scholarly journals Isotropic, high coercive field in melt-spun tetragonal Heusler Mn3Ge

APL Materials ◽  
2016 ◽  
Vol 4 (8) ◽  
pp. 086113 ◽  
Author(s):  
Adel Kalache ◽  
Guido Kreiner ◽  
Siham Ouardi ◽  
Susanne Selle ◽  
Christian Patzig ◽  
...  
2020 ◽  
Vol 103 (11) ◽  
pp. 6149-6156 ◽  
Author(s):  
Michael J. Brova ◽  
Beecher H. Watson ◽  
Rebecca L. Walton ◽  
Elizabeth R. Kupp ◽  
Mark A. Fanton ◽  
...  

2020 ◽  
Vol 103 (9) ◽  
pp. 4794-4802 ◽  
Author(s):  
Michael J. Brova ◽  
Beecher H. Watson ◽  
Rebecca L. Walton ◽  
Elizabeth R. Kupp ◽  
Mark A. Fanton ◽  
...  

2011 ◽  
Vol 11 (3) ◽  
pp. 2632-2635
Author(s):  
Gunadhor S. Okram ◽  
Ajay Soni ◽  
D. T. Adroja ◽  
N. P. Lalla ◽  
T. Shripathi

2006 ◽  
Vol 304 (2) ◽  
pp. e690-e692 ◽  
Author(s):  
Reiko Sato Turtelli ◽  
João Paulo Sinnecker ◽  
Arbelio Penton-Madrigal ◽  
Roland Grössinger ◽  
Ivan Skorvánek ◽  
...  

2000 ◽  
Vol 644 ◽  
Author(s):  
H. Chiriac ◽  
N. Lupu ◽  
R.E. Vandenberghe ◽  
K.V. Rao

AbstractThe large values over 300 kA/m at room temperature were found for the coercive field of Nd50Fe40Si10−xAlx (x = 0; 10) amorphous melt-spun ribbons and cast rods. The dependence of the coercive field on the thickness and the preparation method, namely the cooling rate, is ascribed to the existence in the amorphous matrix of very small ferromagnetic clusters, which approach of a single magnetic domain. Coercivity increases substantially up to 600 kA/m by decreasing the temperature down to 200 K, although the measurements are carried out in low fields (up to 800 kA/m). The Mässbauer spectra can be fitted to two Fe sites with magnetic moments ranging from 1.25 to 2.20νB depending on the additional element.


2018 ◽  
Vol 124 (21) ◽  
pp. 213904 ◽  
Author(s):  
K. Knížek ◽  
M. Pashchenko ◽  
P. Levinský ◽  
O. Kaman ◽  
J. Houdková ◽  
...  

2014 ◽  
Vol 775-776 ◽  
pp. 437-442 ◽  
Author(s):  
Marcos Flavio de Campos

In the first part of this article, the SW-CLC (Stoner-Wohlfarth with CLC modification) model is discussed for nanocrystalline magnets, as melt-spun exchange coupled NdFeB. In the second part, the effect of grain size of coercivity for large grain size, above the single domain particle size, is addressed. The Kondorsky law observed for large grain size only can be due to domain wall displacement phenomena, where there is nucleus expansion. There are two main situations, one for nanocrystalline grain size, where the SW-CLC model is obeyed, and other for large grain size, where the coercive field decreases proportionally to the square root of the grain size.


1996 ◽  
Vol 32 (5) ◽  
pp. 4570-4572 ◽  
Author(s):  
D. Sander ◽  
A. Enders ◽  
R. Skomski ◽  
J. Kirschner

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