Yerin Lee, Hoyoung Song, Dongjin Choi, MyeongSeob Sim, Donghwan Kim, Yoonmook Kang, Hae-Seok Lee
Tunnel oxide passivated contact (TOPCon) solar cells achieve efficiencies exceeding 26% by incorporating a heavily doped poly-Si layer with a tunnel oxide, with recent efforts focusing on enhancing the rear passivation structure. In industrial TOPCon cells, the high-temperature firing process during metal contact formation degrades the passivation quality of poly-Si/SiOx contacts, necessitating improvements to maintain cell performance. While previous studies examine degradation factors related to the rear structure, research on mechanisms driven by the firing process remains limited. This study identifies how excess hydrogen, rather than phosphorus in-diffusion, degrades passivation quality by diffusing from SiNx into SiOx during the firing process. Thermal stress during the firing process dissociates c-Si/SiOx bonds, while interstitial hydrogen accumulates at the SiOx interface and forms hydrogen pores as defects, reducing passivation quality. To mitigate this, we introduce an Al2O3 layer as a hydrogen diffusion barrier, effectively preventing hydrogen diffusion into SiOx. This approach increases the implied open-circuit voltage (iVoc) after firing, achieving a record 729.8 mV with Al2O3/SiNx double passivation layers. These findings advance the understanding of degradation mechanisms in industrial TOPCon solar cells during firing and offer practical strategies for optimizing industrial-scale solar cell manufacturing.
{"title":"Improving the Performance of Bifacial Tunnel Oxide Passivated Contact Solar Cells: Insights into Firing-Induced Degradation Mechanisms","authors":"Yerin Lee, Hoyoung Song, Dongjin Choi, MyeongSeob Sim, Donghwan Kim, Yoonmook Kang, Hae-Seok Lee","doi":"10.1002/solr.202400860","DOIUrl":"https://doi.org/10.1002/solr.202400860","url":null,"abstract":"<p>\u0000Tunnel oxide passivated contact (TOPCon) solar cells achieve efficiencies exceeding 26% by incorporating a heavily doped poly-Si layer with a tunnel oxide, with recent efforts focusing on enhancing the rear passivation structure. In industrial TOPCon cells, the high-temperature firing process during metal contact formation degrades the passivation quality of poly-Si/SiO<sub><i>x</i></sub> contacts, necessitating improvements to maintain cell performance. While previous studies examine degradation factors related to the rear structure, research on mechanisms driven by the firing process remains limited. This study identifies how excess hydrogen, rather than phosphorus in-diffusion, degrades passivation quality by diffusing from SiN<sub><i>x</i></sub> into SiO<sub><i>x</i></sub> during the firing process. Thermal stress during the firing process dissociates c-Si/SiO<sub><i>x</i></sub> bonds, while interstitial hydrogen accumulates at the SiO<i><sub>x</sub></i> interface and forms hydrogen pores as defects, reducing passivation quality. To mitigate this, we introduce an Al<sub>2</sub>O<sub>3</sub> layer as a hydrogen diffusion barrier, effectively preventing hydrogen diffusion into SiO<sub><i>x</i></sub>. This approach increases the implied open-circuit voltage (iV<sub>oc</sub>) after firing, achieving a record 729.8 mV with Al<sub>2</sub>O<sub>3</sub>/SiN<sub><i>x</i></sub> double passivation layers. These findings advance the understanding of degradation mechanisms in industrial TOPCon solar cells during firing and offer practical strategies for optimizing industrial-scale solar cell manufacturing.</p>","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 6","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-03-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143688823","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Zhengjie Xu, Jianing Wang, Qiang Lou, Yufeng Jin, Hong Meng, Hang Zhou
Poly(3-hexylthiophene) (P3HT) has attracted significant interest due to its cost-effective synthesis, high purity, and stable film properties. However, the efficiency of perovskite solar cells is limited by energy-level mismatches and nonradiative recombination at the P3HT/perovskite interface. In this study, we introduce the 2,7-dimetapyridinebenzo[4,5]thieno[3,2-b]benzofuran (Mpy-BTBF) small molecule, which features extended π-conjugation and lone pair electrons from oxygen and sulfur atoms. Incorporating Mpy-BTBF into P3HT (M-P3HT) improves charge transport and passivates iodine-related defects, achieving a power conversion efficiency (PCE) of 16.36%, surpassing the pristine P3HT-based device (14.49%). With further Li salts doping, the champion PCE increased to 21.24 from 17.30%. Finally, M-P3HT-based devices maintained over 70% of their efficiency after 600 h of aging at 60% relative humidity and 60°C.
