PERTURBED MAGNETIC-ORDERING IN THE DISORDERED SPINEL ZNXCO1-XFECRO4

被引:38
|
作者
CHAKRAVARTHY, R
RAO, LM
PARANJPE, SK
KULSHRESHTHA, SK
ROY, SB
机构
[1] BHABHA ATOM RES CTR,DIV SOLID STATE PHYS,BOMBAY 400085,INDIA
[2] BHABHA ATOM RES CTR,DIV CHEM,BOMBAY 400085,INDIA
[3] UNIV LONDON IMPERIAL COLL SCI & TECHNOL,BLACKETT LAB,LONDON SW7 2BZ,ENGLAND
来源
PHYSICAL REVIEW B | 1991年 / 43卷 / 07期
关键词
D O I
10.1103/PhysRevB.43.6031
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Neutron-diffraction results on Zn(x)Co(1-x)FeCrO4 (x = 0.45, 0.50, and 0.55) and ac susceptibility measurements are described. Neutron measurements were extended down to 6 K for the x = 0.50 compound to check the magnetic structure associated with the phase transition seen in X(ac) around 20 K for the x greater-than-or-equal-to 0.50 compounds. For Zn ion concentration greater than 0.45, the broad distribution of X(ac) and the sluggish behavior of the ordered magnetic moment in the temperature range 300 greater-than-or-equal-to T greater-than-or-equal-to 100 K suggest the presence of finite magnetic clusters coexisting with the infinite magnetic network. For all the compositions, considerable reduction in the B-site moment and the absence of the (200) magnetic reflection confirm that the system is not a conventional ferrimagnet. The most interesting feature is the appearance of a diffuse hump at a Q value corresponding to the (200) reflection for x = 0.50, indicating the buildup of short-range correlation of the transverse components of the B-site moments. On further lowering the temperature, the intensity of the fundamental Bragg reflection decreases below 10 K, while the diffuse hump persists. A qualitative explanation of all these observed features is given in light of theoretical ideas on random magnetic systems.
引用
收藏
页码:6031 / 6036
页数:6
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