G. Lucovsky, L. Miotti, D. Zeller, C. Adamo, D. Scholm
{"title":"单质和复杂过渡金属氧化物的x射线吸收研究:差异:(i)化学,和(ii)局部位置对称多价","authors":"G. Lucovsky, L. Miotti, D. Zeller, C. Adamo, D. Scholm","doi":"10.1109/ULIS.2011.5758000","DOIUrl":null,"url":null,"abstract":"Alloy induced multivalency in transition metal oxides increases device functionality. Effects include insulator to metal transitions in the d<sup>0</sup> perovskites (i) GdScO<inf>3</inf>, by substitution of tetravalent Ti trivalent for Sc, and (ii) LaMnO<inf>3</inf> by alloy substitution of trivalent La and divalent Sr for trivalent La. Substituion of Ti<sup>3+</sup> for Sc<sup>3+</sup> on the ScO<inf>2</inf> planes leads to hopping induced multivalencey for both Ti and Sc, but only for Ti compositions above a percolation threshold. The formation of La<inf>1−x</inf>Sr<inf>x</inf>MnO<inf>3</inf> alloys leads to mixed valence of the Mn-atoms: Mn<sup>3+</sup> in the LaMnO<inf>3</inf> fraction, and Mn<sup>4+</sup> in the SrMnO<inf>3</inf> fraction. Spectroscopic detection is based on charge transfer multiplet theory applied to Ti, Sc and Mn L<inf>2,3</inf> spectra were multivalent charge states increase the number of spectral features. Multivalency also occurs suboxide alloys such as TiO<inf>2−x</inf> in a composition range: TiO<inf>2</inf> > TiO<inf>2−x</inf> > TiO<inf>1.5</inf>. These alloys have a mix of Ti<sup>4+</sup> and Ti<sup>3+</sup> local bonding states, but due to hopping transport, the mix includes Ti<sup>2+</sup>. One important aspect of controlled multivalency is that it provides a way of changing and/or controlling the density of O-vacancy defects. Electrons can be injected into the oxide negative ion states ion states from Si, Ge, and other semiconductors, as well as metals with different offset energies [1]. The two terminal devices with asymmetric current-voltage charateristics providing options for memory devices.","PeriodicalId":146779,"journal":{"name":"Ulis 2011 Ultimate Integration on Silicon","volume":"3 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2011-03-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"X-ray absorption studies of elemental and complex transition metal (TM) oxides: Differences between: (i) Chemical, and (ii) Local site symmetry multivalency\",\"authors\":\"G. Lucovsky, L. Miotti, D. Zeller, C. Adamo, D. Scholm\",\"doi\":\"10.1109/ULIS.2011.5758000\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Alloy induced multivalency in transition metal oxides increases device functionality. Effects include insulator to metal transitions in the d<sup>0</sup> perovskites (i) GdScO<inf>3</inf>, by substitution of tetravalent Ti trivalent for Sc, and (ii) LaMnO<inf>3</inf> by alloy substitution of trivalent La and divalent Sr for trivalent La. Substituion of Ti<sup>3+</sup> for Sc<sup>3+</sup> on the ScO<inf>2</inf> planes leads to hopping induced multivalencey for both Ti and Sc, but only for Ti compositions above a percolation threshold. The formation of La<inf>1−x</inf>Sr<inf>x</inf>MnO<inf>3</inf> alloys leads to mixed valence of the Mn-atoms: Mn<sup>3+</sup> in the LaMnO<inf>3</inf> fraction, and Mn<sup>4+</sup> in the SrMnO<inf>3</inf> fraction. Spectroscopic detection is based on charge transfer multiplet theory applied to Ti, Sc and Mn L<inf>2,3</inf> spectra were multivalent charge states increase the number of spectral features. Multivalency also occurs suboxide alloys such as TiO<inf>2−x</inf> in a composition range: TiO<inf>2</inf> > TiO<inf>2−x</inf> > TiO<inf>1.5</inf>. These alloys have a mix of Ti<sup>4+</sup> and Ti<sup>3+</sup> local bonding states, but due to hopping transport, the mix includes Ti<sup>2+</sup>. One important aspect of controlled multivalency is that it provides a way of changing and/or controlling the density of O-vacancy defects. Electrons can be injected into the oxide negative ion states ion states from Si, Ge, and other semiconductors, as well as metals with different offset energies [1]. 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X-ray absorption studies of elemental and complex transition metal (TM) oxides: Differences between: (i) Chemical, and (ii) Local site symmetry multivalency
Alloy induced multivalency in transition metal oxides increases device functionality. Effects include insulator to metal transitions in the d0 perovskites (i) GdScO3, by substitution of tetravalent Ti trivalent for Sc, and (ii) LaMnO3 by alloy substitution of trivalent La and divalent Sr for trivalent La. Substituion of Ti3+ for Sc3+ on the ScO2 planes leads to hopping induced multivalencey for both Ti and Sc, but only for Ti compositions above a percolation threshold. The formation of La1−xSrxMnO3 alloys leads to mixed valence of the Mn-atoms: Mn3+ in the LaMnO3 fraction, and Mn4+ in the SrMnO3 fraction. Spectroscopic detection is based on charge transfer multiplet theory applied to Ti, Sc and Mn L2,3 spectra were multivalent charge states increase the number of spectral features. Multivalency also occurs suboxide alloys such as TiO2−x in a composition range: TiO2 > TiO2−x > TiO1.5. These alloys have a mix of Ti4+ and Ti3+ local bonding states, but due to hopping transport, the mix includes Ti2+. One important aspect of controlled multivalency is that it provides a way of changing and/or controlling the density of O-vacancy defects. Electrons can be injected into the oxide negative ion states ion states from Si, Ge, and other semiconductors, as well as metals with different offset energies [1]. The two terminal devices with asymmetric current-voltage charateristics providing options for memory devices.