{"title":"Tailoring Iodide-Capturing Molecules for High-Performance Perovskite Solar Cells Based on P3HT","authors":"Zhengjie Xu, Jianing Wang, Qiang Lou, Yufeng Jin, Hong Meng, Hang Zhou","doi":"10.1002/solr.202400901","DOIUrl":"https://doi.org/10.1002/solr.202400901","url":null,"abstract":"<p>Poly(3-hexylthiophene) (P3HT) has attracted significant interest due to its cost-effective synthesis, high purity, and stable film properties. However, the efficiency of perovskite solar cells is limited by energy-level mismatches and nonradiative recombination at the P3HT/perovskite interface. In this study, we introduce the 2,7-dimetapyridinebenzo[4,5]thieno[3,2-b]benzofuran (Mpy-BTBF) small molecule, which features extended <i>π</i>-conjugation and lone pair electrons from oxygen and sulfur atoms. Incorporating Mpy-BTBF into P3HT (M-P3HT) improves charge transport and passivates iodine-related defects, achieving a power conversion efficiency (PCE) of 16.36%, surpassing the pristine P3HT-based device (14.49%). With further Li salts doping, the champion PCE increased to 21.24 from 17.30%. Finally, M-P3HT-based devices maintained over 70% of their efficiency after 600 h of aging at 60% relative humidity and 60°C.</p>","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 7","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143762176","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Xinjie Liu, Yanqing Zhu, Bo Zhang, Jiahui Chen, Bingxin Duan, Min Hu, Peiran Hou, Junye Pan, Yuchen Pan, Qiqing Luo, Yanxi Li, Yijie Wang, Kan Liu, Jianfeng Lu
Scaling up high-performance perovskite solar cells (PSCs) while avoiding losses in the power conversion efficiency (PCE) is a challenging task. Surface passivation of the perovskite film has been demonstrated as an effective strategy to mitigate PCE losses. However, there is limited research on scalable surface passivation techniques. Herein, we studied how to develop a slot-die coating technique applying for passivation layers to PSCs, which can be adapted for industrial-scale production. Molecular structure of passivators and coating parameters have been systematically optimized to achieve high-quality film morphology, which enable effectively inhibition of interface recombination. As a result, champion efficiencies of 22.4% for small-size solar cells (0.16 cm2) and 18.3% for solar modules (10.0 cm2) have been achieved with 4-bromophenethylammonium chloride. Moreover, the encapsulated solar cells retained 89% of their initial performance after continuous operation under 100 mW·cm2 illumination for 400 h.
{"title":"Slot-Die Coating of Ammonium Salt Passivation Layer for High-Performance Perovskite Solar Cells and Modules","authors":"Xinjie Liu, Yanqing Zhu, Bo Zhang, Jiahui Chen, Bingxin Duan, Min Hu, Peiran Hou, Junye Pan, Yuchen Pan, Qiqing Luo, Yanxi Li, Yijie Wang, Kan Liu, Jianfeng Lu","doi":"10.1002/solr.202400896","DOIUrl":"https://doi.org/10.1002/solr.202400896","url":null,"abstract":"<p>Scaling up high-performance perovskite solar cells (PSCs) while avoiding losses in the power conversion efficiency (PCE) is a challenging task. Surface passivation of the perovskite film has been demonstrated as an effective strategy to mitigate PCE losses. However, there is limited research on scalable surface passivation techniques. Herein, we studied how to develop a slot-die coating technique applying for passivation layers to PSCs, which can be adapted for industrial-scale production. Molecular structure of passivators and coating parameters have been systematically optimized to achieve high-quality film morphology, which enable effectively inhibition of interface recombination. As a result, champion efficiencies of 22.4% for small-size solar cells (0.16 cm<sup>2</sup>) and 18.3% for solar modules (10.0 cm<sup>2</sup>) have been achieved with 4-bromophenethylammonium chloride. Moreover, the encapsulated solar cells retained 89% of their initial performance after continuous operation under 100 mW·cm<sup>2</sup> illumination for 400 h.</p>","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 6","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-02-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143690177","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The development of efficient photothermal materials for solar steam generation (SSG) garners significant interest as a solution to the global clean water scarcity crisis. Photothermal properties of organic molecules can be fine-tuned by molecular design. Despite this fact, the use of organic small-molecular photothermal materials in SSG applications is seldom explored due to their limited optical absorption range for solar energy harvesting. In this research, 6,6,12,12-tetrakis(4-octylphenyl)dithieno[2,3-d:2′,3′-d′]-s-indaceno[1,2-b:5,6-b′]dithiophene (DTIDT) is focused upon as the potent conjugated core unit, and the [2 + 2] cycloaddition–retroelectrocyclization (CA-RE) reaction is applied to introduce additional intramolecular charge-transfer chromophores. DTIDT derivatives exhibit broad optical absorption, weak photoluminescence, and high nonradiative decay rates, which are useful for efficient photothermal conversion. In addition, the DTIDT derivatives are placed on the top surface of a filter paper, and the SSG devices are fabricated as a Janus membrane to enhance the solar-to-vapor efficiency. The DTIDT derivatives produced by the [2 + 2] CA-RE exhibit a maximum efficiency of 78.3% under simulated sunlight irradiation for 30 min. The result suggests that the CA-RE reaction is an effective method for synthesizing organic photothermal materials tailored for SSG applications.
