Enhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes.
This study investigates the utilization of Cu2ZnSnS4/ZnCo2O4 (CZTS/ZCO) nanocomposites prepared through hydrothermal and combustion methods as counter electrodes in Dye-Sensitized Solar Cells (DSSCs). Different ratios of Cu2ZnSnS4 and ZnCo2O4 were explored, and comprehensive analyses were conducted...
- Autores:
-
AL-Zoubi, Omar H.
Grimaldo Guerrero, John William
Khan, Ahmad Raza
Kumar, Ashwani
Olegovich Bokov, Dmitry
Juraev, Nizomiddin
Pramanik, Atreyi
Qasim, Maytham T.
Redhee, Ahmeed hoseen
- Tipo de recurso:
- Article of investigation
- Fecha de publicación:
- 2024
- Institución:
- Corporación Universidad de la Costa
- Repositorio:
- REDICUC - Repositorio CUC
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.cuc.edu.co:11323/13812
- Acceso en línea:
- https://hdl.handle.net/11323/13812
- Palabra clave:
- Counter electrode
CZTS
DSSC
ZCO
- Rights
- openAccess
- License
- Atribución 4.0 Internacional (CC BY 4.0)
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dc.title.eng.fl_str_mv |
Enhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes. |
title |
Enhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes. |
spellingShingle |
Enhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes. Counter electrode CZTS DSSC ZCO |
title_short |
Enhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes. |
title_full |
Enhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes. |
title_fullStr |
Enhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes. |
title_full_unstemmed |
Enhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes. |
title_sort |
Enhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes. |
dc.creator.fl_str_mv |
AL-Zoubi, Omar H. Grimaldo Guerrero, John William Khan, Ahmad Raza Kumar, Ashwani Olegovich Bokov, Dmitry Juraev, Nizomiddin Pramanik, Atreyi Qasim, Maytham T. Redhee, Ahmeed hoseen |
dc.contributor.author.none.fl_str_mv |
AL-Zoubi, Omar H. Grimaldo Guerrero, John William Khan, Ahmad Raza Kumar, Ashwani Olegovich Bokov, Dmitry Juraev, Nizomiddin Pramanik, Atreyi Qasim, Maytham T. Redhee, Ahmeed hoseen |
dc.subject.proposal.eng.fl_str_mv |
Counter electrode CZTS DSSC ZCO |
topic |
Counter electrode CZTS DSSC ZCO |
description |
This study investigates the utilization of Cu2ZnSnS4/ZnCo2O4 (CZTS/ZCO) nanocomposites prepared through hydrothermal and combustion methods as counter electrodes in Dye-Sensitized Solar Cells (DSSCs). Different ratios of Cu2ZnSnS4 and ZnCo2O4 were explored, and comprehensive analyses were conducted using X-ray Diffraction (XRD), Transmission Electron Microscopy (TEM), High-Resolution TEM (HRTEM), Brunauer–Emmett–Teller (BET) surface area analysis, Raman Spectroscopy, Electrochemical Impedance Spectroscopy (EIS), cyclic voltammetry (CV), Tafel analysis, Field Emission Scanning Electron Microscopy (FESEM), and Incident Photon-to-Electron Conversion Efficiency (IPCE), alongside long-term stability assessments. The CZTS:ZCO ratio of 2:1 exhibited the highest efficiency, reaching 8.81 %, with an open-circuit voltage of 729 mV, short-circuit current of 17.80 mAcm−2, and a fill factor of 67.9 %. This surpasses the efficiency of the reference Pt cell (8.42 %), which had an open-circuit voltage of 735 mV, short-circuit current of 17.16 mAcm−2, and a fill factor of 66.8 %. The average crystallite sizes for the main peaks of CZTS and ZCO samples were estimated to be 19.8 and 16.7 nm, respectively. The crystallite size can significantly affect the charge transfer and conductivity in the counter electrode during electrochemical processes; the presence of nanocrystals with these sizes can notably enhance the electrochemical properties and conductivity of the synthesized samples. Raman analysis results indicate that no additional phases or secondary phases such as ZnS and CuSnS3 have formed in the kesterite CZTS structure, and the crystal has formed as a single phase. Additionally, the F2g modes in the Raman spectrum of ZCO indicate tetrahedral units in the spinel ZCO structure, and the A1g modes represent octahedral structures in this phase, indicating the formation of suitable ZCO phase. The superior performance of the CZTS/ZCO nanocomposite can be attributed to its enhanced crystalline structure, superior charge transport characteristics, and improved electrocatalytic behaviours. |
