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The physical and photo electrochemical characterization of the crednerite CuMnO sub(2)
CuMnO sub(2) is prepared via Cu super(+) 1 Li super(+) exchange in molten copper (I) chloride. It crystallizes in a monoclinic structure (SG C2/m) where the MnO sub(6) octahedra elongation is ascribed to the Yahn-Teller (Y-T) effect of Mn super(3+) ions. From chemical analysis, the oxide is more acc...
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Published in: | Journal of materials science 2007-08, Vol.42 (15), p.6469-6476 |
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description | CuMnO sub(2) is prepared via Cu super(+) 1 Li super(+) exchange in molten copper (I) chloride. It crystallizes in a monoclinic structure (SG C2/m) where the MnO sub(6) octahedra elongation is ascribed to the Yahn-Teller (Y-T) effect of Mn super(3+) ions. From chemical analysis, the oxide is more accurately formulated as CuMnO sub(2.01). Above 250 C, it undergoes a reversible transition to spinel Cu sub(x)Mn sub(3-x)O sub(4) and beyond 940 C it converts back to Cu sub(1.1)Mn sub(0.9)O sub(2). Extrapolation of high-temperature magnetic data indicates T-intercept [thetas] sub(p) of -450 K and an effective moment of 5.22 k sub(B), consistent with strong antiferromagnetism in the basal plans and high spin (HS) configuration Mn super(3+). This value is slightly larger than that of the spin only moment, a behavior ascribed to Cu super(2+) originating from oxygen insertion. As prepared, CuMnO sub(2) displays p-type conductivity with an activation energy of 0.16 eV. Most holes generated upon band gap excitation are trapped on Cu super(+) ions and the conduction occurs by small polarons hopping between neighboring sites. The linear increase of thermopower for Cu sub(1.05)Mn sub(0.95)O sub(2) with temperature indicates a hole mobility k sub(300 K) (3.5 x 10 super(-6) cm super(2) V super(-1 )s super(-1)) thermally activated. CuMnO sub(2) is made p- and n-type and the difference in the carriers mobilities is attributed to different oxygen polyhedra. The title oxide, characterized photo electrochemically, exhibits a pH-insensitive flat band potential (+0.13 V sub(SCE)). The valence band, located at 5.3 eV below vacuum, is made up of Cu 3d orbital. As application, the powder showed a good performance for the H sub(2)-photo evolution. |
doi_str_mv | 10.1007/s10853-006-1250-x |
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It crystallizes in a monoclinic structure (SG C2/m) where the MnO sub(6) octahedra elongation is ascribed to the Yahn-Teller (Y-T) effect of Mn super(3+) ions. From chemical analysis, the oxide is more accurately formulated as CuMnO sub(2.01). Above 250 C, it undergoes a reversible transition to spinel Cu sub(x)Mn sub(3-x)O sub(4) and beyond 940 C it converts back to Cu sub(1.1)Mn sub(0.9)O sub(2). Extrapolation of high-temperature magnetic data indicates T-intercept [thetas] sub(p) of -450 K and an effective moment of 5.22 k sub(B), consistent with strong antiferromagnetism in the basal plans and high spin (HS) configuration Mn super(3+). This value is slightly larger than that of the spin only moment, a behavior ascribed to Cu super(2+) originating from oxygen insertion. As prepared, CuMnO sub(2) displays p-type conductivity with an activation energy of 0.16 eV. Most holes generated upon band gap excitation are trapped on Cu super(+) ions and the conduction occurs by small polarons hopping between neighboring sites. The linear increase of thermopower for Cu sub(1.05)Mn sub(0.95)O sub(2) with temperature indicates a hole mobility k sub(300 K) (3.5 x 10 super(-6) cm super(2) V super(-1 )s super(-1)) thermally activated. CuMnO sub(2) is made p- and n-type and the difference in the carriers mobilities is attributed to different oxygen polyhedra. The title oxide, characterized photo electrochemically, exhibits a pH-insensitive flat band potential (+0.13 V sub(SCE)). The valence band, located at 5.3 eV below vacuum, is made up of Cu 3d orbital. As application, the powder showed a good performance for the H sub(2)-photo evolution.</description><identifier>ISSN: 0022-2461</identifier><identifier>DOI: 10.1007/s10853-006-1250-x</identifier><language>eng</language><subject>Chlorides ; Copper ; Insertion ; Materials science ; Orbitals ; Oxides ; Polyhedrons ; Yttrium</subject><ispartof>Journal of materials science, 2007-08, Vol.42 (15), p.6469-6476</ispartof><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>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Bessekhouad, Yassine</creatorcontrib><creatorcontrib>Gabes, Yamina</creatorcontrib><creatorcontrib>Bouguelia, Aissa</creatorcontrib><creatorcontrib>Trari, Mohamed</creatorcontrib><title>The physical and photo electrochemical characterization of the crednerite CuMnO sub(2)</title><title>Journal of materials science</title><description>CuMnO sub(2) is prepared via Cu super(+) 1 Li super(+) exchange in molten copper (I) chloride. It crystallizes in a monoclinic structure (SG C2/m) where the MnO sub(6) octahedra elongation is ascribed to the Yahn-Teller (Y-T) effect of Mn super(3+) ions. From chemical analysis, the oxide is more accurately formulated as CuMnO sub(2.01). Above 250 C, it undergoes a reversible transition to spinel Cu sub(x)Mn sub(3-x)O sub(4) and beyond 940 C it converts back to Cu sub(1.1)Mn sub(0.9)O sub(2). Extrapolation of high-temperature magnetic data indicates T-intercept [thetas] sub(p) of -450 K and an effective moment of 5.22 k sub(B), consistent with strong antiferromagnetism in the basal plans and high spin (HS) configuration Mn super(3+). This value is slightly larger than that of the spin only moment, a behavior ascribed to Cu super(2+) originating from oxygen insertion. As prepared, CuMnO sub(2) displays p-type conductivity with an activation energy of 0.16 eV. Most holes generated upon band gap excitation are trapped on Cu super(+) ions and the conduction occurs by small polarons hopping between neighboring sites. The linear increase of thermopower for Cu sub(1.05)Mn sub(0.95)O sub(2) with temperature indicates a hole mobility k sub(300 K) (3.5 x 10 super(-6) cm super(2) V super(-1 )s super(-1)) thermally activated. CuMnO sub(2) is made p- and n-type and the difference in the carriers mobilities is attributed to different oxygen polyhedra. The title oxide, characterized photo electrochemically, exhibits a pH-insensitive flat band potential (+0.13 V sub(SCE)). The valence band, located at 5.3 eV below vacuum, is made up of Cu 3d orbital. As application, the powder showed a good performance for the H sub(2)-photo evolution.</description><subject>Chlorides</subject><subject>Copper</subject><subject>Insertion</subject><subject>Materials science</subject><subject>Orbitals</subject><subject>Oxides</subject><subject>Polyhedrons</subject><subject>Yttrium</subject><issn>0022-2461</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><recordid>eNqVTjsKAjEUTKHg9wB2KbWIvmRdP7UoNmIjthLjk13JJpqXBfX0BvECwsAwPxjGBhLGEmA-IQmLPBMAMyFVDuLZYG0ApYSazmSLdYhuAJDPlWyz46FAfi9eVBptuXaXJHz0HC2aGLwpsPomptBBm4ihfOtYesf9lcc0NQEvLrkR-areuT2n-jxUox5rXrUl7P-4y4ab9WG1FffgHzVSPFUlGbRWO_Q1ndJjJZd5QvZH9QMdVUm_</recordid><startdate>20070801</startdate><enddate>20070801</enddate><creator>Bessekhouad, Yassine</creator><creator>Gabes, Yamina</creator><creator>Bouguelia, Aissa</creator><creator>Trari, Mohamed</creator><scope>7SR</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20070801</creationdate><title>The physical and photo electrochemical characterization of the crednerite CuMnO sub(2)</title><author>Bessekhouad, Yassine ; Gabes, Yamina ; Bouguelia, Aissa ; Trari, Mohamed</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_10821951953</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2007</creationdate><topic>Chlorides</topic><topic>Copper</topic><topic>Insertion</topic><topic>Materials science</topic><topic>Orbitals</topic><topic>Oxides</topic><topic>Polyhedrons</topic><topic>Yttrium</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bessekhouad, Yassine</creatorcontrib><creatorcontrib>Gabes, Yamina</creatorcontrib><creatorcontrib>Bouguelia, Aissa</creatorcontrib><creatorcontrib>Trari, Mohamed</creatorcontrib><collection>Engineered Materials Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of materials science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bessekhouad, Yassine</au><au>Gabes, Yamina</au><au>Bouguelia, Aissa</au><au>Trari, Mohamed</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The physical and photo electrochemical characterization of the crednerite CuMnO sub(2)</atitle><jtitle>Journal of materials science</jtitle><date>2007-08-01</date><risdate>2007</risdate><volume>42</volume><issue>15</issue><spage>6469</spage><epage>6476</epage><pages>6469-6476</pages><issn>0022-2461</issn><abstract>CuMnO sub(2) is prepared via Cu super(+) 1 Li super(+) exchange in molten copper (I) chloride. It crystallizes in a monoclinic structure (SG C2/m) where the MnO sub(6) octahedra elongation is ascribed to the Yahn-Teller (Y-T) effect of Mn super(3+) ions. From chemical analysis, the oxide is more accurately formulated as CuMnO sub(2.01). Above 250 C, it undergoes a reversible transition to spinel Cu sub(x)Mn sub(3-x)O sub(4) and beyond 940 C it converts back to Cu sub(1.1)Mn sub(0.9)O sub(2). Extrapolation of high-temperature magnetic data indicates T-intercept [thetas] sub(p) of -450 K and an effective moment of 5.22 k sub(B), consistent with strong antiferromagnetism in the basal plans and high spin (HS) configuration Mn super(3+). This value is slightly larger than that of the spin only moment, a behavior ascribed to Cu super(2+) originating from oxygen insertion. As prepared, CuMnO sub(2) displays p-type conductivity with an activation energy of 0.16 eV. Most holes generated upon band gap excitation are trapped on Cu super(+) ions and the conduction occurs by small polarons hopping between neighboring sites. The linear increase of thermopower for Cu sub(1.05)Mn sub(0.95)O sub(2) with temperature indicates a hole mobility k sub(300 K) (3.5 x 10 super(-6) cm super(2) V super(-1 )s super(-1)) thermally activated. CuMnO sub(2) is made p- and n-type and the difference in the carriers mobilities is attributed to different oxygen polyhedra. The title oxide, characterized photo electrochemically, exhibits a pH-insensitive flat band potential (+0.13 V sub(SCE)). The valence band, located at 5.3 eV below vacuum, is made up of Cu 3d orbital. As application, the powder showed a good performance for the H sub(2)-photo evolution.</abstract><doi>10.1007/s10853-006-1250-x</doi></addata></record> |
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subjects | Chlorides Copper Insertion Materials science Orbitals Oxides Polyhedrons Yttrium |
title | The physical and photo electrochemical characterization of the crednerite CuMnO sub(2) |
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