A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells
We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the sho...
Ausführliche Beschreibung
Autor*in: |
Zhao, Xinhai [verfasserIn] Tan, Hu Quee [verfasserIn] Birgersson, Erik [verfasserIn] Xue, Hansong [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2023 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: Solar energy - Amsterdam [u.a.] : Elsevier Science, 1957, 262 |
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Übergeordnetes Werk: |
volume:262 |
DOI / URN: |
10.1016/j.solener.2023.111905 |
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Katalog-ID: |
ELV062191071 |
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520 | |a We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the short-circuit current density under six albedo conditions, identifying the best cell architectures and alternative material combinations that yield optimal and close-to-optimal results. In contrast to monofacial devices and low albedos, tandem devices with top subcells that are not semi-transparent are found to provide the highest short-circuit current densities under high albedos, such as albedos for white sand and snow. According to a sensitivity analysis, the short-circuit current densities in the optimized devices are not significantly affected by small perturbations in layer thicknesses. The device performances are also discussed in the context of the best optical structure. A power conversion efficiency of 34.6% and a bifacial equivalent efficiency of over 50% are predicted for the optimized monofacial device and bifacial device under high albedo values, respectively. | ||
650 | 4 | |a Mixed-integer optimization | |
650 | 4 | |a Optics | |
650 | 4 | |a Two-terminal perovskite-on-perovskite tandem solar cell | |
650 | 4 | |a Bifacial solar cell | |
650 | 4 | |a Sensitivity analysis | |
700 | 1 | |a Tan, Hu Quee |e verfasserin |4 aut | |
700 | 1 | |a Birgersson, Erik |e verfasserin |4 aut | |
700 | 1 | |a Xue, Hansong |e verfasserin |0 (orcid)0000-0001-6393-7931 |4 aut | |
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10.1016/j.solener.2023.111905 doi (DE-627)ELV062191071 (ELSEVIER)S0038-092X(23)00538-8 DE-627 ger DE-627 rda eng 530 VZ 52.56 bkl Zhao, Xinhai verfasserin (orcid)0000-0002-9735-1688 aut A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the short-circuit current density under six albedo conditions, identifying the best cell architectures and alternative material combinations that yield optimal and close-to-optimal results. In contrast to monofacial devices and low albedos, tandem devices with top subcells that are not semi-transparent are found to provide the highest short-circuit current densities under high albedos, such as albedos for white sand and snow. According to a sensitivity analysis, the short-circuit current densities in the optimized devices are not significantly affected by small perturbations in layer thicknesses. The device performances are also discussed in the context of the best optical structure. A power conversion efficiency of 34.6% and a bifacial equivalent efficiency of over 50% are predicted for the optimized monofacial device and bifacial device under high albedo values, respectively. Mixed-integer optimization Optics Two-terminal perovskite-on-perovskite tandem solar cell Bifacial solar cell Sensitivity analysis Tan, Hu Quee verfasserin aut Birgersson, Erik verfasserin aut Xue, Hansong verfasserin (orcid)0000-0001-6393-7931 aut Enthalten in Solar energy Amsterdam [u.a.] : Elsevier Science, 1957 262 Online-Ressource (DE-627)320525597 (DE-600)2015126-3 (DE-576)096806648 1471-1257 nnns volume:262 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2116 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 52.56 Regenerative Energieformen alternative Energieformen VZ AR 262 |
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10.1016/j.solener.2023.111905 doi (DE-627)ELV062191071 (ELSEVIER)S0038-092X(23)00538-8 DE-627 ger DE-627 rda eng 530 VZ 52.56 bkl Zhao, Xinhai verfasserin (orcid)0000-0002-9735-1688 aut A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the short-circuit current density under six albedo conditions, identifying the best cell architectures and alternative material combinations that yield optimal and close-to-optimal results. In contrast to monofacial devices and low albedos, tandem devices with top subcells that are not semi-transparent are found to provide the highest short-circuit current densities under high albedos, such as albedos for white sand and snow. According to a sensitivity analysis, the short-circuit current densities in the optimized devices are not significantly affected by small perturbations in layer thicknesses. The device performances are also discussed in the context of the best optical structure. A power conversion efficiency of 34.6% and a bifacial equivalent efficiency of over 50% are predicted for the optimized monofacial device and bifacial device under high albedo values, respectively. Mixed-integer optimization Optics Two-terminal perovskite-on-perovskite tandem solar cell Bifacial solar cell Sensitivity analysis Tan, Hu Quee verfasserin aut Birgersson, Erik verfasserin aut Xue, Hansong verfasserin (orcid)0000-0001-6393-7931 aut Enthalten in Solar energy Amsterdam [u.a.] : Elsevier Science, 1957 262 Online-Ressource (DE-627)320525597 (DE-600)2015126-3 (DE-576)096806648 1471-1257 nnns volume:262 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2116 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 52.56 Regenerative Energieformen alternative Energieformen VZ AR 262 |
