et al. 5.91%-efficient Sb2Se3 solar cells with a radio-frequency magnetron-sputtered CdS buffer layer. Applied Materials Today, 2019, 16 (1): 367–374. doi: 10.1016/j.apmt.2019.06.001
    [20]
    Kephart J M, Geisthardt R M, Sampath W S. Optimization of CdTe thin-film solar cell efficiency using a sputtered, oxygenated CdS window layer. Progress in Photovoltaics: Research and Applications, 2015, 23 (11): 1484–1492. doi: 10.1002/pip.2578
    [21]
    Liu Y F, Li B, Liang X Y, et al. Reactively sputtered CdS: O buffer layers for substrate Sb2Se3 solar cells. Journal of Alloys and Compounds, 2023, 932 (1): 167313. doi: 10.1016/j.jallcom.2022.167313
    [22]
    Ou C Z, Shen K, Li Z Q, et al. Bandgap tunable CdS: O as efficient electron buffer layer for high-performance Sb2Se3 thin film solar cells. Solar Energy Materials and Solar Cells, 2019, 194: 47–53. doi: 10.1016/j.solmat.2019.01.043
    [23]
    Paudel N R, Poplawsky J D, Moore K L, et al. Current enhancement of CdTe-based solar cells. IEEE Journal of Photovoltaics, 2015, 5 (5): 1492–1496. doi: 10.1109/JPHOTOV.2015.2458040
    [24]
    Shiel H, Hutter O S, Phillips L J, et al. Natural band alignments and band offsets of Sb2Se3 solar cells. ACS Applied Energy Materials, 2020, 3 (12): 11617–11626. doi: 10.1021/acsaem.0c01477
    [25]
    Stoner J. What is Magnetron Sputtering and How Does it Work. 2022 . https://korvustech.com/magnetron-sputtering/#:~:text=The%20advantages%20of%20magnetron%20sputtering%20include%3A%201%20High,5%20Uniformity%20on%20large-area%20substrates%206%20Low%20temperature. Accessed December 26, 2023.
    [26]
    Mchugh L F, Kumar P, Meendering D, et al. Method of making high-purity (>99%) MoO2 powders, products made from MoO2 powders, deposition of MoO2 thin films, and methods of using such materials. Patent WO2005040044, 2005 .
    [27]
    Wang K C, Shen P S, Li M H, et al. Low-temperature sputtered nickel oxide compact thin film as effective electron blocking layer for mesoscopic NiO/CH3NH3PbI3 perovskite heterojunction solar cells. ACS Applied Materials & Interfaces, 2014, 6 (15): 11851–11858. doi: 10.1021/am503610u
    [28]
    Wan L, Bai Z Z, Hou Z R, et al. Effect of CdCl2 annealing treatment on thin CdS films prepared by chemical bath deposition. Thin Solid Films, 2010, 518 (23): 6858–6865. doi: 10.1016/j.tsf.2010.07.011
    [29]
    Cai H L, Cao R, Gao J X, et al. Interfacial engineering towards enhanced photovoltaic performance of Sb2Se3 solar cell. Advanced Functional Materials, 2022, 32 (46): 2208243. doi: 10.1002/adfm.202208243
    [30]
    Yu M, Kenny S D. Using atomistic simulations to model cadmium telluride thin film growth. Journal of Physics: Condensed Matter, 2016, 28 (10): 105002. doi: 10.1088/0953-8984/28/10/105002
    [31]
    de Assis T A, Aarão Reis F D A. Thin film deposition with time-varying temperature. Journal of Statistical Mechanics: Theory and Experiment, 2013, 2013 (10): P10008. doi: 10.1088/1742-5468/2013/10/P10008
    [32]
    Blackwell S, Smith R, Kenny S D, et al. Modelling the growth of ZnO thin films by PVD methods and the effects of post-annealing. Journal of Physics: Condensed Matter, 2013, 25 (13): 135002. doi: 10.1088/0953-8984/25/13/135002
    [33]
    Liu M, Man B Y, Lin X C, et al. Effect of temperature on pulsed laser deposition of HgCdTe films. Applied Surface Science, 2007, 253 (24): 9291–9294. doi: 10.1016/j.apsusc.2007.05.070
    [34]
    Kephart J M, McCamy J W, Ma Z, et al. Band alignment of front contact layers for high-efficiency CdTe solar cells. Solar Energy Materials and Solar Cells, 2016, 157 (1): 266–275. doi: 10.1016/j.solmat.2016.05.050
    [35]
    Wetzelaer G A H, Kuik M, Nicolai H T, et al. Trap-assisted and Langevin-type recombination in organic light-emitting diodes. Physical Review B, 2011, 83 (16): 165204. doi: 10.1103/PhysRevB.83.165204
