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The Magnetic Properties of the Systems La͓Y₁₋͓TiO₃, La͓Gd₁₋͓TiO₃, LaTiO₃ and CeTiO₃

dc.contributor.advisorGreedan, J.E.en_US
dc.contributor.authorGoral, Paul Johnen_US
dc.contributor.departmentChemistryen_US
dc.date.accessioned2014-06-18T16:34:24Z
dc.date.available2014-06-18T16:34:24Z
dc.date.created2010-04-06en_US
dc.date.issued1982-12en_US
dc.description.abstract<p>The magnetic structures of LaTiO₃ and CeTiO₃ were determined by neutron diffraction. LaTiO₃ is a G-type antiferromagnet. The Ti³⁺ sublattice in CeTiO₃ displays G-type and possibly F-type ordering. The Ce³⁺ sublattice exhibits F-type and C-type components.</p> <p>Solid solutions of the form La͓Y₁₋͓TiO₃ and La͓Gd₁₋͓TiO₃ were prepared. Magnetic measurements suggest a weakening of the antiferromagnetic Ti-O-Ti exchange as the Ti-O-Ti bond angle decreases from 157°(LaTiO₃). For sufficiently small bond angle, the Ti-Ti exchange becomes ferromagnetic. Crystal field calculations based on a localized Ti³⁺ 3d¹ electron have reproduced the general features of susceptibility data reported for La͓Y₁₋͓TiO₃ (x=0,.1,.2,.4,.7). This is in agreement with resistivity measurements undertaken on La.₁.₉TiO₃ and La.₂Y.₈TiO₃ which are characteristic of an activated transport mechanism.</p>en_US
dc.description.degreeDoctor of Philosophy (PhD)en_US
dc.identifier.otheropendissertations/1516en_US
dc.identifier.other2177en_US
dc.identifier.other1263605en_US
dc.identifier.urihttp://hdl.handle.net/11375/6187
dc.subjectChemistryen_US
dc.subjectChemistryen_US
dc.titleThe Magnetic Properties of the Systems La͓Y₁₋͓TiO₃, La͓Gd₁₋͓TiO₃, LaTiO₃ and CeTiO₃en_US
dc.typethesisen_US

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