{"title":"Enhanced Photothermal Property of Dithienoindacenodithiophene Molecules by [2 + 2] Cycloaddition–Retroelectrocyclization Reaction for Efficient Solar Steam Generation","authors":"Chia-Yang Lin, Shohei Shimizu, Yoshimitsu Sagara, Hidetoshi Matsumoto, Tsuyoshi Michinobu","doi":"10.1002/solr.202400803","DOIUrl":"https://doi.org/10.1002/solr.202400803","url":null,"abstract":"<p>The development of efficient photothermal materials for solar steam generation (SSG) garners significant interest as a solution to the global clean water scarcity crisis. Photothermal properties of organic molecules can be fine-tuned by molecular design. Despite this fact, the use of organic small-molecular photothermal materials in SSG applications is seldom explored due to their limited optical absorption range for solar energy harvesting. In this research, 6,6,12,12-tetrakis(4-octylphenyl)dithieno[2,3-<i>d</i>:2′,3′-<i>d</i>′]-<i>s</i>-indaceno[1,2-<i>b</i>:5,6-<i>b</i>′]dithiophene (DTIDT) is focused upon as the potent conjugated core unit, and the [2 + 2] cycloaddition–retroelectrocyclization (CA-RE) reaction is applied to introduce additional intramolecular charge-transfer chromophores. DTIDT derivatives exhibit broad optical absorption, weak photoluminescence, and high nonradiative decay rates, which are useful for efficient photothermal conversion. In addition, the DTIDT derivatives are placed on the top surface of a filter paper, and the SSG devices are fabricated as a Janus membrane to enhance the solar-to-vapor efficiency. The DTIDT derivatives produced by the [2 + 2] CA-RE exhibit a maximum efficiency of 78.3% under simulated sunlight irradiation for 30 min. The result suggests that the CA-RE reaction is an effective method for synthesizing organic photothermal materials tailored for SSG applications.</p>","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 5","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-02-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/solr.202400803","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143571198","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fengshi Chen, Yao Wang, Abd. Rashid bin Mohd Yusoff, Yaming Yu, Peng Gao
Solar energy, as a renewable resource, offers an excellent solution to the increasing global energy demand. Solar cells convert solar energy into electricity, prompting extensive research in this field in recent years. However, enhancing solar cell efficiency presents several challenges. Currently, solar cells can only utilize a limited portion of the solar spectrum, as most UV and infrared light remain unabsorbed. Additionally, UV light can compromise the stability of solar cells. Therefore, optimizing the utilization of solar photons across the spectrum is essential for improving both the efficiency and stability of these devices. Down-conversion (DC) technology, also known as quantum cutting, effectively enhances the spectral absorption of solar cells, thereby increasing their efficiency and stability. Rare earth ions, with their unique electronic configurations and optical properties, are pivotal in DC research related to solar cells. This review discusses the principles of DC technology and the synthesis of DC materials, emphasizing the application of rare earth-based DC materials in enhancing the efficiency and stability of various types of solar cells and their role in modifying the solar spectrum.
