Visible-Light-Induced Reversible Photomagnetism in Rubidium Manganese Hexacyanoferrate
The photoreversibility of a photoinduced phase transition was investigated in a rubidium manganese hexacyanoferrate, Rb0.88Mn[Fe(CN)6]0.96·0.5H2O. The present material shows a charge-transfer phase transition from the MnII−FeIII [high-temperature (HT)] phase to the MnIII−FeII [low-temperature (LT)]...
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Veröffentlicht in: | Chemistry of materials 2008-01, Vol.20 (2), p.423-428 |
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creator | Tokoro, Hiroko Matsuda, Tomoyuki Nuida, Tomohiro Moritomo, Yutaka Ohoyama, Kenji Dangui, Edgard Davy Loutete Boukheddaden, Kamel Ohkoshi, Shin-ichi |
description | The photoreversibility of a photoinduced phase transition was investigated in a rubidium manganese hexacyanoferrate, Rb0.88Mn[Fe(CN)6]0.96·0.5H2O. The present material shows a charge-transfer phase transition from the MnII−FeIII [high-temperature (HT)] phase to the MnIII−FeII [low-temperature (LT)] phase, and the LT phase shows ferromagnetism. Spectroscopic ellipsometry measurements of the dielectric constant suggest that the optical transitions in the LT and HT phases are a metal-to-metal charge transfer (FeII → MnIII) band at 420–540 nm and a ligand-to-metal charge transfer (CN– → FeIII) band of [FeIII(CN)6] at 410 nm, respectively. By irradiation with 532 nm light, the LT phase is transmitted to the photoinduced (PI) phase, which has a valence state similar to that of the HT phase, and photodemagnetization is observed. In contrast, irradiating the PI phase with 410 ± 30 nm light causes the reverse phase transition. Neutron powder diffraction measurement of an analogue compound, Rb0.58Mn[Fe(CN)6]0.86·2.3H2O, which does not show a charge-transfer phase transition and maintains the MnII−FeIII phase at a very low temperature, confirms that the PI phase is an antiferromagnet. Hence, the present visible-light-induced reversible photomagnetic effect is due to optical switching between the ferromagnetic LT phase and the antiferromagnetic PI phase. |
doi_str_mv | 10.1021/cm701873s |
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The present material shows a charge-transfer phase transition from the MnII−FeIII [high-temperature (HT)] phase to the MnIII−FeII [low-temperature (LT)] phase, and the LT phase shows ferromagnetism. Spectroscopic ellipsometry measurements of the dielectric constant suggest that the optical transitions in the LT and HT phases are a metal-to-metal charge transfer (FeII → MnIII) band at 420–540 nm and a ligand-to-metal charge transfer (CN– → FeIII) band of [FeIII(CN)6] at 410 nm, respectively. By irradiation with 532 nm light, the LT phase is transmitted to the photoinduced (PI) phase, which has a valence state similar to that of the HT phase, and photodemagnetization is observed. In contrast, irradiating the PI phase with 410 ± 30 nm light causes the reverse phase transition. Neutron powder diffraction measurement of an analogue compound, Rb0.58Mn[Fe(CN)6]0.86·2.3H2O, which does not show a charge-transfer phase transition and maintains the MnII−FeIII phase at a very low temperature, confirms that the PI phase is an antiferromagnet. Hence, the present visible-light-induced reversible photomagnetic effect is due to optical switching between the ferromagnetic LT phase and the antiferromagnetic PI phase.