publishDate |
2024 |
dc.date.accessioned.none.fl_str_mv |
2024-11-25T16:26:06Z |
dc.date.available.none.fl_str_mv |
2024-11-25T16:26:06Z |
dc.date.issued.none.fl_str_mv |
2024-05-14 |
dc.type.none.fl_str_mv |
Artículo de revista |
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http://purl.org/coar/resource_type/c_2df8fbb1 |
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Text |
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info:eu-repo/semantics/article |
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http://purl.org/redcol/resource_type/ART |
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info:eu-repo/semantics/publishedVersion |
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http://purl.org/coar/version/c_970fb48d4fbd8a85 |
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http://purl.org/coar/resource_type/c_2df8fbb1 |
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publishedVersion |
dc.identifier.citation.none.fl_str_mv |
Omar H. AL-Zoubi, John William Grimaldo Guerrero, Ahmad Raza Khan, Ashwani Kumar, Dmitry Olegovich Bokov, Nizomiddin Juraev, Atreyi Pramanik, Maytham T. Qasim, Ahmeed hoseen Redhee, Enhancing dye-sensitized solar cell performance: Optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes, Materials Science in Semiconductor Processing, Volume 179, 2024, 108526, ISSN 1369-8001, https://doi.org/10.1016/j.mssp.2024.108526. |
dc.identifier.issn.none.fl_str_mv |
1369-8001 |
dc.identifier.uri.none.fl_str_mv |
https://hdl.handle.net/11323/13812 |
dc.identifier.doi.none.fl_str_mv |
10.1016/j.mssp.2024.108526 |
dc.identifier.eissn.none.fl_str_mv |
1873-4081 |
identifier_str_mv |
Omar H. AL-Zoubi, John William Grimaldo Guerrero, Ahmad Raza Khan, Ashwani Kumar, Dmitry Olegovich Bokov, Nizomiddin Juraev, Atreyi Pramanik, Maytham T. Qasim, Ahmeed hoseen Redhee, Enhancing dye-sensitized solar cell performance: Optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes, Materials Science in Semiconductor Processing, Volume 179, 2024, 108526, ISSN 1369-8001, https://doi.org/10.1016/j.mssp.2024.108526. 1369-8001 10.1016/j.mssp.2024.108526 1873-4081 |
url |
https://hdl.handle.net/11323/13812 |
dc.language.iso.none.fl_str_mv |
eng |
language |
eng |
dc.relation.ispartofjournal.none.fl_str_mv |
Materials Science in Semiconductor Processing |
dc.relation.references.none.fl_str_mv |
M. Soltanmohammadi, V. Karimi, S. Alee, M. Abrari, M. Ahmadi, M. Ghanaatshoar Cu2ZnSnS4 thin film as a counter electrode in zinc stannate-based dye-sensitized solar cells Semicond. Sci. Technol., 36 (10) (2021), Article 105008 X. Wang, B. Zhao, W. Kan, Y. Xie, K. Pan Review on low‐cost counter electrode materials for dye‐sensitized solar cells: effective strategy to improve photovoltaic performance Adv. Mater. Interfac., 9 (2) (2022), Article 2101229 G. Richhariya, A. Kumar, A.K. Shukla, K. Shukla, B.C. Meikap Effect of different counter electrodes on power conversion efficiency of DSSCs J. Electron. Mater., 52 (1) (2023), pp. 60-71 M. Ahmadi, S.J. Anaghizi, M. Asemi, M. Ghanaatshoar Plasma-treated room temperature synthesized CuCrO2/Au/CuCrO2 on Polyethylene terephthalate: towards a high-performance flexible p-type transparent conductor Thin Solid Films, 723 (2021), Article 138582 M.M. Ibrahim, M.A. Hassan, K.I. Hassoon Novel route to prepare iron sulphide as a counter electrode for dye-sensitized solar cell Bull. Mater. Sci., 46 (3) (2023), p. 120 Y. Hu, Y. Zheng, J. Jin, Y. Wang, Y. Peng, J. Yin, W. Shen, Y. Hou, L. Zhu, L. An Understanding the sulphur-oxygen exchange process of metal sulphides prior to oxygen evolution reaction Nat. Commun., 14 (1) (2023), p. 1949 Z. Golshani, F. Arjmand, S. Maghsoudi, S.M.A. Hosseini Fe2O3–NiO doped carbon counter electrode for high-performance and long-term stable photovoltaic perovskite solar cells J. Mater. Res. Technol., 