Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode

Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent d...
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Autor*in:	Xu, Yunlan [verfasserIn] Yao, Haoyang Zhong, Dengjie Mou, Jiaxin Li, Jun

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2023

Schlagwörter:	PDA/WO /TiO /Ti photoanode Photocatalytic fuel cell Visible light response Electricity generation Rhodamine B

Anmerkung:	© The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.

Übergeordnetes Werk:	Enthalten in: Ionics - Berlin : Springer, 1995, 29(2023), 3 vom: 28. Jan., Seite 1053-1068
Übergeordnetes Werk:	volume:29 ; year:2023 ; number:3 ; day:28 ; month:01 ; pages:1053-1068

Links:	Volltext

DOI / URN:	10.1007/s11581-023-04887-2

Katalog-ID:	SPR049492470

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245	1	0	\|a Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode
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520			\|a Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. The maximum power density, photocurrent density, and Rhodamine B degradation rate of the photocatalytic fuel cell (PFC) with PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti photoanode were 18.68 μW·$ cm^{−2} $, 0.18 mA·$ cm^{−2} $, and 84.6%, respectively. Its excellent performance is mainly due to the good carrier mobility of PDA and the stepped heterojunction structure formed by PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti so that photogenerated electrons and holes gather in the conduction bands of $ WO_{3} $ and HOMO of PDA, respectively. This not only expands the light absorption range and improves the light absorption intensity but also promotes the separation of electron–hole pairs and finally significantly enhances the Rhodamine B degradation and power generation performance of PFC.
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allfields	10.1007/s11581-023-04887-2 doi (DE-627)SPR049492470 (SPR)s11581-023-04887-2-e DE-627 ger DE-627 rakwb eng Xu, Yunlan verfasserin aut Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. The maximum power density, photocurrent density, and Rhodamine B degradation rate of the photocatalytic fuel cell (PFC) with PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti photoanode were 18.68 μW·$ cm^{−2} $, 0.18 mA·$ cm^{−2} $, and 84.6%, respectively. Its excellent performance is mainly due to the good carrier mobility of PDA and the stepped heterojunction structure formed by PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti so that photogenerated electrons and holes gather in the conduction bands of $ WO_{3} $ and HOMO of PDA, respectively. This not only expands the light absorption range and improves the light absorption intensity but also promotes the separation of electron–hole pairs and finally significantly enhances the Rhodamine B degradation and power generation performance of PFC. PDA/WO (dpeaa)DE-He213 /TiO (dpeaa)DE-He213 /Ti photoanode (dpeaa)DE-He213 Photocatalytic fuel cell (dpeaa)DE-He213 Visible light response (dpeaa)DE-He213 Electricity generation (dpeaa)DE-He213 Rhodamine B (dpeaa)DE-He213 Yao, Haoyang aut Zhong, Dengjie aut Mou, Jiaxin aut Li, Jun aut Enthalten in Ionics Berlin : Springer, 1995 29(2023), 3 vom: 28. Jan., Seite 1053-1068 (DE-627)509398944 (DE-600)2226746-3 1862-0760 nnns volume:29 year:2023 number:3 day:28 month:01 pages:1053-1068 https://dx.doi.org/10.1007/s11581-023-04887-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 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_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2023 3 28 01 1053-1068
spelling	10.1007/s11581-023-04887-2 doi (DE-627)SPR049492470 (SPR)s11581-023-04887-2-e DE-627 ger DE-627 rakwb eng Xu, Yunlan verfasserin aut Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. The maximum power density, photocurrent density, and Rhodamine B degradation rate of the photocatalytic fuel cell (PFC) with PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti photoanode were 18.68 μW·$ cm^{−2} $, 0.18 mA·$ cm^{−2} $, and 84.6%, respectively. Its excellent performance is mainly due to the good carrier mobility of PDA and the stepped heterojunction structure formed by PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti so that photogenerated