    [36]
    Wetzelaer G J A H, Scheepers M, Sempere A M, et al. Trap-assisted non-radiative recombination in organic–inorganic perovskite solar cells. Advanced Materials, 2015, 27 (11): 1837–1841. doi: 10.1002/adma.201405372
    [37]
    Woo J C S, Plummer J D, Stork J M C. Non-ideal base current in bipolar transistors at low temperatures. IEEE Transactions on Electron Devices, 1987, 34 (1): 130–138. doi: 10.1109/T-ED.1987.22895
    [38]
    Kaminski A, Marchand J J, Laugier A. Non ideal dark I–V curves behavior of silicon solar cells. Solar Energy Materials and Solar Cells, 1998, 51 (3/4): 221–231. doi: 10.1016/S0927-0248(97)00216-X
    [39]
    Liang G X, Chen M D, Ishaq M, et al. Crystal growth promotion and defects healing enable minimum open-circuit voltage deficit in antimony selenide solar cells. Advanced Science, 2022, 9 (9): 2105142. doi: 10.1002/advs.202105142
    [40]
    Ishaq M, Deng H, Yuan S J, et al. Efficient double buffer layer Sb2(SexS1–x)3 thin film solar cell via single source evaporation. Solar RRL, 2018, 2 (10): 1800144. doi: 10.1002/solr.201800144
    [41]
    Zhao J, Li X R, Lin J H, et al. Unveiling the influence of absorber thickness on efficient Sb2(S, Se)3 solar cells through controlled chemical bath deposition. Surfaces and Interfaces, 2023, 42 (1): 103411. doi: 10.1016/j.surfin.2023.103411
    [42]
    Li J M, Zhao Y Q, Li C, et al. Hydrazine hydrate-induced surface modification of CdS electron transport layer enables 10.30%-efficient Sb2(S, Se)3 planar solar cells. Advanced Science, 2022, 9 (25): 2202356. doi: 10.1002/advs.202202356
    [43]
    Sites J R, Mauk P H. Diode quality factor determination for thin-film solar cells. Solar Cells, 1989, 27 (1): 411–417. doi: 10.1016/0379-6787(89)90050-1
    [44]
    Deng B Z, Lian H, Xue B T, et al. Niobium-carbide MXene modified hybrid hole transport layer enabling high-performance organic solar cells over 19%. Small, 2023, 19 (23): 2207505. doi: 10.1002/smll.202207505
    [45]
    Lin Y R, Tunuguntla V, Wei S Y, et al. Bifacial sodium-incorporated treatments: Tailoring deep traps and enhancing carrier transport properties in Cu2ZnSnS4 solar cells. Nano Energy, 2015, 16 (1): 438–445. doi: 10.1016/j.nanoen.2015.07.022
    [46]
    Christians J A, Kamat P V. Trap and transfer. Two-step hole injection across the Sb2S3/CuSCN interface in solid-state solar cells. ACS Nano, 2013, 7 (9): 7967–7974. doi: 10.1021/nn403058f
    [47]
    Yang Z L, Wang X M, Chen Y Z, et al. Ultrafast self-trapping of photoexcited carriers sets the upper limit on antimony trisulfide photovoltaic devices. Nature Communications, 2019, 10 (1): 4540. doi: 10.1038/s41467-019-12445-6
    [48]
    Guo H F, Chen Z W, Wang X, et al. Enhancement in the efficiency of Sb2Se3 thin-film solar cells by increasing carrier concertation and inducing columnar growth of the grains. Solar RRL, 2018, 3 (3): 1800224. doi: 10.1002/solr.201800224
    [49]
    Li Z Q, Liang X Y, Li G, et al. 9.2%-efficient core-shell structured antimony selenide nanorod array solar cells. Nature Communications, 2019, 10 (1): 125. doi: 10.1038/s41467-018-07903-6
    [50]
    Wu Q C, Lin X L, Mahabaduge H, et al. Effect of oxygen on the properties of CdSe thin films prepared by RF-sputtering. Chemical Physics Letters, 2022, 799 (1): 139633. doi: 10.1016/j.cplett.2022.139633
    Recommended articles
    TrendMD
    Volume 54 Issue 6 page: 0604
    Cover

    Article Metrics

    Article views (151) PDF downloads(581)
    Proportional views

    Copyright © Editorial Office of JUSTC, All Rights Reserved. 皖ICP备05002528号

    Supported by: Beijing Renhe Information Technology Co. Ltd    

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return