23 (2023), pp. 2612-2625 D. Cao, Z. Li, Y. Xu, W. Li, H. Zhong, Y. Huang, X. Zhang, L. Wan, X. Zhang, Y. Li Interfacial engineering by p-methylphenylmethylammonium iodide for efficient carbon counter electrode (CE)-based 2D/3D hybrid perovskite solar cells Org. Electron., 113 (2023), Article 106699 S. Ding, C. Yang, J. Yuan, H. Li, X. Yuan, M. Li An overview of the preparation and application of counter electrodes for DSSCs RSC Adv., 13 (18) (2023), pp. 12309-12319 H. Pervaiz, Z.S. Khan, N. Shahzad, G. Ali, N. Iqbal, S. Javed Fabrication of cellulose paper-based counter electrodes for flexible dye-sensitized solar cells Phys. Chem. Chem. Phys., 25 (1) (2023), pp. 428-438 Y. Kurokawa, T. Kato, S.S. Pandey Controlling the electrocatalytic activities of conducting polymer thin films toward suitability as cost-effective counter electrodes of dye-sensitized solar cells Synth. Met., 296 (2023), Article 117362 A. Asok, K. Haribabu Synthesis and performance of polythiophene-iridium oxide composite as counter electrode in dye sensitized solar cell Curr. Appl. Phys., 49 (2023), pp. 64-69 R.H. Althomali, E.A.M. Saleh, R.S. Bhat, S. Askar, I. Sapaev, M.A. Najm, B.M. Ridha, A.H. Alsalamy, R. Riyadh Novel ZnCo2O4/WO3 nanocomposite as the counter electrode for dye-sensitized solar cells (DSSCs): study of electrocatalytic activity and charge transfer properties Opt. Mater., 143 (2023), Article 114248 K. Kaur, M. Patyal, N. Gupta, A. Kumar, M. Khanuja Graphene/macrocylic Yb nanocomposite as counter electrode in dye sensitized solar cell Opt. Mater., 139 (2023), Article 113831 L. Mxakaza, G. Ngubeni, N. Moloto, Z. Tetana Cu2ZnSnS4/N-MWCNTs hybrid systems as counter electrode substitutes for platinum in dye-sensitized solar cells J. Mater. Res. (2024), pp. 1-13 A. Roy, P. Sujatha Devi, S. Karazhanov, D. Mamedov, T.K. Mallick, S. Sundaram A review on applications of Cu2ZnSnS4 as alternative counter electrodes in dye-sensitized solar cells AIP Adv., 8 (7) (2018) O.H. Al-Zoubi, E.A.M. Saleh, A.N.A. Saieed, B.D. Olegovich, E.R. Alwaily, A. Alawadi, M. Talal, Y.F. Mustafa Platinum-free counter electrode based on ZnCo2O4@ NiO core-shell nanostructures in dye-sensitized solar cells Mater. Sci. Semicond. Process., 174 (2024), Article 108234 S.S. Abdullaev, Y.F. Breesam, A.A. AlZubaidi, A.K. Tripathi, A. Kareem, S.V. Kuznetsov, T. Alawsi, R.S. Zabibah ZnO@ ZnCo2O4 core-shell: a novel high electrocatalytic nanostructure to replace platinum as the counter electrode in dye-sensitized solar cells Mater. Sci. Semicond. Process., 165 (2023), Article 107709 G.M. Alvien, D. Xuan Long, K. Yolthida, Y. Hee Jang, J. Hong Combustion‐assisted polyol reduction method to prepare highly transparent and efficient Pt counter electrodes for bifacial dye‐sensitized solar cells Chem.--Asian J., 18 (6) (2023), Article e202201142 K. Subalakshmi, K.A. Kumar, O.P. Paul, S. Saraswathy, A. Pandurangan, J. Senthilselvan Platinum-free metal sulfide counter electrodes for DSSC applications: structural, electrochemical and power conversion efficiency analyses Sol. Energy, 193 (2019), pp. 507-518 K. Xiong, G. Li, C. Jin, S. Jin La0. 65Sr0. 35MnO3@ RGO nanocomposites as an effective counter electrode for dye-sensitized solar cells Mater. Lett., 164 (2016), pp. 609-612 S. Umale, V. Sudhakar, S.M. Sontakke, K. Krishnamoorthy, A.B. Pandit Improved efficiency of DSSC using combustion synthesized TiO2 Mater. Res. Bull., 109 (2019), pp. 222-226 V. Murugadoss, P. Panneerselvam, C. Yan, Z. Guo, S. Angaiah A simple one-step hydrothermal synthesis of cobaltnickel selenide/graphene nanohybrid as an advanced platinum free counter electrode for dye sensitized solar cell Electrochim. Acta, 312 (2019), pp. 157-167 M. Gao, Z. Shen, G. Yue, C. Dong, J. Wu, Y. Gao, F. Tan One-pot hydrothermal in situ growth of In4SnS8@ MoS2@ CNTs as efficient Pt-free counter electrodes for dye-sensitized solar cells J. Alloys Compd., 932 (2023), Article 167643 K. Wu, F. Nie, X. Qi, Y. Wu, H. Zhao, M. Wu Polyoxovanadate derived VN@ C composite catalysts by different synthesis routes as Pt-free counter electrode for dye-sensitized