Magnetization and remagnetization of anisotrophic magnetically hard ferrites

1970 ◽  
Vol 6 (2) ◽  
pp. 172-177 ◽  
Author(s):  
H. Stablein
Nanomaterials ◽  
2021 ◽  
Vol 11 (4) ◽  
pp. 924
Author(s):  
Lev A. Trusov ◽  
Anastasia E. Sleptsova ◽  
Jingtong Duan ◽  
Evgeny A. Gorbachev ◽  
Ekaterina S. Kozlyakova ◽  
...  

Magnetically hard ferrites attract considerable interest due to their ability to maintain a high coercivity of nanosized particles and therefore show promising applications as nanomagnets ranging from magnetic recording to biomedicine. Herein, we report an approach to prepare nonsintered single-domain nanoparticles of chromium-substituted hexaferrite via crystallization of glass in the system SrO–Fe2O3–Cr2O3–B2O3. We have observed a formation of plate-like hexaferrite nanoparticles with diameters changing from 20 to 190 nm depending on the annealing temperature. We demonstrated that chromium substitution led to a significant improvement of the coercivity, which varied from 334 to 732 kA m−1 for the smallest and the largest particles, respectively. The results provide a new strategy for producing high-coercivity ferrite nanomagnets.


Nukleonika ◽  
2015 ◽  
Vol 60 (1) ◽  
pp. 29-33
Author(s):  
Mariusz Hasiak

Abstract The microstructure and magnetic properties of nanocomposite hard magnetic Nd-Fe-B-(Re, Ti) materials with different Nd and Fe contents are studied. The role of Re and Ti addition in phase composition and volume fraction of the Nd-Fe-B phase is determined. All samples are annealed at the same temperature of 993 K for 10 min. Mössbauer spectroscopy shows that the addition of 4 at.% of Re to the Nd8Fe78B14 alloy leads to creation of an ineligible amount of the magnetically hard Nd2Fe14B phase. Moreover, the microstructure and magnetic characteristics recorded in a wide range of temperatures for the Nd8Fe79−xB13Mx (x = 4; M = Re or Ti) alloys are also analyzed.


2018 ◽  
Vol 58 (2) ◽  
pp. 602-606 ◽  
Author(s):  
Bo Shen ◽  
Chao Yu ◽  
Alexander A. Baker ◽  
Scott K. McCall ◽  
Yongsheng Yu ◽  
...  

1979 ◽  
Vol 22 (6) ◽  
pp. 664-666
Author(s):  
A. V. Deryagin ◽  
E. A. Barabanova ◽  
N. V. Kudrevatykh ◽  
V. N. Moskalev

1979 ◽  
Vol 22 (7) ◽  
pp. 850-854
Author(s):  
M. A. Artemova ◽  
M. I. Grobovitskii ◽  
V. I. Zingerman

1964 ◽  
Vol 11 (3) ◽  
pp. 218-219 ◽  
Author(s):  
G. Asti ◽  
M. Colombo ◽  
A. Levialdi
Keyword(s):  

2020 ◽  
Vol 62 (2) ◽  
pp. 235
Author(s):  
Д.А. Балаев ◽  
С.В. Семенов ◽  
А.А. Дубровский ◽  
А.А. Красиков ◽  
С.И. Попков ◽  
...  

Fe3O4 / CoFe2O4 nanoparticles with a core-shell structure with an average size of 5 nm were obtained by co-precipitation from solutions of iron and cobalt chlorides. An analysis of the magnetic properties of the resulting system and their comparison with the data for single-phase Fe3O4 (4 nm) and CoFe2O4 (6 nm) nanoparticles led to the conclusion that there is a noticeable interaction between the soft magnetic (Fe3O4) and magnetically hard (CoFe2O4) phases that form the core and the shell of hybrid particles, correspondingly.


2020 ◽  
Vol 224 (2) ◽  
pp. 1256-1271
Author(s):  
Andrei Kosterov ◽  
Mary Kovacheva ◽  
Maria Kostadinova-Avramova ◽  
Pavel Minaev ◽  
Natalia Salnaia ◽  
...  

SUMMARY The thorough understanding of magnetic mineralogy is a prerequisite of any successful palaeomagnetic or archaeomagnetic study. Magnetic minerals in archaeological ceramics and baked clay may be inherited from the parent material or, more frequently, formed during the firing process. The resulting magnetic mineralogy may be complex, including ferrimagnetic phases not commonly encountered in rocks. Towards this end, we carried out a detailed rock magnetic study on a representative collection of archaeological ceramics (baked clay from combustion structures and bricks) from Bulgaria and Russia. Experiments included measurement of isothermal remanence acquisition and demagnetization as a function of temperature between 20 and >600 °C. For selected samples, low-temperature measurements of saturation remanence and initial magnetic susceptibility between 1.8 and 300 K have been carried out. All studied samples contain a magnetically soft mineral identified as maghemite probably substituted by Ti, Mn and/or Al. Stoichiometric magnetite has never been observed, as evidenced by the absence of the Verwey phase transition. In addition, one or two magnetically hard mineral phases have been detected, differing sharply in their respective unblocking temperatures. One of these unblocking between 540 and 620 °C is believed to be substituted hematite. Another phase unblocks at much lower temperatures, between 140 and 240 °C, and its magnetic properties correspond to an enigmatic high coercivity, stable, low-unblocking temperature (HCSLT) phase reported earlier. In a few samples, high- and low unblocking temperature, magnetically hard phases appear to coexist; in the others, the HCSLT phase is the only magnetically hard mineral present.


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