scholarly journals Coupling of superconductors through a half-metallic ferromagnet: Evidence for a long-range proximity effect

2004 ◽  
Vol 69 (22) ◽  
Author(s):  
V. Peña ◽  
Z. Sefrioui ◽  
D. Arias ◽  
C. Leon ◽  
J. Santamaria ◽  
...  
2021 ◽  
Author(s):  
D. Sanchez-Manzano ◽  
S. Mesoraca ◽  
F. A. Cuellar ◽  
M. Cabero ◽  
V. Rouco ◽  
...  

2010 ◽  
Vol 84 (6) ◽  
pp. 717-721 ◽  
Author(s):  
Dibya Prakash Rai ◽  
Javad Hashemifar ◽  
Morteeza Jamal ◽  
Lalmuanpuia ◽  
M. P. Ghimire ◽  
...  

2008 ◽  
Vol 255 (3) ◽  
pp. 685-687 ◽  
Author(s):  
R. Tetean ◽  
L. Chioncel ◽  
E. Burzo ◽  
N. Bucur ◽  
A. Bezergheanu ◽  
...  

2018 ◽  
Vol 8 (11) ◽  
pp. 2200 ◽  
Author(s):  
Yu Feng ◽  
Zhou Cui ◽  
Ming-sheng Wei ◽  
Bo Wu ◽  
Sikander Azam

Employing first-principle calculations, we investigated the influence of the impurity, Fe atom, on magnetism and electronic structures of Heusler compound Ti2CoSi, which is a spin gapless semiconductor (SGS). When the impurity, Fe atom, intervened, Ti2CoSi lost its SGS property. As TiA atoms (which locate at (0, 0, 0) site) are completely occupied by Fe, the compound converts to half-metallic ferromagnet (HMF) TiFeCoSi. During this SGS→HMF transition, the total magnetic moment linearly decreases as Fe concentration increases, following the Slate–Pauling rule well. When all Co atoms are substituted by Fe, the compound converts to nonmagnetic semiconductor Fe2TiSi. During this HMF→nonmagnetic semiconductor transition, when Fe concentration y ranges from y = 0.125 to y = 0.625, the magnetic moment of Fe atom is positive and linearly decreases, while those of impurity Fe and TiB (which locate at (0.25, 0.25, 0.25) site) are negative and linearly increase. When the impurity Fe concentration reaches up to y = 1, the magnetic moments of Ti, Fe, and Si return to zero, and the compound is a nonmagnetic semiconductor.


2019 ◽  
Vol 100 (1) ◽  
Author(s):  
A. V. Samokhvalov ◽  
J. W. A. Robinson ◽  
A. I. Buzdin

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