solar cells Mater. Sci. Eng., B, 295 (2023), Article 116584 M. Ahmadi, M. Abrari, M. Ghanaatshoar An all-sputtered photovoltaic ultraviolet photodetector based on co-doped CuCrO2 and Al-doped ZnO heterojunction Sci. Rep., 11 (1) (2021), Article 18694 P. Fernandes, P. Salomé, A. Da Cunha Study of polycrystalline Cu2ZnSnS4 films by Raman scattering J. Alloys Compd., 509 (28) (2011), pp. 7600-7606 C. Sripan, R. Ganesan, E. Vinod, A.K. Viswanath The effect of sulfur on the phase formation of Cu2ZnSnS4 solar cell material Mater. Lett., 180 (2016), pp. 295-297 E. Samiei, S. Mohammadi, M. Torkzadeh-Mahani Effect of gamma-irradiation on electrochemical properties of ZnCo2O4-rGO for supercapacitor application Diam. Relat. Mater., 127 (2022), Article 109157 K.-M. Lee, P.-Y. Chen, C.-Y. Hsu, J.-H. Huang, W.-H. Ho, H.-C. Chen, K.-C. Ho A high-performance counter electrode based on poly (3, 4-alkylenedioxythiophene) for dye-sensitized solar cells J. Power Sources, 188 (1) (2009), pp. 313-318 R. Senthilkumar, M. Balu, S. Ramakrishnan, P.C. Ramamurthy, S.K. Batabyal, D. Kumaresan, N.K. Kothurkar Molybdenum disulfide/reduced graphene oxide hybrids with enhanced electrocatalytic activity: an efficient counter electrode for dye-sensitized solar cells J. Electroanal. Chem., 847 (2019), Article 113236 T. Sawatsuk, A. Chindaduang, C. Sae-Kung, S. Pratontep, G. Tumcharern Dye-sensitized solar cells based on TiO2–MWCNTs composite electrodes: performance improvement and their mechanisms Diam. Relat. Mater., 18 (2–3) (2009), pp. 524-527 |
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108526 |
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179 |
dc.rights.eng.fl_str_mv |
© 2024 |
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Atribución 4.0 Internacional (CC BY 4.0) |
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https://creativecommons.org/licenses/by/4.0/ |
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info:eu-repo/semantics/openAccess |
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Atribución 4.0 Internacional (CC BY 4.0) © 2024 https://creativecommons.org/licenses/by/4.0/ http://purl.org/coar/access_right/c_abf2 |
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Elsevier Ltd |
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Corporación Universidad de la Costa |
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Atribución 4.0 Internacional (CC BY 4.0)© 2024https://creativecommons.org/licenses/by/4.0/info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2AL-Zoubi, Omar H.Grimaldo Guerrero, John WilliamKhan, Ahmad RazaKumar, AshwaniOlegovich Bokov, DmitryJuraev, NizomiddinPramanik, AtreyiQasim, Maytham T.Redhee, Ahmeed hoseen2024-11-25T16:26:06Z2024-11-25T16:26:06Z2024-05-14Omar H. AL-Zoubi, John William Grimaldo Guerrero, Ahmad Raza Khan, Ashwani Kumar, Dmitry Olegovich Bokov, Nizomiddin Juraev, Atreyi Pramanik, Maytham T. Qasim, Ahmeed hoseen Redhee, Enhancing dye-sensitized solar cell performance: Optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes, Materials Science in Semiconductor Processing, Volume 179, 2024, 108526, ISSN 1369-8001, https://doi.org/10.1016/j.mssp.2024.108526.1369-8001https://hdl.handle.net/11323/1381210.1016/j.mssp.2024.1085261873-4081This study investigates the utilization of Cu2ZnSnS4/ZnCo2O4 (CZTS/ZCO) nanocomposites prepared through hydrothermal and combustion methods as counter electrodes in Dye-Sensitized Solar Cells (DSSCs). Different ratios of Cu2ZnSnS4 and ZnCo2O4 were explored, and comprehensive analyses were conducted using X-ray Diffraction (XRD), Transmission Electron Microscopy (TEM), High-Resolution TEM (HRTEM), Brunauer–Emmett–Teller (BET) surface area analysis, Raman Spectroscopy, Electrochemical Impedance Spectroscopy (EIS), cyclic voltammetry (CV), Tafel analysis, Field Emission Scanning Electron Microscopy (FESEM), and Incident Photon-to-Electron Conversion Efficiency (IPCE), alongside long-term stability assessments. The CZTS:ZCO ratio of 2:1 exhibited the highest efficiency, reaching 8.81 %, with an open-circuit voltage of 729 mV, short-circuit