Magnetic and Electric properties of La_{1-delta}MnO_{3}
arXiv:cond-mat/9803024 · doi:10.1103/PhysRevB.59.1304
Abstract
The magnetic phase diagram of powdered samples have been studied as a function of in the low doping range. has a canted magnetic structure at low temperature $(θ\simeq 130\QTR{group}{{}^{\circ}})$. Above , it becomes a paramagnet with a huge effective magnetic moment, , reflecting the presence of magnetoelastic polarons which are not affected by the magnetic field (up to 20T) nor the temperature . When is increased to , polarons are still presen at high temperature, with a smaller size: . The system becomes fully ferromagnetic below 170K but remains insulating down to the lowest temperature.
8pages; 6 figures as EPS files added
References in corpus (6)
- Double Exchange Alone Does Not Explain the Resistivity of
- Dynamic Jahn-Teller Effect and Colossal Magnetoresistance in
- Transport Properties of the Kondo Lattice Model in the Limit and
- Electronic and Magnetic States in the Giant Magneto-resistive Compounds
- Liquid-like spatial distribution of magnetic polarons revealed by neutron scattering in La{1-x}Ca{x}MnO3
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- The effect of oxygen stoichiometry on electrical transport and magnetic properties of La0.9Te0.1MnOy
- Electric field driven destabilization of the insulating state in nominally pure LaMnO3
- Inhomogeneous phase separation and domain wall dynamics in the orthorhombically distorted La_{0.87}MnO_x
- Influence of the Magnetic Sub-Lattices in the Double Perovskite Compound LaCaNiReO
- LiSr[MnN]: a magnetically ordered, metallic nitride