electrons and holes gather in the conduction bands of $ WO_{3} $ and HOMO of PDA, respectively. This not only expands the light absorption range and improves the light absorption intensity but also promotes the separation of electron–hole pairs and finally significantly enhances the Rhodamine B degradation and power generation performance of PFC. PDA/WO (dpeaa)DE-He213 /TiO (dpeaa)DE-He213 /Ti photoanode (dpeaa)DE-He213 Photocatalytic fuel cell (dpeaa)DE-He213 Visible light response (dpeaa)DE-He213 Electricity generation (dpeaa)DE-He213 Rhodamine B (dpeaa)DE-He213 Yao, Haoyang aut Zhong, Dengjie aut Mou, Jiaxin aut Li, Jun aut Enthalten in Ionics Berlin : Springer, 1995 29(2023), 3 vom: 28. Jan., Seite 1053-1068 (DE-627)509398944 (DE-600)2226746-3 1862-0760 nnns volume:29 year:2023 number:3 day:28 month:01 pages:1053-1068 https://dx.doi.org/10.1007/s11581-023-04887-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 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_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2023 3 28 01 1053-1068
allfields_unstemmed	10.1007/s11581-023-04887-2 doi (DE-627)SPR049492470 (SPR)s11581-023-04887-2-e DE-627 ger DE-627 rakwb eng Xu, Yunlan verfasserin aut Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. The maximum power density, photocurrent density, and Rhodamine B degradation rate of the photocatalytic fuel cell (PFC) with PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti photoanode were 18.68 μW·$ cm^{−2} $, 0.18 mA·$ cm^{−2} $, and 84.6%, respectively. Its excellent performance is mainly due to the good carrier mobility of PDA and the stepped heterojunction structure formed by PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti so that photogenerated electrons and holes gather in the conduction bands of $ WO_{3} $ and HOMO of PDA, respectively. This not only expands the light absorption range and improves the light absorption intensity but also promotes the separation of electron–hole pairs and finally significantly enhances the Rhodamine B degradation and power generation performance of PFC. PDA/WO (dpeaa)DE-He213 /TiO (dpeaa)DE-He213 /Ti photoanode (dpeaa)DE-He213 Photocatalytic fuel cell (dpeaa)DE-He213 Visible light response (dpeaa)DE-He213 Electricity generation (dpeaa)DE-He213 Rhodamine B (dpeaa)DE-He213 Yao, Haoyang aut Zhong, Dengjie aut Mou, Jiaxin aut Li, Jun aut Enthalten in Ionics Berlin : Springer, 1995 29(2023), 3 vom: 28. Jan., Seite 1053-1068 (DE-627)509398944 (DE-600)2226746-3 1862-0760 nnns volume:29 year:2023 number:3 day:28 month:01 pages:1053-1068 https://dx.doi.org/10.1007/s11581-023-04887-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 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_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2023 3 28 01 1053-1068
allfieldsGer	10.1007/s11581-023-04887-2 doi (DE-627)SPR049492470 (SPR)s11581-023-04887-2-e DE-627 ger DE-627 rakwb eng Xu, Yunlan verfasserin aut Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. The maximum power density, photocurrent density, and Rhodamine B degradation rate of the photocatalytic fuel cell (PFC) with PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti photoanode were 18.68 μW·$ cm^{−2} $, 0.18 mA·$ cm^{−2} $, and 84.6%, respectively. Its excellent performance is mainly due to the good carrier mobility of PDA and the stepped heterojunction structure formed by PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti so that photogenerated electrons and holes gather in the conduction bands of $ WO_{3} $ and HOMO of PDA, respectively. This not only expands the light absorption range and improves the light absorption intensity but also promotes the separation of electron–hole pairs and finally significantly enhances the Rhodamine B degradation and power generation performance of PFC. PDA/WO (dpeaa)DE-He213 /TiO (dpeaa)DE-He213 /Ti photoanode (dpeaa)DE-He213 Photocatalytic fuel cell (dpeaa)DE-He213 Visible light response (dpeaa)DE-He213 Electricity generation (dpeaa)DE-He213 Rhodamine B (dpeaa)DE-He213 Yao, Haoyang aut Zhong, Dengjie aut Mou, Jiaxin aut Li, Jun aut Enthalten in Ionics Berlin : Springer, 1995 29(2023), 3 vom: 28. Jan., Seite 1053-1068 (DE-627)509398944 (DE-600)2226746-3 1862-0760 nnns volume:29 year:2023 number:3 day:28 month:01 pages:1053-1068 https://dx.doi.org/10.1007/s11581-023-04887-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 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_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2023 3 28 01 1053-1068