current of 17.80 mAcm−2, and a fill factor of 67.9 %. This surpasses the efficiency of the reference Pt cell (8.42 %), which had an open-circuit voltage of 735 mV, short-circuit current of 17.16 mAcm−2, and a fill factor of 66.8 %. The average crystallite sizes for the main peaks of CZTS and ZCO samples were estimated to be 19.8 and 16.7 nm, respectively. The crystallite size can significantly affect the charge transfer and conductivity in the counter electrode during electrochemical processes; the presence of nanocrystals with these sizes can notably enhance the electrochemical properties and conductivity of the synthesized samples. Raman analysis results indicate that no additional phases or secondary phases such as ZnS and CuSnS3 have formed in the kesterite CZTS structure, and the crystal has formed as a single phase. Additionally, the F2g modes in the Raman spectrum of ZCO indicate tetrahedral units in the spinel ZCO structure, and the A1g modes represent octahedral structures in this phase, indicating the formation of suitable ZCO phase. The superior performance of the CZTS/ZCO nanocomposite can be attributed to its enhanced crystalline structure, superior charge transport characteristics, and improved electrocatalytic behaviours.8 páginasapplication/pdfengElsevier LtdUnited Kingdomhttps://www.sciencedirect.com/science/article/pii/S1369800124004220?via%3DihubEnhancing dye-sensitized solar cell performance: optimizing Cu2ZnSnS4/ZnCo2O4 nanocomposites as efficient and cost-effective counter electrodes.Artículo de revistahttp://purl.org/coar/resource_type/c_2df8fbb1Textinfo:eu-repo/semantics/articlehttp://purl.org/redcol/resource_type/ARTinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/version/c_970fb48d4fbd8a85Materials Science in Semiconductor ProcessingM. Soltanmohammadi, V. Karimi, S. Alee, M. Abrari, M. Ahmadi, M. Ghanaatshoar Cu2ZnSnS4 thin film as a counter electrode in zinc stannate-based dye-sensitized solar cells Semicond. Sci. Technol., 36 (10) (2021), Article 105008X. Wang, B. Zhao, W. Kan, Y. Xie, K. Pan Review on low‐cost counter electrode materials for dye‐sensitized solar cells: effective strategy to improve photovoltaic performance Adv. Mater. Interfac., 9 (2) (2022), Article 2101229G. Richhariya, A. Kumar, A.K. Shukla, K. Shukla, B.C. Meikap Effect of different counter electrodes on power conversion efficiency of DSSCs J. Electron. Mater., 52 (1) (2023), pp. 60-71M. Ahmadi, S.J. Anaghizi, M. Asemi, M. Ghanaatshoar Plasma-treated room temperature synthesized CuCrO2/Au/CuCrO2 on Polyethylene terephthalate: towards a high-performance flexible p-type transparent conductor Thin Solid Films, 723 (2021), Article 138582M.M. Ibrahim, M.A. Hassan, K.I. Hassoon Novel route to prepare iron sulphide as a counter electrode for dye-sensitized solar cell Bull. Mater. Sci., 46 (3) (2023), p. 120Y. Hu, Y. Zheng, J. Jin, Y. Wang, Y. Peng, J. Yin, W. Shen, Y. Hou, L. Zhu, L. An Understanding the sulphur-oxygen exchange process of metal sulphides prior to oxygen evolution reaction Nat. Commun., 14 (1) (2023), p. 1949Z. Golshani, F. Arjmand, S. Maghsoudi, S.M.A. Hosseini Fe2O3–NiO doped carbon counter electrode for high-performance and long-term stable photovoltaic perovskite solar cells J. Mater. Res. Technol., 23 (2023), pp. 2612-2625D. Cao, Z. Li, Y. Xu, W. Li, H. Zhong, Y. Huang, X. Zhang, L. Wan, X. Zhang, Y. Li Interfacial engineering by p-methylphenylmethylammonium iodide for efficient carbon counter electrode (CE)-based 2D/3D hybrid perovskite solar cells Org. Electron., 113 (2023), Article 106699S. Ding, C. Yang, J. Yuan, H. Li, X. Yuan, M. Li An overview of the preparation and application of counter electrodes for DSSCs RSC Adv., 13 (18) (2023), pp. 12309-12319H. Pervaiz, Z.S. Khan, N. Shahzad, G. Ali, N. Iqbal, S. Javed Fabrication of cellulose paper-based counter electrodes for flexible dye-sensitized solar cells Phys. Chem. Chem. Phys., 25 (1) (2023), pp. 428-438Y. Kurokawa, T. Kato, S.S. Pandey Controlling the electrocatalytic activities of conducting polymer thin films toward suitability as cost-effective counter