Electronic structures of various (001) and (111) surfaces, interfaces and spin transport properties of half-metallic fully compensated ferrimagnet Cr2Se

2021 ◽  
pp. 161089
Author(s):  
Zhou Cui ◽  
Haonan Ding ◽  
Ke Xu ◽  
Yu Feng
2019 ◽  
Vol 21 (40) ◽  
pp. 22475-22481 ◽  
Author(s):  
Roghayeh Farzadi ◽  
Hossain Milani Moghaddam

We have theoretically investigated spin transport properties of one-dimensional ruthenium-cyclopentadienyl sandwich molecules, Run(Cp)n+1, between two gold electrodes.


2019 ◽  
Vol 31 (30) ◽  
pp. 305501 ◽  
Author(s):  
Jiangchao Han ◽  
Xuming Wu ◽  
Yulin Feng ◽  
Guoying Gao

2018 ◽  
Vol 6 (15) ◽  
pp. 4087-4094 ◽  
Author(s):  
Yulin Feng ◽  
Xuming Wu ◽  
Jiangchao Han ◽  
Guoying Gao

Half-metallic band structure and spin transport characteristics of a 1T-FeCl2 monolayer.


2011 ◽  
Vol 83 (24) ◽  
Author(s):  
Masashi Shiraishi ◽  
Yoshiya Honda ◽  
Eiji Shikoh ◽  
Yoshishige Suzuki ◽  
Teruya Shinjo ◽  
...  

2001 ◽  
Vol 117 (1-3) ◽  
pp. 61-65 ◽  
Author(s):  
Tokio Yamabe ◽  
Masahiro Imade ◽  
Motoki Tanaka ◽  
Thohru Sato

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.


2017 ◽  
Vol 111 (13) ◽  
pp. 132402 ◽  
Author(s):  
Jiangchao Han ◽  
Yulin Feng ◽  
Kailun Yao ◽  
G. Y. Gao

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