</description><identifier>ISSN: 0897-4756</identifier><identifier>EISSN: 1520-5002</identifier><identifier>DOI: 10.1021/cm701873s</identifier><language>eng</language><publisher>American Chemical Society</publisher><subject>Magnetic Materials ; Molecular Crystals ; Optical Materials (including Non-Linear Optic, Photonic, and Optoelectronic Materials)</subject><ispartof>Chemistry of materials, 2008-01, Vol.20 (2), p.423-428</ispartof><rights>Copyright © 2008 American Chemical Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a363t-54142208651f6459939264aa2cbea880a2831b85ce3f0f0e88353e7d12c87ee73</citedby><cites>FETCH-LOGICAL-a363t-54142208651f6459939264aa2cbea880a2831b85ce3f0f0e88353e7d12c87ee73</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://pubs.acs.org/doi/pdf/10.1021/cm701873s$$EPDF$$P50$$Gacs$$H</linktopdf><linktohtml>$$Uhttps://pubs.acs.org/doi/10.1021/cm701873s$$EHTML$$P50$$Gacs$$H</linktohtml><link.rule.ids>314,776,780,2752,27053,27901,27902,56713,56763</link.rule.ids></links><search><creatorcontrib>Tokoro, Hiroko</creatorcontrib><creatorcontrib>Matsuda, Tomoyuki</creatorcontrib><creatorcontrib>Nuida, Tomohiro</creatorcontrib><creatorcontrib>Moritomo, Yutaka</creatorcontrib><creatorcontrib>Ohoyama, Kenji</creatorcontrib><creatorcontrib>Dangui, Edgard Davy Loutete</creatorcontrib><creatorcontrib>Boukheddaden, Kamel</creatorcontrib><creatorcontrib>Ohkoshi, Shin-ichi</creatorcontrib><title>Visible-Light-Induced Reversible Photomagnetism in Rubidium Manganese Hexacyanoferrate</title><title>Chemistry of materials</title><addtitle>Chem. Mater</addtitle><description>The photoreversibility of a photoinduced phase transition was investigated in a rubidium manganese hexacyanoferrate, Rb0.88Mn[Fe(CN)6]0.96·0.5H2O. The present material shows a charge-transfer phase transition from the MnII−FeIII [high-temperature (HT)] phase to the MnIII−FeII [low-temperature (LT)] phase, and the LT phase shows ferromagnetism. Spectroscopic ellipsometry measurements of the dielectric constant suggest that the optical transitions in the LT and HT phases are a metal-to-metal charge transfer (FeII → MnIII) band at 420–540 nm and a ligand-to-metal charge transfer (CN– → FeIII) band of [FeIII(CN)6] at 410 nm, respectively. By irradiation with 532 nm light, the LT phase is transmitted to the photoinduced (PI) phase, which has a valence state similar to that of the HT phase, and photodemagnetization is observed. In contrast, irradiating the PI phase with 410 ± 30 nm light causes the reverse phase transition. Neutron powder diffraction measurement of an analogue compound, Rb0.58Mn[Fe(CN)6]0.86·2.3H2O, which does not show a charge-transfer phase transition and maintains the MnII−FeIII phase at a very low temperature, confirms that the PI phase is an antiferromagnet. Hence, the present visible-light-induced reversible photomagnetic effect is due to optical switching between the ferromagnetic LT phase and the antiferromagnetic PI phase.</description><subject>Magnetic Materials</subject><subject>Molecular Crystals</subject><subject>Optical Materials (including Non-Linear Optic, Photonic, and Optoelectronic Materials)</subject><issn>0897-4756</issn><issn>1520-5002</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNpt0L1OwzAUBWALgUQpDLxBFgYGg3_i2BlRBbQiFVUpXS3HuWldmgTZCWrfnkBRJ6Y73E9HOgeha0ruKGH03laSUCV5OEEDKhjBghB2igZEpRLHUiTn6CKEDSG052qAlksXXL4FnLnVusWTuugsFNEcvsD_PqLZummbyqxqaF2oIldH8y53heuqaGrqlakhQDSGnbF7UzcleG9auERnpdkGuPq7Q_T-9LgYjXH2-jwZPWTY8IS3WMQ0ZoyoRNAyiUWa8pQlsTHM5mCUIoYpTnMlLPCSlASU4oKDLCizSgJIPkS3h1zrmxA8lPrTu8r4vaZE_wyij4P0Fh-sCy3sjtD4D51ILoVezN50MmeLl2w81dPe3xy8sUFvms7XfZN_cr8BUjtuzA</recordid><startdate>20080122</startdate><enddate>20080122</enddate><creator>Tokoro, Hiroko</creator><creator>Matsuda, Tomoyuki</creator><creator>Nuida, Tomohiro</creator><creator>Moritomo, Yutaka</creator><creator>Ohoyama, Kenji</creator><creator>Dangui, Edgard Davy