allfieldsSound	10.1007/s11581-023-04887-2 doi (DE-627)SPR049492470 (SPR)s11581-023-04887-2-e DE-627 ger DE-627 rakwb eng Xu, Yunlan verfasserin aut Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. The maximum power density, photocurrent density, and Rhodamine B degradation rate of the photocatalytic fuel cell (PFC) with PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti photoanode were 18.68 μW·$ cm^{−2} $, 0.18 mA·$ cm^{−2} $, and 84.6%, respectively. Its excellent performance is mainly due to the good carrier mobility of PDA and the stepped heterojunction structure formed by PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti so that photogenerated electrons and holes gather in the conduction bands of $ WO_{3} $ and HOMO of PDA, respectively. This not only expands the light absorption range and improves the light absorption intensity but also promotes the separation of electron–hole pairs and finally significantly enhances the Rhodamine B degradation and power generation performance of PFC. PDA/WO (dpeaa)DE-He213 /TiO (dpeaa)DE-He213 /Ti photoanode (dpeaa)DE-He213 Photocatalytic fuel cell (dpeaa)DE-He213 Visible light response (dpeaa)DE-He213 Electricity generation (dpeaa)DE-He213 Rhodamine B (dpeaa)DE-He213 Yao, Haoyang aut Zhong, Dengjie aut Mou, Jiaxin aut Li, Jun aut Enthalten in Ionics Berlin : Springer, 1995 29(2023), 3 vom: 28. Jan., Seite 1053-1068 (DE-627)509398944 (DE-600)2226746-3 1862-0760 nnns volume:29 year:2023 number:3 day:28 month:01 pages:1053-1068 https://dx.doi.org/10.1007/s11581-023-04887-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 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_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2023 3 28 01 1053-1068
language	English
source	Enthalten in Ionics 29(2023), 3 vom: 28. Jan., Seite 1053-1068 volume:29 year:2023 number:3 day:28 month:01 pages:1053-1068
sourceStr	Enthalten in Ionics 29(2023), 3 vom: 28. Jan., Seite 1053-1068 volume:29 year:2023 number:3 day:28 month:01 pages:1053-1068
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	PDA/WO /TiO /Ti photoanode Photocatalytic fuel cell Visible light response Electricity generation Rhodamine B
isfreeaccess_bool	false
container_title	Ionics
authorswithroles_txt_mv	Xu, Yunlan @@aut@@ Yao, Haoyang @@aut@@ Zhong, Dengjie @@aut@@ Mou, Jiaxin @@aut@@ Li, Jun @@aut@@
publishDateDaySort_date	2023-01-28T00:00:00Z
hierarchy_top_id	509398944
id	SPR049492470
language_de	englisch
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Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. 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author	Xu, Yunlan
spellingShingle	Xu, Yunlan misc PDA/WO misc /TiO misc /Ti photoanode misc Photocatalytic fuel cell misc Visible light response misc Electricity generation misc Rhodamine B Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode
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topic_title	Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode PDA/WO (dpeaa)DE-He213 /TiO (dpeaa)DE-He213 /Ti photoanode (dpeaa)DE-He213 Photocatalytic fuel cell (dpeaa)DE-He213 Visible light response (dpeaa)DE-He213 Electricity generation (dpeaa)DE-He213 Rhodamine B (dpeaa)DE-He213
topic	misc PDA/WO misc /TiO misc /Ti photoanode misc Photocatalytic fuel cell misc Visible light response misc Electricity generation misc Rhodamine B
topic_unstemmed	misc PDA/WO misc /TiO misc /Ti photoanode misc Photocatalytic fuel cell misc Visible light response misc Electricity generation misc Rhodamine B
topic_browse	misc PDA/WO misc /TiO misc /Ti photoanode misc Photocatalytic fuel cell misc Visible light response misc Electricity generation misc Rhodamine B
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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title	Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode
ctrlnum	(DE-627)SPR049492470 (SPR)s11581-023-04887-2-e
title_full	Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode
author_sort	Xu, Yunlan
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author_browse	Xu, Yunlan Yao, Haoyang Zhong, Dengjie Mou, Jiaxin Li, Jun
