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Giant magnetoresistance (GMR), which was until recently confined to magnetic layered and granular materials, as well as doped magnetic semiconductors, occurs in manganate perovskites of the general formula Ln 1- x A x MnO 3 (Ln = rare earth; A = divalent ion). These manganates are ferromagnetic at or above a certain value of x (or Mn 4+ content) and become metallic at temperatures below the curie temperature, T c . GMR is generally a maximum close to T c or the insulator−metal (I−M) transition temperature, T im . The T c and %MR are markedly affected by the size of the A site cation, 〈 r A 〉, thereby affording a useful electronic phase diagram when T c or T im is plotted against 〈 r A 〉. We discuss GMR and related properties of manganates in polycrystalline, thin-film, and single-crystal forms and point out certain commonalities and correlations. We also examine some unusual features in the electron-transport properties of manganates, in particular charge-ordering effects. Charge ordering is crucially dependent on 〈 r A 〉 or the e g band width, and the charge-ordered insulating state transforms to a metallic ferromagnetic state on the application of a magnetic field.
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Rao et al. (1996) studied this question.
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