electrodes of dye-sensitized solar cells Synth. Met., 296 (2023), Article 117362A. Asok, K. Haribabu Synthesis and performance of polythiophene-iridium oxide composite as counter electrode in dye sensitized solar cell Curr. Appl. Phys., 49 (2023), pp. 64-69R.H. Althomali, E.A.M. Saleh, R.S. Bhat, S. Askar, I. Sapaev, M.A. Najm, B.M. Ridha, A.H. Alsalamy, R. Riyadh Novel ZnCo2O4/WO3 nanocomposite as the counter electrode for dye-sensitized solar cells (DSSCs): study of electrocatalytic activity and charge transfer properties Opt. Mater., 143 (2023), Article 114248K. Kaur, M. Patyal, N. Gupta, A. Kumar, M. Khanuja Graphene/macrocylic Yb nanocomposite as counter electrode in dye sensitized solar cell Opt. Mater., 139 (2023), Article 113831L. Mxakaza, G. Ngubeni, N. Moloto, Z. 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ara ejercer estos derechos sobre la Obra tal y como se indica a continuación:</p>
    <ol type="a">
      <li>Reproducir la Obra, incorporar la Obra en una o más Obras Colectivas, y reproducir la Obra incorporada en las Obras Colectivas.</li>
      <li>Distribuir copias o fonogramas de las Obras, exhibirlas públicamente, ejecutarlas públicamente y/o ponerlas a disposición pública, incluyéndolas como incorporadas en Obras Colectivas, según corresponda.</li>
      <li>Distribuir copias de las Obras Derivadas que se generen, exhibirlas públicamente, ejecutarlas públicamente y/o ponerlas a disposición pública.</li>
    </ol>
    <p>Los derechos mencionados anteriormente pueden ser ejercidos en todos los medios y formatos, actualmente conocidos o que se inventen en el futuro. Los derechos antes mencionados incluyen el derecho a realizar dichas modificaciones en la medida que sean técnicamente necesarias para ejercer los derechos en otro medio o formatos, pero de otra manera usted no está autorizado para realizar obras derivadas. Todos los derechos no otorgados expresamente por el Licenciante quedan por este medio reservados, incluyendo pero sin limitarse a aquellos que se mencionan en las secciones 4(d) y 4(e).</p>
  </li>
  <br/>
  <li>
    Restricciones.
    <p>La licencia otorgada en la anterior Sección 3 está expresamente sujeta y limitada por las siguientes restricciones:</p>
    <ol type="a">
      <li>Usted puede distribuir, exhibir públicamente, ejecutar públicamente, o poner a disposición pública la Obra sólo bajo las condiciones de esta Licencia, y Usted debe incluir una copia de esta licencia o del Identificador Universal de Recursos de la misma con cada copia de la Obra que distribuya, exhiba públicamente, ejecute públicamente o ponga a disposición pública. No es posible ofrecer o imponer ninguna condición sobre la Obra que altere o limite las condiciones de esta Licencia o el ejercicio de los derechos de los destinatarios otorgados en este documento. No es posible sublicenciar la Obra. Usted debe mantener intactos todos los avisos que hagan referencia a esta Licencia y a la cláusula de limitación de garantías. Usted no puede distribuir, exhibir públicamente, ejecutar públicamente, o poner a disposición pública la Obra con alguna medida tecnológica que controle el acceso o la utilización de ella de una forma que sea inconsistente con las condiciones de esta Licencia. Lo anterior se aplica a la Obra incorporada a una Obra Colectiva, pero esto no exige que la Obra Colectiva aparte de la obra misma quede sujeta a las condiciones de esta Licencia. Si Usted crea una Obra Colectiva, previo aviso de cualquier Licenciante debe, en la medida de lo posible, eliminar de la Obra Colectiva cualquier referencia a dicho Licenciante o al Autor Original, según lo solicitado por el Licenciante y conforme lo exige la cláusula 4(c).</li>
      <li>Usted no puede ejercer ninguno de los derechos que le han sido otorgados en la Sección 3 precedente de modo que estén principalmente destinados o directamente dirigidos a conseguir un provecho comercial o una compensación monetaria privada. El intercambio de la Obra por otras obras protegidas por derechos de autor, ya sea a través de un sistema para compartir archivos digitales (digital file-sharing) o de cualquier otra manera no será considerado como estar destinado principalmente o dirigido directamente a conseguir un provecho comercial o una compensación monetaria privada, siempre que no se realice un pago mediante una compensación monetaria en relación con el intercambio de obras protegidas por el derecho de autor.</li>