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10.1016/j.solener.2023.111905 doi (DE-627)ELV062191071 (ELSEVIER)S0038-092X(23)00538-8 DE-627 ger DE-627 rda eng 530 VZ 52.56 bkl Zhao, Xinhai verfasserin (orcid)0000-0002-9735-1688 aut A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the short-circuit current density under six albedo conditions, identifying the best cell architectures and alternative material combinations that yield optimal and close-to-optimal results. In contrast to monofacial devices and low albedos, tandem devices with top subcells that are not semi-transparent are found to provide the highest short-circuit current densities under high albedos, such as albedos for white sand and snow. According to a sensitivity analysis, the short-circuit current densities in the optimized devices are not significantly affected by small perturbations in layer thicknesses. The device performances are also discussed in the context of the best optical structure. A power conversion efficiency of 34.6% and a bifacial equivalent efficiency of over 50% are predicted for the optimized monofacial device and bifacial device under high albedo values, respectively. Mixed-integer optimization Optics Two-terminal perovskite-on-perovskite tandem solar cell Bifacial solar cell Sensitivity analysis Tan, Hu Quee verfasserin aut Birgersson, Erik verfasserin aut Xue, Hansong verfasserin (orcid)0000-0001-6393-7931 aut Enthalten in Solar energy Amsterdam [u.a.] : Elsevier Science, 1957 262 Online-Ressource (DE-627)320525597 (DE-600)2015126-3 (DE-576)096806648 1471-1257 nnns volume:262 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2116 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 52.56 Regenerative Energieformen alternative Energieformen VZ AR 262 |
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10.1016/j.solener.2023.111905 doi (DE-627)ELV062191071 (ELSEVIER)S0038-092X(23)00538-8 DE-627 ger DE-627 rda eng 530 VZ 52.56 bkl Zhao, Xinhai verfasserin (orcid)0000-0002-9735-1688 aut A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the short-circuit current density under six albedo conditions, identifying the best cell architectures and alternative material combinations that yield optimal and close-to-optimal results. In contrast to monofacial devices and low albedos, tandem devices with top subcells that are not semi-transparent are found to provide the highest short-circuit current densities under high albedos, such as albedos for white sand and snow. According to a sensitivity analysis, the short-circuit current densities in the optimized devices are not significantly affected by small perturbations in layer thicknesses. The device performances are also discussed in the context of the best optical structure. A power conversion efficiency of 34.6% and a bifacial equivalent efficiency of over 50% are predicted for the optimized monofacial device and bifacial device under high albedo values, respectively. Mixed-integer optimization Optics Two-terminal perovskite-on-perovskite tandem solar cell Bifacial solar cell Sensitivity analysis Tan, Hu Quee verfasserin aut Birgersson, Erik verfasserin aut Xue, Hansong verfasserin (orcid)0000-0001-6393-7931 aut Enthalten in Solar energy Amsterdam [u.a.] : Elsevier Science, 1957 262 Online-Ressource (DE-627)320525597 (DE-600)2015126-3 (DE-576)096806648 1471-1257 nnns volume:262 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2116 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 52.56 Regenerative Energieformen alternative Energieformen VZ AR 262 |
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10.1016/j.solener.2023.111905 doi (DE-627)ELV062191071 (ELSEVIER)S0038-092X(23)00538-8 DE-627 ger DE-627 rda eng 530 VZ 52.56 bkl Zhao, Xinhai verfasserin (orcid)0000-0002-9735-1688 aut A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the short-circuit current density under six albedo conditions, identifying the best cell architectures and alternative material combinations that yield optimal and close-to-optimal results. In contrast to monofacial devices and low albedos, tandem devices with top subcells that are not semi-transparent are found to provide the highest short-circuit current densities under high albedos, such as albedos for white sand and snow. According to a sensitivity analysis, the short-circuit current densities in the optimized devices are not significantly affected by small perturbations in layer thicknesses. The device performances are also discussed in the context of the best optical structure. A power conversion efficiency of 34.6% and a bifacial equivalent efficiency of over 50% are predicted for the optimized monofacial device and bifacial device under high albedo values, respectively. Mixed-integer optimization Optics Two-terminal perovskite-on-perovskite tandem solar cell Bifacial solar cell Sensitivity analysis Tan, Hu Quee verfasserin aut Birgersson, Erik verfasserin aut Xue, Hansong verfasserin (orcid)0000-0001-6393-7931 aut Enthalten in Solar energy Amsterdam [u.a.] : Elsevier Science, 1957 262 Online-Ressource (DE-627)320525597 (DE-600)2015126-3 (DE-576)096806648 1471-1257 nnns volume:262 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2116 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 52.56 Regenerative Energieformen alternative Energieformen VZ AR 262 |
