ferrimagnetic ordering
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2021 ◽  
Vol 853 ◽  
pp. 157256
Author(s):  
Narayanan Kutty Rajeesh Kumar ◽  
Leonid Vasylechko ◽  
Shailja Sharma ◽  
Chandra S. Yadav ◽  
Ramakrishnan Kalai Selvan

2020 ◽  
Vol 117 (1) ◽  
pp. 012401
Author(s):  
Zhendong Chen ◽  
Wenqing Liu ◽  
Peng Chen ◽  
Xuezhong Ruan ◽  
Jiabao Sun ◽  
...  

2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Somnath Jana ◽  
Payel Aich ◽  
P. Anil Kumar ◽  
O. K. Forslund ◽  
E. Nocerino ◽  
...  

AbstractThe magnetic ground states in highly ordered double perovskites LaSr1−xCaxNiReO6 (x = 0.0, 0.5, 1.0) are studied in view of the Goodenough-Kanamori rules of superexchange interactions in this paper. In LaSrNiReO6, Ni and Re sublattices are found to exhibit curious magnetic states separately, but no long range magnetic ordering is achieved. The magnetic transition at ~255 K is identified with the independent Re sublattice magnetic ordering. Interestingly, the sublattice interactions are tuned by modifying the Ni-O-Re bond angles through Ca doping. Upon Ca doping, the Ni and Re sublattices start to display a ferrimagnetically ordered state at low temperature. The neutron powder diffraction data reveals long range ferrimagnetic ordering of the Ni and Re magnetic sublattices along the crystallographic b-axis. The transition temperature of the ferrimagnetic phase increases monotonically with increasing Ca concentration.


2019 ◽  
Vol 58 (22) ◽  
pp. 15529-15535 ◽  
Author(s):  
Lei Gao ◽  
Xiao Wang ◽  
Xubin Ye ◽  
Weipeng Wang ◽  
Zhehong Liu ◽  
...  

2019 ◽  
Vol 289 ◽  
pp. 12-20
Author(s):  
Volodymyr Levytskyi ◽  
Herwig Michor ◽  
Volodymyr Babizhetskyy ◽  
Bogdan Kotur

The isothermal section of the phase diagram of Tb–Fe–C system at 800 °C was studied in the full concentration range using powder X-ray phase and structure analyses, and energy-dispersive X-ray spectroscopy. Six ternary compounds Tb1.88Fe14C, Tb13Fe10C13, TbFeC2, Tb15Fe8C25, Tb5.64Fe2C9, Tb2FeC4 and a limited solid solubility of carbon in the crystal structure of the binary parent compound Tb2Fe17Cх (0≤ х ≤0.8) have been found to exist at 800 °C. The crystal structures of two new ternary carbides have been determined by means of powder X-ray diffraction: Tb15Fe8C25 with structure type Er15Fe8C25, space group P321, a = 11.9706(3) Å, c = 5.1733(2) Å, RB(I) = 0.07, RP = 0.06, RPw = 0.08, and Tb13Fe10C13 with structure type Gd13Fe10C13, space group P3121, a = 9.1800(9) Å, c = 23.703(5) Å, RB(I) = 0.04, RP = 0.16. Both compounds are representatives of the carbometalate class of complex carbides. Tb15Fe8C25 displays an itinerant ferro-or ferrimagnetic ordering of the Fe 3d-moments below TM ≈ 50 K while Tb 4f-moments remain essentially paramagnetic at least down to about 10 K.


2019 ◽  
Vol 99 (5) ◽  
Author(s):  
S. V. Grigoriev ◽  
K. A. Pschenichnyi ◽  
E. V. Altynbaev ◽  
A. Heinemann ◽  
A. Magrez

2019 ◽  
Vol 48 (24) ◽  
pp. 8843-8852
Author(s):  
Xiao-Qin Wei ◽  
Kang-Jie Wang ◽  
Dong-Qing Wu ◽  
Dong Shao ◽  
Le Shi ◽  
...  

Two 3D [MoIII(CN)7]4−-based magnets with new topologies and ferrimagnetic ordering below 80 K have been prepared using different amides as auxiliary ligands.


2018 ◽  
Vol 60 (9) ◽  
pp. 1683
Author(s):  
Б.К. Аргымбек ◽  
С.Е. Кичанов ◽  
Д.П. Козленко ◽  
Е.В. Лукин ◽  
А.Т. Морченко ◽  
...  

AbstractSome specific features of the crystal and magnetic structures of granular powder spinel-like ferrites Mn_0.160Mg_0.404Zn_0.448Fe_2O_4, Mn_0.676Zn_0.227Fe_0.09Fe_2O_4, Mn_0.5792Zn_0.2597Fe_0.1612Fe_2O_4, and Ni_0.32Zn_0.68Fe_2O_4 have been studied by neutron diffraction. It has been established that the crystal structure of all the studied compounds has a cubic symmetry with space group Fd $$\bar 3$$ 3 ¯ m . Ferrimagnetic ordering is observed in all the studied structures. Based on the experimental data, the unit cell parameters and interatomic bond lengths of the studied compounds are determined alongside with the distribution of cations between octahedral and tetrahedral crystallographic positions in their cubic crystal structure. Corresponding average magnetic moments are calculated for different positions in their cubic structure. Some structural mechanisms of the formation of magnetic properties depending on the level of doping and the size of powder grains are discussed.


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