      <li>Si usted distribuye, exhibe públicamente, ejecuta públicamente o ejecuta públicamente en forma digital la Obra o cualquier Obra Derivada u Obra Colectiva, Usted debe mantener intacta toda la información de derecho de autor de la Obra y proporcionar, de forma razonable según el medio o manera que Usted esté utilizando: (i) el nombre del Autor Original si está provisto (o seudónimo, si fuere aplicable), y/o (ii) el nombre de la parte o las partes que el Autor Original y/o el Licenciante hubieren designado para la atribución (v.g., un instituto patrocinador, editorial, publicación) en la información de los derechos de autor del Licenciante, términos de servicios o de otras formas razonables; el título de la Obra si está provisto; en la medida de lo razonablemente factible y, si está provisto, el Identificador Uniforme de Recursos (Uniform Resource Identifier) que el Licenciante especifica para ser asociado con la Obra, salvo que tal URI no se refiera a la nota sobre los derechos de autor o a la información sobre el licenciamiento de la Obra; y en el caso de una Obra Derivada, atribuir el crédito identificando el uso de la Obra en la Obra Derivada (v.g., "Traducción Francesa de la Obra del Autor Original," o "Guión Cinematográfico basado en la Obra original del Autor Original"). Tal crédito puede ser implementado de cualquier forma razonable; en el caso, sin embargo, de Obras Derivadas u Obras Colectivas, tal crédito aparecerá, como mínimo, donde aparece el crédito de cualquier otro autor comparable y de una manera, al menos, tan destacada como el crédito de otro autor comparable.</li>
      <li>
        Para evitar toda confusión, el Licenciante aclara que, cuando la obra es una composición musical:
        <ol type="i">
          <li>Regalías por interpretación y ejecución bajo licencias generales. El Licenciante se reserva el derecho exclusivo de autorizar la ejecución pública o la ejecución pública digital de la obra y de recolectar, sea individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, SAYCO), las regalías por la ejecución pública o por la ejecución pública digital de la obra (por ejemplo Webcast) licenciada bajo licencias generales, si la interpretación o ejecución de la obra está primordialmente orientada por o dirigida a la obtención de una ventaja comercial o una compensación monetaria privada.</li>
          <li>Regalías por Fonogramas. El Licenciante se reserva el derecho exclusivo de recolectar, individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, los consagrados por la SAYCO), una agencia de derechos musicales o algún agente designado, las regalías por cualquier fonograma que Usted cree a partir de la obra (“versión cover”) y distribuya, en los términos del régimen de derechos de autor, si la creación o distribución de esa versión cover está primordialmente destinada o dirigida a obtener una ventaja comercial o una compensación monetaria privada.</li>
        </ol>
      </li>
      <li>Gestión de Derechos de Autor sobre Interpretaciones y Ejecuciones Digitales (WebCasting). Para evitar toda confusión, el Licenciante aclara que, cuando la obra sea un fonograma, el Licenciante se reserva el derecho exclusivo de autorizar la ejecución pública digital de la obra (por ejemplo, webcast) y de recolectar, individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, ACINPRO), las regalías por la ejecución pública digital de la obra (por ejemplo, webcast), sujeta a las disposiciones aplicables del régimen de Derecho de Autor, si esta ejecución pública digital está primordialmente dirigida a obtener una ventaja comercial o una compensación monetaria privada.</li>
    </ol>
  </li>
  <br/>
  <li>
    Representaciones, Garantías y Limitaciones de Responsabilidad.
