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Structure, magnetism and giant dielectric constant of BiCr0.5Mn0.5O3 synthesized at high pressures

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dc.contributor.author Mandal, P
dc.contributor.author Iyo, A
dc.contributor.author Tanaka, Y
dc.contributor.author Sundaresan, A
dc.contributor.author Rao, C N R
dc.date.accessioned 2011-03-04T06:57:27Z
dc.date.available 2011-03-04T06:57:27Z
dc.date.issued 2010
dc.identifier 0959-9428 en_US
dc.identifier.citation Journal of Materials Chemistry 20(9), 1646-165 (2010) en_US
dc.identifier.uri https://libjncir.jncasr.ac.in/xmlui/10572/59
dc.description.abstract BiCr0.5Mn0.5O3, synthesized at high pressure and high temperature, has a monoclinic structure (space group C2/c) at room temperature with a 9.4590(3) angstrom, b 5.5531(2) angstrom, c 9.6465(3) angstrom and beta = 108.149(2)degrees. It undergoes a structural transition from the monoclinic to an orthorhombic (Pnma) symmetry around 650 K. Magnetic measurements show three distinct anomalies at 25, 50 and 97 K. AC susceptibility measurements confirm the occurrence of the magnetic anomalies, but suggest no spin frustration. Interestingly, this oxide shows a giant dielectric constant at room temperature. Two clear relaxation processes commencing around 200 K and 300 K are exhibited by this material. The first relaxation process is due to Maxwell-Wagner polarization at the grain boundary whereas the second relaxation may arise from hopping of electrons in the B-site. en_US
dc.description.sponsorship Department of Science and Technology (DST), Government of India , Japan Science and Technology (JST), Japan en_US
dc.description.uri http://dx.doi.org/10.1039/b914350p en_US
dc.language.iso en en_US
dc.publisher The Royal Society of Chemistry en_US
dc.rights © 2010 The Royal Society of Chemistry en_US
dc.subject Crystal-Structure en_US
dc.subject BiMnO3; en_US
dc.subject BiCrO3 en_US
dc.subject BiFeO3 en_US
dc.title Structure, magnetism and giant dielectric constant of BiCr0.5Mn0.5O3 synthesized at high pressures en_US
dc.type Article en_US


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