Magnetic phase diagram of the reentrant spin glass system (Fe0.65Ni0.35)1−xMnx

1992 ◽  
Vol 104-107 ◽  
pp. 2069-2071 ◽  
Author(s):  
A. Wulfes ◽  
Ch. Böttger ◽  
J. Hesse ◽  
J. Sievert ◽  
H. Ahlers
1988 ◽  
Vol 49 (C8) ◽  
pp. C8-1119-C8-1120 ◽  
Author(s):  
R. Rodriguez ◽  
X. Obradors ◽  
A. Labarta ◽  
J. Tejada ◽  
M. Pernet ◽  
...  

Soft Matter ◽  
2014 ◽  
Vol 10 (38) ◽  
pp. 7495-7501 ◽  
Author(s):  
Kevin R. Pilkiewicz ◽  
Joel D. Eaves

Adding a driven, active component to a model spin glass system leads to dramatic shifts in the phase diagram and the emergence of a reentrant glass transition.


1990 ◽  
Vol 41 (16) ◽  
pp. 11405-11416 ◽  
Author(s):  
I. Mirebeau ◽  
S. Itoh ◽  
S. Mitsuda ◽  
T. Watanabe ◽  
Y. Endoh ◽  
...  

1984 ◽  
Vol 80 (5) ◽  
pp. 2079-2086 ◽  
Author(s):  
Gary C. DeFotis ◽  
Christoph Pohl ◽  
Spencer A. Pugh ◽  
Ekk Sinn

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
N. Martin ◽  
L. J. Bannenberg ◽  
M. Deutsch ◽  
C. Pappas ◽  
G. Chaboussant ◽  
...  

AbstractWe study the evolution of the low-temperature field-induced magnetic defects observed under an applied magnetic field in a series of frustrated amorphous ferromagnets (Fe$$_{1-x}$$ 1 - x Mn$$_{x}$$ x )$$_{75}$$ 75 P$$_{16}$$ 16 B$$_{3}$$ 3 Al$$_{3}$$ 3 (“a-Fe$$_{1-x}$$ 1 - x Mn$$_{x}$$ x ”). Combining small-angle neutron scattering and Monte Carlo simulations, we show that the morphology of these defects resemble that of quasi-bidimensional spin vortices. They are observed in the so-called “reentrant” spin-glass (RSG) phase, up to the critical concentration $$x_{\mathrm{C}} \approx 0.36$$ x C ≈ 0.36 which separates the RSG and “true” spin glass (SG) within the low temperature part of the magnetic phase diagram of a-Fe1−xMnx. These textures systematically decrease in size with increasing magnetic field or decreasing the average exchange interaction, and they finally disappear in the SG sample ($$x = 0.41$$ x = 0.41 ), being replaced by field-induced correlations over finite length scales. We argue that the study of these nanoscopic defects could be used to probe the critical line between the RSG and SG phases.


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