{"title":"Unlocking the Potential of Rare Earth-Doped Down-Conversion Materials for Enhanced Solar Cell Performance and Durability","authors":"Fengshi Chen, Yao Wang, Abd. Rashid bin Mohd Yusoff, Yaming Yu, Peng Gao","doi":"10.1002/solr.202400798","DOIUrl":"https://doi.org/10.1002/solr.202400798","url":null,"abstract":"<p>Solar energy, as a renewable resource, offers an excellent solution to the increasing global energy demand. Solar cells convert solar energy into electricity, prompting extensive research in this field in recent years. However, enhancing solar cell efficiency presents several challenges. Currently, solar cells can only utilize a limited portion of the solar spectrum, as most UV and infrared light remain unabsorbed. Additionally, UV light can compromise the stability of solar cells. Therefore, optimizing the utilization of solar photons across the spectrum is essential for improving both the efficiency and stability of these devices. Down-conversion (DC) technology, also known as quantum cutting, effectively enhances the spectral absorption of solar cells, thereby increasing their efficiency and stability. Rare earth ions, with their unique electronic configurations and optical properties, are pivotal in DC research related to solar cells. This review discusses the principles of DC technology and the synthesis of DC materials, emphasizing the application of rare earth-based DC materials in enhancing the efficiency and stability of various types of solar cells and their role in modifying the solar spectrum.</p>","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 5","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-02-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143571199","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Sujung Park, Febrian Tri Adhi Wibowo, Dohui Kim, Jina Roe, Jin Hee Lee, Jung Hwa Seo, Jin Young Kim, Sung-Yeon Jang, Shinuk Cho
The widely used ZnO electron transport layer in inverted nonfullerene organic solar cells (nf-OSCs) offers advantages such as excellent electron mobility and optical transparency. However, challenges arise from surface defects in solution-processed ZnO, where oxygen-containing defects can penetrate the photoactive layer, leading to photocatalytic reactions with nonfullerene acceptors under UV light, thereby compromising device stability. Another challenge is that most recent high-efficiency nf-OSCs employ conventional structures, while inverted structures exhibit comparatively lower performance. To develop stable and high-performance inverted nf-OSCs, interface modification is essential to mitigate photocatalytic issues and enhance the relatively lower power conversion efficiency (PCE). To overcome these limitations, we introduce bathophenanthroline (BPhen) doped with Cs2CO3. The BPhen:Cs2CO3 layer creates suitable energy levels, enhancing electron transport and reducing charge recombination. This approach significantly improves current density and fill factor, resulting in a notable enhancement in the PCE of pristine ZnO devices from 15.54% to 17.09% in PM6:Y6 inverted nf-OSCs. Furthermore, ZnO/BPhen:Cs2CO3 devices exhibit excellent stability, retaining ~83% of their initial efficiency even after 1000 h without encapsulation, showcasing superior stability compared to pristine ZnO-based devices.
{"title":"Interface Engineering with BPhen:Cs2CO3 for High-Performance and Stable Inverted Nonfullerene Organic Solar Cells","authors":"Sujung Park, Febrian Tri Adhi Wibowo, Dohui Kim, Jina Roe, Jin Hee Lee, Jung Hwa Seo, Jin Young Kim, Sung-Yeon Jang, Shinuk Cho","doi":"10.1002/solr.202400902","DOIUrl":"https://doi.org/10.1002/solr.202400902","url":null,"abstract":"<p>The widely used ZnO electron transport layer in inverted nonfullerene organic solar cells (nf-OSCs) offers advantages such as excellent electron mobility and optical transparency. However, challenges arise from surface defects in solution-processed ZnO, where oxygen-containing defects can penetrate the photoactive layer, leading to photocatalytic reactions with nonfullerene acceptors under UV light, thereby compromising device stability. Another challenge is that most recent high-efficiency nf-OSCs employ conventional structures, while inverted structures exhibit comparatively lower performance. To develop stable and high-performance inverted nf-OSCs, interface modification is essential to mitigate photocatalytic issues and enhance the relatively lower power conversion efficiency (PCE). To overcome these limitations, we introduce bathophenanthroline (BPhen) doped with Cs<sub>2</sub>CO<sub>3</sub>. The BPhen:Cs<sub>2</sub>CO<sub>3</sub> layer creates suitable energy levels, enhancing electron transport and reducing charge recombination. This approach significantly improves current density and fill factor, resulting in a notable enhancement in the PCE of pristine ZnO devices from 15.54% to 17.09% in PM6:Y6 inverted nf-OSCs. Furthermore, ZnO/BPhen:Cs<sub>2</sub>CO<sub>3</sub> devices exhibit excellent stability, retaining ~83% of their initial efficiency even after 1000 h without encapsulation, showcasing superior stability compared to pristine ZnO-based devices.</p>","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 6","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143688883","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In the quest for advancing photovoltaic efficiency, the adoption of multijunction solar cell architectures has emerged as a promising approach. Perovskite/silicon double-junction solar cells have already achieved efficiencies surpassing 33%, exceeding the theoretical efficiency limit for single-junction devices. To enhance efficiency even further, exploring perovskite/perovskite/silicon (PPS) triple-junction solar cells seems a logical next step, as they offer the potential to further reduce thermalization losses and achieve even higher efficiencies. This study delves into the potential of various configurations of PPS modules, exploring different subcell interconnections. Initially, we present an optoelectrical model to simulate the performance of these devices, incorporating both luminescence coupling and cell-to-module losses. This enables us to optimize the bandgap energy of the top and middle perovskite subcells under both standard test conditions (STC) and outdoor conditions. Our analysis reveals that the addition of a perovskite subcell can improve the STC efficiency up to 9%–13%. This gain in STC performance also translates into a similar gain in energy yield, meaning that triple-junction devices produce 8%–14% more electricity than their double-junction reference devices.