container_volume	29
format_se	Elektronische Aufsätze
author-letter	Xu, Yunlan
doi_str_mv	10.1007/s11581-023-04887-2
title_sort	efficient rhodamine b degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ wo_{3} $/$ tio_{2} $/ti photoanode
title_auth	Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode
abstract	Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. The maximum power density, photocurrent density, and Rhodamine B degradation rate of the photocatalytic fuel cell (PFC) with PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti photoanode were 18.68 μW·$ cm^{−2} $, 0.18 mA·$ cm^{−2} $, and 84.6%, respectively. Its excellent performance is mainly due to the good carrier mobility of PDA and the stepped heterojunction structure formed by PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti so that photogenerated electrons and holes gather in the conduction bands of $ WO_{3} $ and HOMO of PDA, respectively. This not only expands the light absorption range and improves the light absorption intensity but also promotes the separation of electron–hole pairs and finally significantly enhances the Rhodamine B degradation and power generation performance of PFC. © The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.
abstractGer	Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. The maximum power density, photocurrent density, and Rhodamine B degradation rate of the photocatalytic fuel cell (PFC) with PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti photoanode were 18.68 μW·$ cm^{−2} $, 0.18 mA·$ cm^{−2} $, and 84.6%, respectively. Its excellent performance is mainly due to the good carrier mobility of PDA and the stepped heterojunction structure formed by PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti so that photogenerated electrons and holes gather in the conduction bands of $ WO_{3} $ and HOMO of PDA, respectively. This not only expands the light absorption range and improves the light absorption intensity but also promotes the separation of electron–hole pairs and finally significantly enhances the Rhodamine B degradation and power generation performance of PFC. © The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.
abstract_unstemmed	Abstract In order to solve the rapid recombination of electron–hole pairs, limited optical response range, and single electron and hole transmission path, polydopamine (PDA)/$ WO_{3} $ and $ TiO_{2} $ composite (PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti) photoanode was prepared. Its maximum photocurrent density is 2.03 mA·$ cm^{−2} $ at 1.1 V (vs. SCE), which is 1.47 times higher than that of $ WO_{3} $/$ TiO_{2} $/Ti. The maximum power density, photocurrent density, and Rhodamine B degradation rate of the photocatalytic fuel cell (PFC) with PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti photoanode were 18.68 μW·$ cm^{−2} $, 0.18 mA·$ cm^{−2} $, and 84.6%, respectively. Its excellent performance is mainly due to the good carrier mobility of PDA and the stepped heterojunction structure formed by PDA-11.5%/$ WO_{3} $/$ TiO_{2} $/Ti so that photogenerated electrons and holes gather in the conduction bands of $ WO_{3} $ and HOMO of PDA, respectively. This not only expands the light absorption range and improves the light absorption intensity but also promotes the separation of electron–hole pairs and finally significantly enhances the Rhodamine B degradation and power generation performance of PFC. © The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.
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container_issue	3
title_short	Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode
url	https://dx.doi.org/10.1007/s11581-023-04887-2
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author2	Yao, Haoyang Zhong, Dengjie Mou, Jiaxin Li, Jun
author2Str	Yao, Haoyang Zhong, Dengjie Mou, Jiaxin Li, Jun
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doi_str	10.1007/s11581-023-04887-2
up_date	2024-07-04T01:02:23.947Z
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Efficient Rhodamine B degradation and electricity generation by a photocatalytic fuel cell with visible light response polydopamine/$ WO_{3} $/$ TiO_{2} $/Ti photoanode

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