dc.contributor.author | Santhosh, P N | |
dc.contributor.author | Arulraj, Anthony | |
dc.contributor.author | Vanitha, P V | |
dc.contributor.author | Singh, R S | |
dc.contributor.author | Sooryanarayana, K | |
dc.contributor.author | Rao, C N R | |
dc.date.accessioned | 2012-03-21T09:06:18Z | |
dc.date.available | 2012-03-21T09:06:18Z | |
dc.date.issued | 1999-02-08 | |
dc.identifier | 0953-8984 | en_US |
dc.identifier.citation | Journal Of Physics: Condensed Matter 11(5), L27-L33 (1999 ) | en_US |
dc.identifier.uri | https://libjncir.jncasr.ac.in/xmlui/10572/714 | |
dc.description | Restricted Access | en_US |
dc.description.abstract | Electron-doped rare-earth manganates of the type Ca(1-x)Ln(x) MnO3 (Ln = La, Nd, Gd or Y) with x = 0.2 and 0.3 show charge ordering in the 150-270 K range, but the charge-ordering transition temperature, T-CO generally decreases with the decrease in the size of the A-site cations, a trend exactly opposite to that for hole-doped manganates. On the other hand, T-CO increases with x or the electron concentration. These trends are also seen for Ca1-xBixMnO3 compounds (T-CO = 300 K for x = 0.3) which show transitions to a more distorted orthorhombic structure below T-CO. In Ca(1-x)Ln(x) MnO3, Cr doping does not melt the charge-ordered state, unlike the case for the hole-doped systems. CaMnO2.82, for which electron doping is affected by anion vacancies, appears to show charge ordering at around 200 K. | en_US |
dc.description.uri | http://dx.doi.org/10.1088/0953-8984/11/5/002 | en_US |
dc.language.iso | en | en_US |
dc.publisher | IOP Publishing Ltd | en_US |
dc.rights | © 1999 IOP Publishing Ltd | en_US |
dc.subject | Magnetoresistance | en_US |
dc.title | Charge ordering in electron-doped manganates | en_US |
dc.type | Article | en_US |