{"title":"Exploring the Potential of Perovskite/Perovskite/Silicon Triple-Junction Pv Modules in Two- and Four-Terminal Configuration","authors":"Youri Blom, Malte Ruben Vogt, Hisashi Uzu, Gensuke Koizumi, Kenji Yamamoto, Olindo Isabella, Rudi Santbergen","doi":"10.1002/solr.202400613","DOIUrl":"https://doi.org/10.1002/solr.202400613","url":null,"abstract":"<p>In the quest for advancing photovoltaic efficiency, the adoption of multijunction solar cell architectures has emerged as a promising approach. Perovskite/silicon double-junction solar cells have already achieved efficiencies surpassing 33%, exceeding the theoretical efficiency limit for single-junction devices. To enhance efficiency even further, exploring perovskite/perovskite/silicon (PPS) triple-junction solar cells seems a logical next step, as they offer the potential to further reduce thermalization losses and achieve even higher efficiencies. This study delves into the potential of various configurations of PPS modules, exploring different subcell interconnections. Initially, we present an optoelectrical model to simulate the performance of these devices, incorporating both luminescence coupling and cell-to-module losses. This enables us to optimize the bandgap energy of the top and middle perovskite subcells under both standard test conditions (STC) and outdoor conditions. Our analysis reveals that the addition of a perovskite subcell can improve the STC efficiency up to 9%–13%. This gain in STC performance also translates into a similar gain in energy yield, meaning that triple-junction devices produce 8%–14% more electricity than their double-junction reference devices.</p>","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 5","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/solr.202400613","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143571385","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The rising demand for sustainable low-power devices has driven interest in indoor photovoltaic (IPV) technologies for Internet of Things (IoT) applications. Composed of earth-abundant and non-toxic elements, Kesterite-based Cu2ZnSnS4 (CZTS) solar cells are highly attractive for IPV. This study systematically investigates the effects of sodium (Na), lithium (Li), and Na–Li co-doping on solution-processed CZTS devices. A comprehensive analysis reveals that Na-doping substantially improves crystallinity and grain morphology, significantly boosting efficiency, whereas Li alone has minimal impact. Notably, Na–Li co-doping achieves a 10.1% efficiency under AM 1.5G illumination, outperforming both the reference and singly doped devices. The co-doping synergy arises from Na-induced grain growth and Li-induced defect passivation and carrier concentration regulation. These devices exhibit high adaptability under 20 different indoor lighting conditions representative of real-world environments, achieving up to 15.1% power conversion efficiency under 3000 K illumination at 2.93 mW cm−2;—the highest reported indoor efficiency for CZTS cells. Their stable open-circuit voltage, high fill factor, and consistent efficiency across various color temperatures and intensities underline their suitability for IPV applications. Future work should focus on improving bandgap alignment with indoor light spectra to further enhance the efficiency of this eco-friendly technology for IoT energy solutions.
