Sumaiya Parveen , Prem P. Singh , Madan S. Chauhan , Shiv P. Patel , Manish K. Singh , Dhirendra K. Chaudhary , Ravi S. Singh , Vidya N. Singh , Vineet K. Singh
{"title":"超薄钝化层(1nm)的带隙梯度策略使钙钛矿/CdTe串联太阳能电池的SRH电压损失更低","authors":"Sumaiya Parveen , Prem P. Singh , Madan S. Chauhan , Shiv P. Patel , Manish K. Singh , Dhirendra K. Chaudhary , Ravi S. Singh , Vidya N. Singh , Vineet K. Singh","doi":"10.1016/j.jpcs.2025.113187","DOIUrl":null,"url":null,"abstract":"<div><div>An experimentally demonstrated open-circuit voltage of a CdTe-based solar cell is only 904.8 mV, which is ∼235.2 mV lower than the Shockley–Queisser voltage limit. This voltage loss can be attributed to the factors such as radiative, nonradiative, and thermodynamic recombination losses. To circumvent the voltage loss issue, this study proposes a strategy of implementation a CdSe<sub>0.2</sub>Te<sub>0.8</sub> passivation layer in conjunction with graded bandgap absorber layers. Initially, we examined a device with a configuration of V<sub>2</sub>O<sub>5</sub>/CdTe/ZnSe in absence of passivation layer. This device resulted in a larger Shockley-Read-Hall (SRH) recombination voltage loss of 281 mV and a total voltage loss of 716 mV. We modified this device configuration by utilizing an ultrathin layer (1 nm) of CdSe<sub>0.2</sub>Te<sub>0.8</sub>, i.e., V<sub>2</sub>O<sub>5</sub>/CdTe/CdSe<sub>0.2</sub>Te<sub>0.8</sub>/ZnSe. An ultrathin layer of CdSe<sub>0.2</sub>Te<sub>0.8</sub> works as an effective passivation layer, substantially reducing the SRH recombination voltage loss to 46 mV from 281 mV. Interestingly, when a thicker layer of CdSe<sub>0.2</sub>Te<sub>0.8</sub> is utilized, it not only acts as a passivation layer but also functions as an absorber layer, creating a bandgap gradient. However, improving the grain boundary between CdSe<sub>0.2</sub>Te<sub>0.8</sub> and ZnSe is necessary to further cuts down to SRH recombination voltage loss below 46 mV. To overcome this issue, a thin window layer of CdS<sub>0.102</sub>Se<sub>0.336</sub>Te<sub>0.562</sub> has been incorporated in between CdSe<sub>0.2</sub>Te<sub>0.8</sub> and ZnSe, close to the front contact, which reduces the SRH recombination voltage loss to 20 mV. This SRH recombination voltage loss can be further minimized to zero from 20 mV when the back interface has been optimized. All simulation data have been justified by previous reported experimental finding to validate the proposed simulation models. Additionally, two-terminal and four-terminal perovskite/CdTe tandem configurations have also been proposed and simulated, yielding power conversion efficiency of 28.64 % and 29.80 %, respectively. These findings demonstrate the efficacy of passivation layer, double absorber layer, bandgap grading, window layer, and interface engineering in mitigating SRH recombination voltage loss, offering a roadmap for future perovskite/CdTe tandem solar cells.</div></div>","PeriodicalId":16811,"journal":{"name":"Journal of Physics and Chemistry of Solids","volume":"208 ","pages":"Article 113187"},"PeriodicalIF":4.9000,"publicationDate":"2025-09-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Bandgap gradient strategy with ultra-thin passivation layer (1 nm) enabling lower SRH voltage loss in perovskite/CdTe Tandem Solar Cells\",\"authors\":\"Sumaiya Parveen , Prem P. Singh , Madan S. Chauhan , Shiv P. Patel , Manish K. Singh , Dhirendra K. Chaudhary , Ravi S. Singh , Vidya N. Singh , Vineet K. Singh\",\"doi\":\"10.1016/j.jpcs.2025.113187\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>An experimentally demonstrated open-circuit voltage of a CdTe-based solar cell is only 904.8 mV, which is ∼235.2 mV lower than the Shockley–Queisser voltage limit. This voltage loss can be attributed to the factors such as radiative, nonradiative, and thermodynamic recombination losses. To circumvent the voltage loss issue, this study proposes a strategy of implementation a CdSe<sub>0.2</sub>Te<sub>0.8</sub> passivation layer in conjunction with graded bandgap absorber layers. Initially, we examined a device with a configuration of V<sub>2</sub>O<sub>5</sub>/CdTe/ZnSe in absence of passivation layer. This device resulted in a larger Shockley-Read-Hall (SRH) recombination voltage loss of 281 mV and a total voltage loss of 716 mV. We modified this device configuration by utilizing an ultrathin layer (1 nm) of CdSe<sub>0.2</sub>Te<sub>0.8</sub>, i.e., V<sub>2</sub>O<sub>5</sub>/CdTe/CdSe<sub>0.2</sub>Te<sub>0.8</sub>/ZnSe. An ultrathin layer of CdSe<sub>0.2</sub>Te<sub>0.8</sub> works as an effective passivation layer, substantially reducing the SRH recombination voltage loss to 46 mV from 281 mV. Interestingly, when a thicker layer of CdSe<sub>0.2</sub>Te<sub>0.8</sub> is utilized, it not only acts as a passivation layer but also functions as an absorber layer, creating a bandgap gradient. However, improving the grain boundary between