Gh. Rao et al., CRYSTAL-STRUCTURE AND MAGNETORESISTANCE OF LA(2-X) 3NDX/3CA1/3MNO3 - LOCAL LATTICE DISTORTION EFFECT/, Physical review. B, Condensed matter, 55(6), 1997, pp. 3742-3748
The crystal structure, low field ac susceptibility, magnetization, and
magnetoresistance behavior of La-(2-x/3)Ndx/3Ca1/3MnO3 (x=0-2) compou
nds are investigated. The crystal structure of the compounds belongs t
o an orthorhombically distorted perovskite structure. The lattice dist
ortion and the bending of Mn-O-Mn bond increase with the increase of N
d content, ac susceptibility and magnetization measurements show that
the magnetic transition temperature decreases with the increase of Nd
content, and two evident magnetic transitions are observed for x=0.75-
1.0. The magnetization isotherms exhibit a field-induced magnetic tran
sition in the sample. Large magnetoresistance (MR) effects are observe
d in bulk La-(2-x/3)Ndx/3Ca1/3MnO3 at low field. For bulk La1/3Nd1/3Ca
1/3MnO3 a MR ratio as high as -96% is achieved in a field of 0.67 T. T
he maximum MR ratio in a field of 0.67 T increases linearly with the d
ecrease of peak temperature of zero-field resistivity. Based upon the
discussion on local distortions of the lattice and measurements of ac
susceptibility, magnetization, and resistivity, a magnetic inhomogenei
ty model, i.e., simultaneous occurrence of metallic La-rich ferromagne
tic domains and semiconducting Nd-rich domains, is proposed for the ma
gnetic structure of La-(2-x/3)Ndx/3Ca1/3MnO3 compounds. Within the fra
mework of the magnetic inhomogeneity model, it is argued that the occu
rrence of resistivity peak could result from a competition of opposite
temperature dependence of resistivities in La-rich phase and in Nd-ri
ch phase, thus the peak temperature of resistivity does not necessaril
y correspond to a magnetic transition temperature.