{"title":"Attaining 15.1% Efficiency in Cu2ZnSnS4 Solar Cells Under Indoor Conditions Through Sodium and Lithium Codoping","authors":"Yuancai Gong, Alex Jimenez-Arguijo, Ivan Caño, Romain Scaffidi, Claudia Malerba, Matteo Valentini, David Payno, Alejandro Navarro-Güell, Oriol Segura-Blanch, Denis Flandre, Bart Vermang, Alejandro Perez-Rodriguez, Sergio Giraldo, Marcel Placidi, Zacharie Jehl Li-Kao, Edgardo Saucedo","doi":"10.1002/solr.202400756","DOIUrl":"https://doi.org/10.1002/solr.202400756","url":null,"abstract":"<p>The rising demand for sustainable low-power devices has driven interest in indoor photovoltaic (IPV) technologies for Internet of Things (IoT) applications. Composed of earth-abundant and non-toxic elements, Kesterite-based Cu<sub>2</sub>ZnSnS<sub>4</sub> (CZTS) solar cells are highly attractive for IPV. This study systematically investigates the effects of sodium (Na), lithium (Li), and Na–Li co-doping on solution-processed CZTS devices. A comprehensive analysis reveals that Na-doping substantially improves crystallinity and grain morphology, significantly boosting efficiency, whereas Li alone has minimal impact. Notably, Na–Li co-doping achieves a 10.1% efficiency under AM 1.5G illumination, outperforming both the reference and singly doped devices. The co-doping synergy arises from Na-induced grain growth and Li-induced defect passivation and carrier concentration regulation. These devices exhibit high adaptability under 20 different indoor lighting conditions representative of real-world environments, achieving up to 15.1% power conversion efficiency under 3000 K illumination at 2.93 mW cm<sup>−2</sup>;—the highest reported indoor efficiency for CZTS cells. Their stable open-circuit voltage, high fill factor, and consistent efficiency across various color temperatures and intensities underline their suitability for IPV applications. Future work should focus on improving bandgap alignment with indoor light spectra to further enhance the efficiency of this eco-friendly technology for IoT energy solutions.</p>","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 4","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-02-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143513848","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Yuner Luo, Yanhao Wang, Siyi Liu, Shaojuan Bao, Jilei Wang, Shan-Ting Zhang, Li Tian, Shihua Huang, Dongdong Li
<p>Yuner Luo, Yanhao Wang, Siyi Liu, Shaojuan Bao, Jilei Wang, Shan-Ting Zhang, Li Tian, Shihua Huang, Dongdong Li (2024). Hydrogenation strategy for Al<sub>2</sub>O<sub>3</sub>/MoO<sub><i>x</i></sub> passivating contact in High-Efficiency Crystalline Silicon Solar Cells, <i>Solar RRL</i>, https://doi.org/10.1002/solr.202400740</p><p>In paragraph 3 of the “Results and Discussion” section, the text “The <i>Q</i><sub><i>f</i></sub> value for H*-Al<sub>2</sub>O<sub>3</sub> films was −4.74 × 10<sup>12</sup> cm<sup>−2</sup>, higher than the values for H-Al<sub>2</sub>O<sub>3</sub> (−4.63 × 10<sup>12 </sup>cm<sup>−2</sup>), Al<sub>2</sub>O<sub>3</sub> (−4.5 × 10<sup>12 </sup>cm<sup>−2</sup>), and H*-Al<sub>2</sub>O<sub>3</sub> (O<sub>3</sub>) (−4.41 × 10<sup>12 </sup>cm<sup>−2</sup>).” was incorrect. This should have read: “The <i>Q</i><sub>f</sub> value for H*-Al<sub>2</sub>O<sub>3</sub> films was −2.45 × 10<sup>10 </sup>cm<sup>−2</sup>, higher than the values for H-Al<sub>2</sub>O<sub>3</sub> (−1.64 × 10<sup>10 </sup>cm<sup>−2</sup>), Al<sub>2</sub>O<sub>3</sub> (−1.08 × 10<sup>10 </sup>cm<sup>−2</sup>), and H*-Al<sub>2</sub>O<sub>3</sub> (O<sub>3</sub>) (−9.6 × 10<sup>9 </sup>cm<sup>−2</sup>).”</p><p>In Note S1 of “Supporting Information”, the text “From formula 1, we can obtain the <i>Q</i><sub>f</sub> of Al<sub>2</sub>O<sub>3</sub> which equals to −4.5 × 10<sup>12 </sup>cm<sup>−2</sup> based on the <i>V</i><sub>fb</sub> = 1.21 V and the oxide capacitance <i>C</i><sub>ox</sub> = 7.47 × 10<sup>−12 </sup>F. The <i>Q</i><sub>f</sub> of H-Al<sub>2</sub>O<sub>3</sub> film calculated from the <i>V</i><sub>fb</sub> = 1.32 V and the oxide capacitance <i>C</i><sub>ox</sub> = 7.3 × 10<sup>−12 </sup>F is −4.63 × 10<sup>12 </sup>cm<sup>−2</sup>. The <i>Q</i><sub>f</sub> of H*-Al<sub>2</sub>O<sub>3</sub> film calculated from the <i>V</i><sub>fb</sub> = 1.18 V and the oxide capacitance <i>C</i><sub>ox</sub> = 7.98 × 10<sup>−12</sup> F is −4.74 × 10<sup>12</sup> cm<sup>−2</sup>. And the <i>Q</i><sub>f</sub> of H*-Al<sub>2</sub>O<sub>3</sub> (O<sub>3</sub>) film calculated from the <i>V</i><sub>fb</sub> = 