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Revealing the role of the Rh valence state, La doping level and Ru cocatalyst in determining the H2 evolution efficiency in doped SrTiO3 photocatalysts
SrTiO3 (STO) has favorable opto-electronic properties for overall water splitting. Nevertheless, realizing a higher efficiency is impeded by its band gap which can only harvest UV light. In order to extend the spectral response towards visible light, STO is (co)doped with lanthanum (La) and rhodium...
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Published in: | Sustainable energy & fuels 2019-01, Vol.3 (1), p.208-218 |
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creator | Murthy, Dharmapura H K Matsuzaki, Hiroyuki Wang, Qian Suzuki, Yohichi Seki, Kazuhiko Hisatomi, Takashi Yamada, Taro Kudo, Akihiko Domen, Kazunari Furube, Akihiro |
description | SrTiO3 (STO) has favorable opto-electronic properties for overall water splitting. Nevertheless, realizing a higher efficiency is impeded by its band gap which can only harvest UV light. In order to extend the spectral response towards visible light, STO is (co)doped with lanthanum (La) and rhodium (Rh). However, notwithstanding the amount of visible light absorbed, the H2 evolution rates are remarkably governed by the valence state of Rh, La doping level and ruthenium (Ru) cocatalyst loading. Hence, it is essential to unravel the underlying effect of doping on the photophysical processes to gain insight into material design. To this end, charge carrier dynamics was probed over a wide time (sub-picosecond to microsecond) and spectral (visible to IR) region using transient absorption spectroscopy. Depending on the dopant composition, an interplay between the electron trapping and the kinetics of the electron transfer to the Ru cocatalyst was rationalized. For Rh4+:STO, free electrons probed at 3435 nm decayed virtually completely by 20 ps resulting in a kinetic competition between the electron trapping and the electron transfer to Ru cocatalyst. In the case of Rh3+:STO, free electrons decayed by a factor of three by 100 ps, thus demonstrating the effect of Rh valence state on the electron lifetime. The time constant and quantum yield of electron transfer from Rh3+:STO to the Ru cocatalyst were found to be 1.6 ps and 14.7%, respectively. In addition to a longer electron lifetime, enhanced electron transfer to the Ru cocatalyst makes Rh3+:STO one of the promising photocatalysts for H2 generation. Engineering the energetic position of the dopant within the band gap to avoid undesirable carrier trapping is crucial to enhance the efficiency of photocatalytic reactions. |
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Nevertheless, realizing a higher efficiency is impeded by its band gap which can only harvest UV light. In order to extend the spectral response towards visible light, STO is (co)doped with lanthanum (La) and rhodium (Rh). However, notwithstanding the amount of visible light absorbed, the H2 evolution rates are remarkably governed by the valence state of Rh, La doping level and ruthenium (Ru) cocatalyst loading. Hence, it is essential to unravel the underlying effect of doping on the photophysical processes to gain insight into material design. To this end, charge carrier dynamics was probed over a wide time (sub-picosecond to microsecond) and spectral (visible to IR) region using transient absorption spectroscopy. Depending on the dopant composition, an interplay between the electron trapping and the kinetics of the electron transfer to the Ru cocatalyst was rationalized. For Rh4+:STO, free electrons probed at 3435 nm decayed virtually completely by 20 ps resulting in a kinetic competition between the electron trapping and the electron transfer to Ru cocatalyst. In the case of Rh3+:STO, free electrons