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dc.contributor.authorHaque, A-
dc.contributor.authorShukla, A-
dc.contributor.authorDutta, U-
dc.contributor.authorGhosh, D-
dc.contributor.authorGayen, A-
dc.contributor.authorMahata, P-
dc.contributor.authorVasundhara, M-
dc.contributor.authorKundu, K A-
dc.contributor.authorSeikh, M M-
dc.date.accessioned2020-02-25T13:00:38Z-
dc.date.available2020-02-25T13:00:38Z-
dc.date.issued2019-11-06-
dc.identifier.citationCeramics Internationalen_US
dc.identifier.urihttps://doi.org/10.1016/j.ceramint.2019.11.043-
dc.identifier.urihttp://10.10.100.66:8080/xmlui/handle/123456789/3529-
dc.description.abstractHere we report ambient pressure synthesis, magnetic and dielectric properties of BiCu3Ti3(Fe/Mn)O12 and BiCu2.5Mn0.5Ti2.5Fe1.5O12. Both the samples are crystallized in a cubic Im-3 space group. The antiferromagnetic ground state of A-site copper in Bi2/3Cu3Ti4O12 is differently affected by substitution of nonmagnetic Ti4+ by magnetic Fe and Mn ions in B-site. In contrast to the Mn substitution, the antiferromagnetic ordering of A-site Cu is robust towards Fe substitution. The substitution of iron for Ti4+ initially weakens the antiferromagnetic structure of A-site Cu and eventually it results in the crossover from antiferromagnetic to ferrimagnetic state, whereas the Mn substitution quickly turns antiferromagnetic to ferrimagnetic state. For x > 1.0 Fe-doped sample and low Mn-doped samples exhibit phase separation where the ferromagnetic like phase coexists with antiferromagnetic phase. The glassy magnetic state is realized for x = 1.0 Fe doped sample. The magnetic ground state strongly influences the dielectric behavior of the samples. Near room temperature the dielectric constant value is ~2000 for BiCu3Ti3FeO12, whereas for BiCu2.5Mn0.5Ti2.5Fe1.5O12 the value is much lower (<600) with higher dielectric loss. The leaky nature in magnetically phase separated BiCu2.5Mn0.5Ti2.5Fe1.5O12 can be ascribed to the opening of conducting ferrimagnetic channels. The present investigation revealed that in quadruple perovskite the magnetic and dielectric properties are incompatible where improvement of magnetic response eventually suppresses the dielectric behavior.en_US
dc.language.isoenen_US
dc.publisherScienceDirecten_US
dc.subjectbi-based perovskiteen_US
dc.subjectquadruple perovskiteen_US
dc.subjectferrimagneticen_US
dc.subjectantiferromagneticen_US
dc.subjectdielectric constanten_US
dc.subjectphase separationen_US
dc.titleINCOMPATIBLE MAGNETIC AND DIELECTRIC PROPERTIES OF BiCu3-xMnxTi4-yMyO12 (x = 0 & 0.5; y = 1 & 1.5 and M = Fe & Mn)en_US
dc.typeArticleen_US
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