1.31 V and the oxide capacitance <i>C</i><sub>ox</sub> = 6.98 × 10<sup>−12</sup> F is −4.41 × 10<sup>12 </sup>cm<sup>−2</sup>” was incorrect. This should have read: “From formula 1, we can obtain the <i>Q</i><sub>f</sub> of Al<sub>2</sub>O<sub>3</sub> which equals to −1.08 × 10<sup>10 </sup>cm<sup>−2</sup> based on the <i>V</i><sub>fb</sub> = −0.6 V and the oxide capacitance <i>C</i><sub>ox</sub> = 2.58 × 10<sup>−11</sup> F. The <i>Q</i><sub>f</sub> of H-Al<sub>2</sub>O<sub>3</sub> film calculated from the <i>V</i><sub>fb</sub> = −0.63 V and the oxide capacitance <i>C</i><sub>ox</sub> = 2.89 × 10<sup>−11</sup> F is −1.64 × 10<sup>10</sup> cm<sup>−2</sup>. The <i>Q</i><sub>f</sub> of H*-Al<sub>2</sub>O<sub>3</sub> film calculated from the <i>V</i><sub>fb</sub> = 0.63 V and the oxide capacitance <i>C</i><sub>ox</sub> = 3 × 10<sup>−11</sup> F is −2.45 × 10<sup>10</s
{"title":"Correction to “Hydrogenation Strategy for Al2O3/MoOx Passivating Contact in High-Efficiency Crystalline Silicon Solar Cells”","authors":"Yuner Luo, Yanhao Wang, Siyi Liu, Shaojuan Bao, Jilei Wang, Shan-Ting Zhang, Li Tian, Shihua Huang, Dongdong Li","doi":"10.1002/solr.202500031","DOIUrl":"https://doi.org/10.1002/solr.202500031","url":null,"abstract":"<p>Yuner Luo, Yanhao Wang, Siyi Liu, Shaojuan Bao, Jilei Wang, Shan-Ting Zhang, Li Tian, Shihua Huang, Dongdong Li (2024). Hydrogenation strategy for Al<sub>2</sub>O<sub>3</sub>/MoO<sub><i>x</i></sub> passivating contact in High-Efficiency Crystalline Silicon Solar Cells, <i>Solar RRL</i>, https://doi.org/10.1002/solr.202400740</p><p>In paragraph 3 of the “Results and Discussion” section, the text “The <i>Q</i><sub><i>f</i></sub> value for H*-Al<sub>2</sub>O<sub>3</sub> films was −4.74 × 10<sup>12</sup> cm<sup>−2</sup>, higher than the values for H-Al<sub>2</sub>O<sub>3</sub> (−4.63 × 10<sup>12 </sup>cm<sup>−2</sup>), Al<sub>2</sub>O<sub>3</sub> (−4.5 × 10<sup>12 </sup>cm<sup>−2</sup>), and H*-Al<sub>2</sub>O<sub>3</sub> (O<sub>3</sub>) (−4.41 × 10<sup>12 </sup>cm<sup>−2</sup>).” was incorrect. This should have read: “The <i>Q</i><sub>f</sub> value for H*-Al<sub>2</sub>O<sub>3</sub> films was −2.45 × 10<sup>10 </sup>cm<sup>−2</sup>, higher than the values for H-Al<sub>2</sub>O<sub>3</sub> (−1.64 × 10<sup>10 </sup>cm<sup>−2</sup>), Al<sub>2</sub>O<sub>3</sub> (−1.08 × 10<sup>10 </sup>cm<sup>−2</sup>), and H*-Al<sub>2</sub>O<sub>3</sub> (O<sub>3</sub>) (−9.6 × 10<sup>9 </sup>cm<sup>−2</sup>).”</p><p>In Note S1 of “Supporting Information”, the text “From formula 1, we can obtain the <i>Q</i><sub>f</sub> of Al<sub>2</sub>O<sub>3</sub> which equals to −4.5 × 10<sup>12 </sup>cm<sup>−2</sup> based on the <i>V</i><sub>fb</sub> = 1.21 V and the oxide capacitance <i>C</i><sub>ox</sub> = 7.47 × 10<sup>−12 </sup>F. The <i>Q</i><sub>f</sub> of H-Al<sub>2</sub>O<sub>3</sub> film calculated from the <i>V</i><sub>fb</sub> = 1.32 V and the oxide capacitance <i>C</i><sub>ox</sub> = 7.3 × 10<sup>−12 </sup>F is −4.63 × 10<sup>12 </sup>cm<sup>−2</sup>. The <i>Q</i><sub>f</sub> of H*-Al<sub>2</sub>O<sub>3</sub> film calculated from the <i>V</i><sub>fb</sub> = 1.18 V and the oxide capacitance <i>C</i><sub>ox</sub> = 7.98 × 10<sup>−12</sup> F is −4.74 × 10<sup>12</sup> cm<sup>−2</sup>. And the <i>Q</i><sub>f</sub> of H*-Al<sub>2</sub>O<sub>3</sub> (O<sub>3</sub>) film calculated from the <i>V</i><sub>fb</sub> = 1.31 V and the oxide capacitance <i>C</i><sub>ox</sub> = 6.98 × 10<sup>−12</sup> F is −4.41 × 10<sup>12 </sup>cm<sup>−2</sup>” was incorrect. This should have read: “From formula 1, we can obtain the <i>Q</i><sub>f</sub> of Al<sub>2</sub>O<sub>3</sub> which equals to −1.08 × 10<sup>10 </sup>cm<sup>−2</sup> based on the <i>V</i><sub>fb</sub> = −0.6 V and the oxide capacitance <i>C</i><sub>ox</sub> = 2.58 × 10<sup>−11</sup> F. The <i>Q</i><sub>f</sub> of H-Al<sub>2</sub>O<sub>3</sub> film calculated from the <i>V</i><sub>fb</sub> = −0.63 V and the oxide capacitance <i>C</i><sub>ox</sub> = 2.89 × 