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530 VZ 52.56 bkl A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells Mixed-integer optimization Optics Two-terminal perovskite-on-perovskite tandem solar cell Bifacial solar cell Sensitivity analysis |
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ddc 530 bkl 52.56 misc Mixed-integer optimization misc Optics misc Two-terminal perovskite-on-perovskite tandem solar cell misc Bifacial solar cell misc Sensitivity analysis |
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ddc 530 bkl 52.56 misc Mixed-integer optimization misc Optics misc Two-terminal perovskite-on-perovskite tandem solar cell misc Bifacial solar cell misc Sensitivity analysis |
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ddc 530 bkl 52.56 misc Mixed-integer optimization misc Optics misc Two-terminal perovskite-on-perovskite tandem solar cell misc Bifacial solar cell misc Sensitivity analysis |
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A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells |
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A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells |
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Zhao, Xinhai |
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Zhao, Xinhai Tan, Hu Quee Birgersson, Erik Xue, Hansong |
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a mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells |
title_auth |
A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells |
abstract |
We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the short-circuit current density under six albedo conditions, identifying the best cell architectures and alternative material combinations that yield optimal and close-to-optimal results. In contrast to monofacial devices and low albedos, tandem devices with top subcells that are not semi-transparent are found to provide the highest short-circuit current densities under high albedos, such as albedos for white sand and snow. According to a sensitivity analysis, the short-circuit current densities in the optimized devices are not significantly affected by small perturbations in layer thicknesses. The device performances are also discussed in the context of the best optical structure. A power conversion efficiency of 34.6% and a bifacial equivalent efficiency of over 50% are predicted for the optimized monofacial device and bifacial device under high albedo values, respectively. |
abstractGer |
We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the short-circuit current density under six albedo conditions, identifying the best cell architectures and alternative material combinations that yield optimal and close-to-optimal results. In contrast to monofacial devices and low albedos, tandem devices with top subcells that are not semi-transparent are found to provide the highest short-circuit current densities under high albedos, such as albedos for white sand and snow. According to a sensitivity analysis, the short-circuit current densities in the optimized devices are not significantly affected by small perturbations in layer thicknesses. The device performances are also discussed in the context of the best optical structure. A power conversion efficiency of 34.6% and a bifacial equivalent efficiency of over 50% are predicted for the optimized monofacial device and bifacial device under high albedo values, respectively. |
abstract_unstemmed |
We present a mixed-integer optimization for the optics of two-terminal perovskite-on-perovskite tandem solar cells, which accounts for thickness and material variations in all thin-film layers. The model, which is validated with experiments for both monofacial and bifacial devices, optimizes the short-circuit current density under six albedo conditions, identifying the best cell architectures and alternative material combinations that yield optimal and close-to-optimal results. In contrast to monofacial devices and low albedos, tandem devices with top subcells that are not semi-transparent are found to provide the highest short-circuit current densities under high albedos, such as albedos for white sand and snow. According to a sensitivity analysis, the short-circuit current densities in the optimized devices are not significantly affected by small perturbations in layer thicknesses. The device performances are also discussed in the context of the best optical structure. A power conversion efficiency of 34.6% and a bifacial equivalent efficiency of over 50% are predicted for the optimized monofacial device and bifacial device under high albedo values, respectively. |
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title_short |
A mixed-integer optimization for bifacial two-terminal perovskite-on-perovskite tandem solar cells |
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