CdSe<sub>0.2</sub>Te<sub>0.8</sub> and ZnSe is necessary to further cuts down to SRH recombination voltage loss below 46 mV. To overcome this issue, a thin window layer of CdS<sub>0.102</sub>Se<sub>0.336</sub>Te<sub>0.562</sub> has been incorporated in between CdSe<sub>0.2</sub>Te<sub>0.8</sub> and ZnSe, close to the front contact, which reduces the SRH recombination voltage loss to 20 mV. This SRH recombination voltage loss can be further minimized to zero from 20 mV when the back interface has been optimized. All simulation data have been justified by previous reported experimental finding to validate the proposed simulation models. Additionally, two-terminal and four-terminal perovskite/CdTe tandem configurations have also been proposed and simulated, yielding power conversion efficiency of 28.64 % and 29.80 %, respectively. These findings demonstrate the efficacy of passivation layer, double absorber layer, bandgap grading, window layer, and interface engineering in mitigating SRH recombination voltage loss, offering a roadmap for future perovskite/CdTe tandem solar cells.</div></div>\",\"PeriodicalId\":16811,\"journal\":{\"name\":\"Journal of Physics and Chemistry of Solids\",\"volume\":\"208 \",\"pages\":\"Article 113187\"},\"PeriodicalIF\":4.9000,\"publicationDate\":\"2025-09-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics and Chemistry of Solids\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0022369725006407\",\"RegionNum\":3,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics and Chemistry of Solids","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0022369725006407","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
Bandgap gradient strategy with ultra-thin passivation layer (1 nm) enabling lower SRH voltage loss in perovskite/CdTe Tandem Solar Cells
An experimentally demonstrated open-circuit voltage of a CdTe-based solar cell is only 904.8 mV, which is ∼235.2 mV lower than the Shockley–Queisser voltage limit. This voltage loss can be attributed to the factors such as radiative, nonradiative, and thermodynamic recombination losses. To circumvent the voltage loss issue, this study proposes a strategy of implementation a CdSe0.2Te0.8 passivation layer in conjunction with graded bandgap absorber layers. Initially, we examined a device with a configuration of V2O5/CdTe/ZnSe in absence of passivation layer. This device resulted in a larger Shockley-Read-Hall (SRH) recombination voltage loss of 281 mV and a total voltage loss of 716 mV. We modified this device configuration by utilizing an ultrathin layer (1 nm) of CdSe0.2Te0.8, i.e., V2O5/CdTe/CdSe0.2Te0.8/ZnSe. An ultrathin layer of CdSe0.2Te0.8 works as an effective passivation layer, substantially reducing the SRH recombination voltage loss to 46 mV from 281 mV. Interestingly, when a thicker layer of CdSe0.2Te0.8 is utilized, it not only acts as a passivation layer but also functions as an absorber layer, creating a bandgap gradient. However, improving the grain boundary between CdSe0.2Te0.8 and ZnSe is necessary to further cuts down to SRH recombination voltage loss below 46 mV. To overcome this issue, a thin window layer of CdS0.102Se0.336Te0.562 has been incorporated in between CdSe0.2Te0.8 and ZnSe, close to the front contact, which reduces the SRH recombination voltage loss to 20 mV. This SRH recombination voltage loss can be further minimized to zero from 20 mV when the back interface has been optimized. All simulation data have been justified by previous reported experimental finding to validate the proposed simulation models. Additionally, two-terminal and four-terminal perovskite/CdTe tandem configurations have also been proposed and simulated, yielding power conversion efficiency of 28.64 % and 29.80 %, respectively. These findings demonstrate the efficacy of passivation layer, double absorber layer, bandgap grading, window layer, and interface engineering in mitigating SRH recombination voltage loss, offering a roadmap for future perovskite/CdTe tandem solar cells.
期刊介绍:
The Journal of Physics and Chemistry of Solids is a well-established international medium for publication of archival research in condensed matter and materials sciences. Areas of interest broadly include experimental and theoretical research on electronic, magnetic, spectroscopic and structural properties as well as the statistical mechanics and thermodynamics of materials. The focus is on gaining physical and chemical insight into the properties and potential applications of condensed matter systems.
Within the broad scope of the journal, beyond regular contributions, the editors have identified submissions in the following areas of physics and chemistry of solids to be of special current interest to the journal:
Low-dimensional systems
Exotic states of quantum electron matter including topological phases
Energy conversion and storage
Interfaces, nanoparticles and catalysts.