Loutete</creator><creator>Boukheddaden, Kamel</creator><creator>Ohkoshi, Shin-ichi</creator><general>American Chemical Society</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20080122</creationdate><title>Visible-Light-Induced Reversible Photomagnetism in Rubidium Manganese Hexacyanoferrate</title><author>Tokoro, Hiroko ; Matsuda, Tomoyuki ; Nuida, Tomohiro ; Moritomo, Yutaka ; Ohoyama, Kenji ; Dangui, Edgard Davy Loutete ; Boukheddaden, Kamel ; Ohkoshi, Shin-ichi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a363t-54142208651f6459939264aa2cbea880a2831b85ce3f0f0e88353e7d12c87ee73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><topic>Magnetic Materials</topic><topic>Molecular Crystals</topic><topic>Optical Materials (including Non-Linear Optic, Photonic, and Optoelectronic Materials)</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tokoro, Hiroko</creatorcontrib><creatorcontrib>Matsuda, Tomoyuki</creatorcontrib><creatorcontrib>Nuida, Tomohiro</creatorcontrib><creatorcontrib>Moritomo, Yutaka</creatorcontrib><creatorcontrib>Ohoyama, Kenji</creatorcontrib><creatorcontrib>Dangui, Edgard Davy Loutete</creatorcontrib><creatorcontrib>Boukheddaden, Kamel</creatorcontrib><creatorcontrib>Ohkoshi, Shin-ichi</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><jtitle>Chemistry of materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tokoro, Hiroko</au><au>Matsuda, Tomoyuki</au><au>Nuida, Tomohiro</au><au>Moritomo, Yutaka</au><au>Ohoyama, Kenji</au><au>Dangui, Edgard Davy Loutete</au><au>Boukheddaden, Kamel</au><au>Ohkoshi, Shin-ichi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Visible-Light-Induced Reversible Photomagnetism in Rubidium Manganese Hexacyanoferrate</atitle><jtitle>Chemistry of materials</jtitle><addtitle>Chem. Mater</addtitle><date>2008-01-22</date><risdate>2008</risdate><volume>20</volume><issue>2</issue><spage>423</spage><epage>428</epage><pages>423-428</pages><issn>0897-4756</issn><eissn>1520-5002</eissn><abstract>The photoreversibility of a photoinduced phase transition was investigated in a rubidium manganese hexacyanoferrate, Rb0.88Mn[Fe(CN)6]0.96·0.5H2O. The present material shows a charge-transfer phase transition from the MnII−FeIII [high-temperature (HT)] phase to the MnIII−FeII [low-temperature (LT)] phase, and the LT phase shows ferromagnetism. Spectroscopic ellipsometry measurements of the dielectric constant suggest that the optical transitions in the LT and HT phases are a metal-to-metal charge transfer (FeII → MnIII) band at 420–540 nm and a ligand-to-metal charge transfer (CN– → FeIII) band of [FeIII(CN)6] at 410 nm, respectively. By irradiation with 532 nm light, the LT phase is transmitted to the photoinduced (PI) phase, which has a valence state similar to that of the HT phase, and photodemagnetization is observed. In contrast, irradiating the PI phase with 410 ± 30 nm light causes the reverse phase transition. Neutron powder diffraction measurement of an analogue compound, Rb0.58Mn[Fe(CN)6]0.86·2.3H2O, which does not show a charge-transfer phase transition and maintains the MnII−FeIII phase at a very low temperature, confirms that the PI phase is an antiferromagnet. Hence, the present visible-light-induced reversible photomagnetic effect is due to optical switching between the ferromagnetic LT phase and the antiferromagnetic PI phase.</abstract><pub>American Chemical Society</pub><doi>10.1021/cm701873s</doi><tpages>6</tpages></addata></record> |
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title | Visible-Light-Induced Reversible Photomagnetism in Rubidium Manganese Hexacyanoferrate |
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