decayed by a factor of three by 100 ps, thus demonstrating the effect of Rh valence state on the electron lifetime. The time constant and quantum yield of electron transfer from Rh3+:STO to the Ru cocatalyst were found to be 1.6 ps and 14.7%, respectively. In addition to a longer electron lifetime, enhanced electron transfer to the Ru cocatalyst makes Rh3+:STO one of the promising photocatalysts for H2 generation. Engineering the energetic position of the dopant within the band gap to avoid undesirable carrier trapping is crucial to enhance the efficiency of photocatalytic reactions.</description><identifier>EISSN: 2398-4902</identifier><identifier>DOI: 10.1039/c8se00487k</identifier><language>eng ; jpn</language><publisher>London: Royal Society of Chemistry</publisher><subject>Absorption spectroscopy ; Current carriers ; Dopants ; Doping ; Efficiency ; Electron transfer ; Electronic properties ; Electrons ; Energy gap ; Free electrons ; Hydrogen evolution ; Hydrogen production ; Infrared spectroscopy ; Kinetics ; Lanthanum ; Optoelectronics ; Photocatalysis ; Photocatalysts ; Reaction kinetics ; Rhodium ; Ruthenium ; Spectral sensitivity ; Strontium titanates ; Time constant ; Trapping ; Ultraviolet radiation ; Water splitting</subject><ispartof>Sustainable energy & fuels, 2019-01, Vol.3 (1), p.208-218</ispartof><rights>Copyright Royal Society of Chemistry 2019</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Murthy, Dharmapura H K</creatorcontrib><creatorcontrib>Matsuzaki, Hiroyuki</creatorcontrib><creatorcontrib>Wang, Qian</creatorcontrib><creatorcontrib>Suzuki, Yohichi</creatorcontrib><creatorcontrib>Seki, Kazuhiko</creatorcontrib><creatorcontrib>Hisatomi, Takashi</creatorcontrib><creatorcontrib>Yamada, Taro</creatorcontrib><creatorcontrib>Kudo, Akihiko</creatorcontrib><creatorcontrib>Domen, Kazunari</creatorcontrib><creatorcontrib>Furube, Akihiro</creatorcontrib><title>Revealing the role of the Rh valence state, La doping level and Ru cocatalyst in determining the H2 evolution efficiency in doped SrTiO3 photocatalysts</title><title>Sustainable energy & fuels</title><description>SrTiO3 (STO) has favorable opto-electronic properties for overall water splitting. Nevertheless, realizing a higher efficiency is impeded by its band gap which can only harvest UV light. In order to extend the spectral response towards visible light, STO is (co)doped with lanthanum (La) and rhodium (Rh). However, notwithstanding the amount of visible light absorbed, the H2 evolution rates are remarkably governed by the valence state of Rh, La doping level and ruthenium (Ru) cocatalyst loading. Hence, it is essential to unravel the underlying effect of doping on the photophysical processes to gain insight into material design. To this end, charge carrier dynamics was probed over a wide time (sub-picosecond to microsecond) and spectral (visible to IR) region using transient absorption spectroscopy. Depending on the dopant composition, an interplay between the electron trapping and the kinetics of the electron transfer to the Ru cocatalyst was rationalized. For Rh4+:STO, free electrons probed at 3435 nm decayed virtually completely by 20 ps resulting in a kinetic competition between the electron trapping and the electron transfer to Ru cocatalyst. In the case of Rh3+:STO, free electrons decayed by a factor of three by 100 ps, thus demonstrating the effect of Rh valence state on the electron lifetime. The time constant and quantum yield of electron transfer from Rh3+:STO to the Ru cocatalyst were found to be 1.6 ps and 14.7%, respectively. In addition to a longer electron lifetime, enhanced electron transfer to the Ru cocatalyst makes Rh3+:STO one of the promising photocatalysts for H2 generation. Engineering the energetic position of the dopant within the band gap to avoid undesirable carrier trapping is crucial to enhance the efficiency of photocatalytic reactions.