10<sup>−11</sup> F is −1.64 × 10<sup>10</sup> cm<sup>−2</sup>. The <i>Q</i><sub>f</sub> of H*-Al<sub>2</sub>O<sub>3</sub> film calculated from the <i>V</i><sub>fb</sub> = 0.63 V and the oxide capacitance <i>C</i><sub>ox</sub> = 3 × 10<sup>−11</sup> F is −2.45 × 10<sup>10</s","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 6","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-02-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/solr.202500031","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143689044","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Shamim Ahmmed, Md. Abdul Karim, Yulu He, Siliang Cao, Md. Emrul Kayesh, Kiyoto Matsuishi, Ashraful Islam
To commercialize perovskite solar cells (PSCs), it is crucial to develop cost-effective, dopant-free hole transport layers (HTLs) that can be processed at low temperatures. Herein, a dopant-free small molecular material 4,4′,4′-Tris[2-naphthyl(phenyl)amino]triphenylamine (2TNATA) was utilized in inverted PSCs as a HTL. The position of the highest occupied molecular orbital energy of 2TNATA is properly aligned with the perovskite valence band maximum. Moreover, 2TNATA can be processed at lower temperatures and shows excellent thermal stability. The lead (Pb) perovskite on 2TNATA exhibited superior crystallinity and morphology compared to the perovskite on poly(3,4-ethylenedioxythiophene) polystyrene sulfonate (PEDOT:PSS) and poly[bis(4-phenyl)(2,4,6-trimethylphenyl)amine] (PTAA). Furthermore, the carrier kinetics in 2TNATA-based PSCs was superior to PTAA and PEDOT:PSS-based PSCs. Consequently, an outstanding power conversion efficiency (PCE) of 20.58% was observed from the 2TNATA HTL-based 0.09 cm2 PSCs, while PTAA and PEDOT:PSS HTLs-based 0.09 cm2 PSCs showed PCE of 19.36% and 14.35%, respectively. Moreover, the 2TNATA HTL-based 1.0 cm2 PSCs demonstrated an impressive PCE of 20.04%. The results indicate that 2TNATA might be a promising HTL for the inexpensive and efficient inverted PSCs.
{"title":"Small Molecular Organic Hole Transport Layer for Efficient Inverted Perovskite Solar Cells","authors":"Shamim Ahmmed, Md. Abdul Karim, Yulu He, Siliang Cao, Md. Emrul Kayesh, Kiyoto Matsuishi, Ashraful Islam","doi":"10.1002/solr.202500017","DOIUrl":"https://doi.org/10.1002/solr.202500017","url":null,"abstract":"<p>To commercialize perovskite solar cells (PSCs), it is crucial to develop cost-effective, dopant-free hole transport layers (HTLs) that can be processed at low temperatures. Herein, a dopant-free small molecular material 4,4′,4′-Tris[2-naphthyl(phenyl)amino]triphenylamine (2TNATA) was utilized in inverted PSCs as a HTL. The position of the highest occupied molecular orbital energy of 2TNATA is properly aligned with the perovskite valence band maximum. Moreover, 2TNATA can be processed at lower temperatures and shows excellent thermal stability. The lead (Pb) perovskite on 2TNATA exhibited superior crystallinity and morphology compared to the perovskite on poly(3,4-ethylenedioxythiophene) polystyrene sulfonate (PEDOT:PSS) and poly[bis(4-phenyl)(2,4,6-trimethylphenyl)amine] (PTAA). Furthermore, the carrier kinetics in 2TNATA-based PSCs was superior to PTAA and PEDOT:PSS-based PSCs. Consequently, an outstanding power conversion efficiency (PCE) of 20.58% was observed from the 2TNATA HTL-based 0.09 cm<sup>2</sup> PSCs, while PTAA and PEDOT:PSS HTLs-based 0.09 cm<sup>2</sup> PSCs showed PCE of 19.36% and 14.35%, respectively. Moreover, the 2TNATA HTL-based 1.0 cm<sup>2</sup> PSCs demonstrated an impressive PCE of 20.04%. The results indicate that 2TNATA might be a promising HTL for the inexpensive and efficient inverted PSCs.</p>","PeriodicalId":230,"journal":{"name":"Solar RRL","volume":"9 7","pages":""},"PeriodicalIF":6.0,"publicationDate":"2025-02-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/solr.202500017","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143761938","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}