dc.description.abstract | Doped rare-earth manganites with the general formula T1xDxMnO3 where `T' is a trivalent
rare earth ion, e.g. La3+;Nd3+; Pr3+ etc. and `D' is a divalent alkaline earth ion,
e.g Ca2+; Sr2+;Ba2+ etc. display various interesting properties. They attracted research
attention because of their unique properties and potential applications [1{5]. These materials
exhibit exciting properties like CMR (colossal magneto resistance), charge ordering
(CO), orbital ordering (OO), ferromagnetism (FM), antiferromagnetism (AFM),
phase separation (PS), electron-hole asymmetry, phase complexities, exchange bias effects
etc. [1,2,6]. These exciting properties exhibited by manganite system are explained
using various interactions taking place in the system like, super exchange (SE), double
exchange (DE), Dzyaloshinsky-Moriya interaction (DM interaction), eg eg coulombic
interactions, electron-phonon interactions etc. [7{9]. In parent compounds TMnO3 and
DMnO3, all Mn ions are in Mn3+ and Mn4+ states respectively. These parent compounds
are governed by SE interaction resulting in AFM insulating phase. On doping
with divalent alkaline earth ion in TMnO3, there is a transition from AFM insulating
phase to canted AFM phase, then to FM insulating phase and FM conducting phase
depending on the ratio of Mn3+ and Mn4+ ions. Manganites depict principal magnetic
and electronic properties across the temperature and composition range. So the phase
diagrams of manganites are complex with various phases like AFM insulating, canted
AFM, FM insulating, FM metallic, PM, CO, OO etc. These phases are very sensitive to
external pressure and magnetic eld. Further research in manganites shows that these
are complicated systems exhibiting strong correlations between electron, spin, lattice and
orbital degrees of freedom.
It is also found that some of the above properties are suppressed when the size of
these particles are reduced to nano-scale. For example the CO phase has been observed
to suppress/completely disappear depending on the size of the particle [10{12].
Electron-hole asymmetry has also been seen to disappear in nanomanganites [13, 14].
Phase complexities, seen in the bulk [14] particles are observed to disappear. These
nanomanganites also display other properties which are not seen in their bulk counterpart,
like ferromagnetism, superparamagnetism, exchange-bias, spin-glass state etc. [15].
In nanomanganites, researchers have come up with various theories to explain the properties
exhibited by them. Among these core-shell model is generally beleived to be most
applicable [16].
Our main objective in this thesis was to perform EPR/FMR studies on certain doped
rare-earth manganites, in polycrystalline bulk and nano form. In this we study di erent
manganite systems exhibiting unique and interesting properties at certain doping
level and try understanding them by performing temperature dependent EPR measurements.
These studies are supplemented by DC magnetization studies to characterize the
magnetic states of the samples. The thesis is organized into chapters as follows. | en_US |