</description><subject>Absorption spectroscopy</subject><subject>Current carriers</subject><subject>Dopants</subject><subject>Doping</subject><subject>Efficiency</subject><subject>Electron transfer</subject><subject>Electronic properties</subject><subject>Electrons</subject><subject>Energy gap</subject><subject>Free electrons</subject><subject>Hydrogen evolution</subject><subject>Hydrogen production</subject><subject>Infrared spectroscopy</subject><subject>Kinetics</subject><subject>Lanthanum</subject><subject>Optoelectronics</subject><subject>Photocatalysis</subject><subject>Photocatalysts</subject><subject>Reaction kinetics</subject><subject>Rhodium</subject><subject>Ruthenium</subject><subject>Spectral sensitivity</subject><subject>Strontium titanates</subject><subject>Time constant</subject><subject>Trapping</subject><subject>Ultraviolet radiation</subject><subject>Water splitting</subject><issn>2398-4902</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNo9jc1OwzAQhC0kJKrSC0-wElcCtpMQ-4gqoEiVKpVyrtbxmqaYuMROpT4Jr0soP5eZOcx8w9iF4NeC5_qmVpE4L1T1dsJGMtcqKzSXZ2wS45ZzLoUsZFmN2OeS9oS-aV8hbQi64AmCO-blBvboqa0JYsJEVzBHsGH33fXDygO2FpY91KHGhP4QEzQtWErUvTftH3ImgfbB96kJLZBzTd0MzMOxGnZk4blbNYscdpuQ_kHxnJ069JEmvz5mLw_3q-ksmy8en6Z382wrKp0ytMpxw91t7owoKkXWCo6GaofOoDBWVQZrqUvliDvU2hqL1lTW2cIpKfMxu_zh7rrw0VNM623ou3a4XEtRVrocVOVfwIxrTQ</recordid><startdate>20190101</startdate><enddate>20190101</enddate><creator>Murthy, Dharmapura H K</creator><creator>Matsuzaki, Hiroyuki</creator><creator>Wang, Qian</creator><creator>Suzuki, Yohichi</creator><creator>Seki, Kazuhiko</creator><creator>Hisatomi, Takashi</creator><creator>Yamada, Taro</creator><creator>Kudo, Akihiko</creator><creator>Domen, Kazunari</creator><creator>Furube, Akihiro</creator><general>Royal Society of Chemistry</general><scope>7QO</scope><scope>7SP</scope><scope>7ST</scope><scope>7U6</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>L7M</scope><scope>P64</scope></search><sort><creationdate>20190101</creationdate><title>Revealing the role of the Rh valence state, La doping level and Ru cocatalyst in determining the H2 evolution efficiency in doped SrTiO3 photocatalysts</title><author>Murthy, Dharmapura H K ; Matsuzaki, Hiroyuki ; Wang, Qian ; Suzuki, Yohichi ; Seki, Kazuhiko ; Hisatomi, Takashi ; Yamada, Taro ; Kudo, Akihiko ; Domen, Kazunari ; Furube, Akihiro</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-j179t-ad8f0b0f63fb1478edd10abecfafba1bd87bac2958fe0fa99dbdadb7dfd4f8223</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng ; jpn</language><creationdate>2019</creationdate><topic>Absorption spectroscopy</topic><topic>Current carriers</topic><topic>Dopants</topic><topic>Doping</topic><topic>Efficiency</topic><topic>Electron transfer</topic><topic>Electronic properties</topic><topic>Electrons</topic><topic>Energy gap</topic><topic>Free electrons</topic><topic>Hydrogen evolution</topic><topic>Hydrogen production</topic><topic>Infrared spectroscopy</topic><topic>Kinetics</topic><topic>Lanthanum</topic><topic>Optoelectronics</topic><topic>Photocatalysis</topic><topic>Photocatalysts</topic><topic>Reaction kinetics</topic><topic>Rhodium</topic><topic>Ruthenium</topic><topic>Spectral sensitivity</topic><topic>Strontium titanates</topic><topic>Time constant</topic><topic>Trapping</topic><topic>Ultraviolet radiation</topic><topic>Water splitting</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Murthy, Dharmapura H K</creatorcontrib><creatorcontrib>Matsuzaki, Hiroyuki</creatorcontrib><creatorcontrib>Wang, Qian</creatorcontrib><creatorcontrib>Suzuki, Yohichi</creatorcontrib><creatorcontrib>Seki, Kazuhiko</creatorcontrib><creatorcontrib>Hisatomi, Takashi</creatorcontrib><creatorcontrib>Yamada, Taro</creatorcontrib><creatorcontrib>Kudo, Akihiko</creatorcontrib><creatorcontrib>Domen, Kazunari</creatorcontrib><creatorcontrib>Furube, Akihiro</creatorcontrib><collection>Biotechnology