    <p>A MENOS QUE LAS PARTES LO ACORDARAN DE OTRA FORMA POR ESCRITO, EL LICENCIANTE OFRECE LA OBRA (EN EL ESTADO EN EL QUE SE ENCUENTRA) “TAL CUAL”, SIN BRINDAR GARANTÍAS DE CLASE ALGUNA RESPECTO DE LA OBRA, YA SEA EXPRESA, IMPLÍCITA, LEGAL O CUALQUIERA OTRA, INCLUYENDO, SIN LIMITARSE A ELLAS, GARANTÍAS DE TITULARIDAD, COMERCIABILIDAD, ADAPTABILIDAD O ADECUACIÓN A PROPÓSITO DETERMINADO, AUSENCIA DE INFRACCIÓN, DE AUSENCIA DE DEFECTOS LATENTES O DE OTRO TIPO, O LA PRESENCIA O AUSENCIA DE ERRORES, SEAN O NO DESCUBRIBLES (PUEDAN O NO SER ESTOS DESCUBIERTOS). ALGUNAS JURISDICCIONES NO PERMITEN LA EXCLUSIÓN DE GARANTÍAS IMPLÍCITAS, EN CUYO CASO ESTA EXCLUSIÓN PUEDE NO APLICARSE A USTED.</p>
  </li>
  <br/>
  <li>
    Limitación de responsabilidad.
    <p>A MENOS QUE LO EXIJA EXPRESAMENTE LA LEY APLICABLE, EL LICENCIANTE NO SERÁ RESPONSABLE ANTE USTED POR DAÑO ALGUNO, SEA POR RESPONSABILIDAD EXTRACONTRACTUAL, PRECONTRACTUAL O CONTRACTUAL, OBJETIVA O SUBJETIVA, SE TRATE DE DAÑOS MORALES O PATRIMONIALES, DIRECTOS O INDIRECTOS, PREVISTOS O IMPREVISTOS PRODUCIDOS POR EL USO DE ESTA LICENCIA O DE LA OBRA, AUN CUANDO EL LICENCIANTE HAYA SIDO ADVERTIDO DE LA POSIBILIDAD DE DICHOS DAÑOS. ALGUNAS LEYES NO PERMITEN LA EXCLUSIÓN DE CIERTA RESPONSABILIDAD, EN CUYO CASO ESTA EXCLUSIÓN PUEDE NO APLICARSE A USTED.</p>
  </li>
  <br/>
  <li>
    Término.
    <ol type="a">
      <li>Esta Licencia y los derechos otorgados en virtud de ella terminarán automáticamente si Usted infringe alguna condición establecida en ella. Sin embargo, los individuos o entidades que han recibido Obras Derivadas o Colectivas de Usted de conformidad con esta Licencia, no verán terminadas sus licencias, siempre que estos individuos o entidades sigan cumpliendo íntegramente las condiciones de estas licencias. Las Secciones 1, 2, 5, 6, 7, y 8 subsistirán a cualquier terminación de esta Licencia.</li>
      <li>Sujeta a las condiciones y términos anteriores, la licencia otorgada aquí es perpetua (durante el período de vigencia de los derechos de autor de la obra). No obstante lo anterior, el Licenciante se reserva el derecho a publicar y/o estrenar la Obra bajo condiciones de licencia diferentes o a dejar de distribuirla en los términos de esta Licencia en cualquier momento; en el entendido, sin embargo, que esa elección no servirá para revocar esta licencia o que deba ser otorgada , bajo los términos de esta licencia), y esta licencia continuará en pleno vigor y efecto a menos que sea terminada como se expresa atrás. La Licencia revocada continuará siendo plenamente vigente y efectiva si no se le da término en las condiciones indicadas anteriormente.</li>
    </ol>
  </li>
  <br/>
  <li>
    Varios.
    <ol type="a">
      <li>Cada vez que Usted distribuya o ponga a disposición pública la Obra o una Obra Colectiva, el Licenciante ofrecerá al destinatario una licencia en los mismos términos y condiciones que la licencia otorgada a Usted bajo esta Licencia.</li>
      <li>Si alguna disposición de esta Licencia resulta invalidada o no exigible, según la legislación vigente, esto no afectará ni la validez ni la aplicabilidad del resto de condiciones de esta Licencia y, sin acción adicional por parte de los sujetos de este acuerdo, aquélla se entenderá reformada lo mínimo necesario para hacer que dicha disposición sea válida y exigible.</li>
      <li>Ningún término o disposición de esta Licencia se estimará renunciada y ninguna violación de ella será consentida a menos que esa renuncia o consentimiento sea otorgado por escrito y firmado por la parte que renuncie o consienta.</li>
      <li>Esta Licencia refleja el acuerdo pleno entre las partes respecto a la Obra aquí licenciada. No hay arreglos, acuerdos o declaraciones respecto a la Obra que no estén especificados en este documento. El Licenciante no se verá limitado por ninguna disposición adicional que pueda surgir en alguna comunicación emanada de Usted. Esta Licencia no puede ser modificada sin el consentimiento mutuo por escrito del Licenciante y Usted.</li>
    </ol>
  </li>
  <br/>
</ol>
 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