TY - GEN
T1 - Crystallographic features of the C-type orbital-ordered, and charge- and orbital-ordered states in the simple perovskite manganite Ca 1-xLaxMnO3
AU - Inoue, Yasuhide
AU - Arao, Masazumi
AU - Shiga, Daisuke
AU - Koyama, Yasumasa
N1 - Copyright:
Copyright 2020 Elsevier B.V., All rights reserved.
PY - 2012
Y1 - 2012
N2 - The C-type orbital-ordered (CTOO), and charge- and orbital-ordered (COO) states are present in the simple perovskite manganite Ca1-xLa xMnO3, which has a three-dimensional highly-correlated electronic system. In this study, the crystallographic features of the CTOO and COO states have been investigated mainly by transmission electron microscopy to understand responses of a lattice system to these orderings. Of these two states, the cooling from the disordered orthorhombic Pnma (DO) state around x = 0.20 resulted in the CTOO state with the monoclinic P21/m symmetry. As a result of the monoclinic distortion as a response of the lattice system, the CTOO state consisted of a banded structure that was characterized by an alternating array of two monoclinic domains with different β values. In 0.30 < x < 0.50, on the other hand, the appearance of the COO state from the DO state on cooling accompanied a transverse lattice modulation with q = [ 0 0ζ]DO as a response to orbital ordering in the COO state. The subsequent cooling in the COO state led to the antiferromagnetic ordering with a large lattice dilatation. In other words, no change in the crystal symmetry occurs in the appearance of the antiferromagnetic ordering.
AB - The C-type orbital-ordered (CTOO), and charge- and orbital-ordered (COO) states are present in the simple perovskite manganite Ca1-xLa xMnO3, which has a three-dimensional highly-correlated electronic system. In this study, the crystallographic features of the CTOO and COO states have been investigated mainly by transmission electron microscopy to understand responses of a lattice system to these orderings. Of these two states, the cooling from the disordered orthorhombic Pnma (DO) state around x = 0.20 resulted in the CTOO state with the monoclinic P21/m symmetry. As a result of the monoclinic distortion as a response of the lattice system, the CTOO state consisted of a banded structure that was characterized by an alternating array of two monoclinic domains with different β values. In 0.30 < x < 0.50, on the other hand, the appearance of the COO state from the DO state on cooling accompanied a transverse lattice modulation with q = [ 0 0ζ]DO as a response to orbital ordering in the COO state. The subsequent cooling in the COO state led to the antiferromagnetic ordering with a large lattice dilatation. In other words, no change in the crystal symmetry occurs in the appearance of the antiferromagnetic ordering.
KW - Charge- and orbital-ordered state
KW - Manganite
KW - Orbital-ordered state
KW - Simple perovskite
KW - Transmission electron microscopy
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U2 - 10.4028/www.scientific.net/MSF.706-709.1612
DO - 10.4028/www.scientific.net/MSF.706-709.1612
M3 - Conference contribution
AN - SCOPUS:84856204210
SN - 9783037853030
T3 - Materials Science Forum
SP - 1612
EP - 1617
BT - THERMEC 2011
PB - Trans Tech Publications Ltd
T2 - 7th International Conference on Processing and Manufacturing of Advanced Materials, THERMEC'2011
Y2 - 1 August 2011 through 5 August 2011
ER -