Research Abstracts</collection><collection>Electronics & Communications Abstracts</collection><collection>Environment Abstracts</collection><collection>Sustainability Science Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>Engineering Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Biotechnology and BioEngineering Abstracts</collection><jtitle>Sustainable energy & fuels</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Murthy, Dharmapura H K</au><au>Matsuzaki, Hiroyuki</au><au>Wang, Qian</au><au>Suzuki, Yohichi</au><au>Seki, Kazuhiko</au><au>Hisatomi, Takashi</au><au>Yamada, Taro</au><au>Kudo, Akihiko</au><au>Domen, Kazunari</au><au>Furube, Akihiro</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Revealing the role of the Rh valence state, La doping level and Ru cocatalyst in determining the H2 evolution efficiency in doped SrTiO3 photocatalysts</atitle><jtitle>Sustainable energy & fuels</jtitle><date>2019-01-01</date><risdate>2019</risdate><volume>3</volume><issue>1</issue><spage>208</spage><epage>218</epage><pages>208-218</pages><eissn>2398-4902</eissn><abstract>SrTiO3 (STO) has favorable opto-electronic properties for overall water splitting. Nevertheless, realizing a higher efficiency is impeded by its band gap which can only harvest UV light. In order to extend the spectral response towards visible light, STO is (co)doped with lanthanum (La) and rhodium (Rh). However, notwithstanding the amount of visible light absorbed, the H2 evolution rates are remarkably governed by the valence state of Rh, La doping level and ruthenium (Ru) cocatalyst loading. Hence, it is essential to unravel the underlying effect of doping on the photophysical processes to gain insight into material design. To this end, charge carrier dynamics was probed over a wide time (sub-picosecond to microsecond) and spectral (visible to IR) region using transient absorption spectroscopy. Depending on the dopant composition, an interplay between the electron trapping and the kinetics of the electron transfer to the Ru cocatalyst was rationalized. For Rh4+:STO, free electrons probed at 3435 nm decayed virtually completely by 20 ps resulting in a kinetic competition between the electron trapping and the electron transfer to Ru cocatalyst. In the case of Rh3+:STO, free electrons decayed by a factor of three by 100 ps, thus demonstrating the effect of Rh valence state on the electron lifetime. The time constant and quantum yield of electron transfer from Rh3+:STO to the Ru cocatalyst were found to be 1.6 ps and 14.7%, respectively. In addition to a longer electron lifetime, enhanced electron transfer to the Ru cocatalyst makes Rh3+:STO one of the promising photocatalysts for H2 generation. Engineering the energetic position of the dopant within the band gap to avoid undesirable carrier trapping is crucial to enhance the efficiency of photocatalytic reactions.</abstract><cop>London</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/c8se00487k</doi><tpages>11</tpages></addata></record> |
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subjects | Absorption spectroscopy Current carriers Dopants Doping Efficiency Electron transfer Electronic properties Electrons Energy gap Free electrons Hydrogen evolution Hydrogen production Infrared spectroscopy Kinetics Lanthanum Optoelectronics Photocatalysis Photocatalysts Reaction kinetics Rhodium Ruthenium Spectral sensitivity Strontium titanates Time constant Trapping Ultraviolet radiation Water splitting |
title | Revealing the role of the Rh valence state, La doping level and Ru cocatalyst in determining the H2 evolution efficiency in doped SrTiO3 photocatalysts |
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