Electrical spin injection from highly spin polarized Co2CrAl Heusler alloy into non-magnetic p-Si semiconductor

2017 ◽  
Vol 185 (1) ◽  
pp. 127-133
Author(s):  
Uddipta Kar ◽  
J. Panda ◽  
T. K. Nath
2016 ◽  
Vol 9 (6) ◽  
pp. 063006 ◽  
Author(s):  
Takehiro Yamaguchi ◽  
Rai Moriya ◽  
Soichiro Oki ◽  
Shinya Yamada ◽  
Satoru Masubuchi ◽  
...  

2001 ◽  
Vol 79 (19) ◽  
pp. 3098-3100 ◽  
Author(s):  
B. T. Jonker ◽  
A. T. Hanbicki ◽  
Y. D. Park ◽  
G. Itskos ◽  
M. Furis ◽  
...  

2006 ◽  
Vol 18 (32) ◽  
pp. 7703-7708 ◽  
Author(s):  
Moon-Ho Ham ◽  
Sukho Yoon ◽  
Yongjo Park ◽  
Lifeng Bian ◽  
Manfred Ramsteiner ◽  
...  

2018 ◽  
Vol 914 ◽  
pp. 111-116 ◽  
Author(s):  
Ya Xin Wang ◽  
Tong Sheng Xia

To obtain a larger spin signal for use in graphene-based spintronic devices, the spin injection efficiency needs to be enhanced. Previously researchers can increase the efficiency by inserting a tunnel barrier such as Al2O3or MgO between ferromagnet and graphene. However, the key value in spin transport is still very low because of the conductance mismatch as well as the limit to fabricate a high-quality tunnel barrier at the junction surface. Here we use a highly spin-polarized ferromagnetic material—Heusler alloy Co2MnGe as a substitutional scheme without the tunnel barrier. The spin injection efficiency of our Co2MnGe (111)/graphene junction can be as high as 73% which is much higher than 1% of ferromagnet/graphene or 30% of ferromagnet/oxide/graphene using first-principles study. The large spin polarization can be explicated by analyzing the transmission spectrum at the nonequilibrium state.


2008 ◽  
Vol 17 (01) ◽  
pp. 105-109
Author(s):  
ASAWIN SINSARP ◽  
TAKASHI MANAGO ◽  
FUMIYOSHI TAKANO ◽  
HIRO AKINAGA

We fabricated an FePt / MgO tunneling junction ( Fe 55 atomic %) on a GaAs -based light-emitting-diode structure. The out-of-plane magnetization of the FePt thin film was confirmed by a magneto-optical measurement. The electrical spin injection from FePt into GaAs at room temperature was studied using the technique of spin-polarized electroluminescence. The spin polarization of the injected electrons under the magnetic field of 1 T was at least 6.0%. The remnant polarization at 0 T, which indicates the spin injection without a magnetic field, was at least 3.3%.


MRS Bulletin ◽  
2003 ◽  
Vol 28 (10) ◽  
pp. 740-748 ◽  
Author(s):  
B.T. Jonker ◽  
S.C. Erwin ◽  
A. Petrou ◽  
A.G. Petukhov

AbstractSemiconductor heterostructures that utilize carrier spin as a new degree of freedom offer entirely new functionality and enhanced performance over conventional devices. We describe the essential requirements for implementing this technology, focusing on the materials and interface issues relevant to electrical spin injection into a semiconductor. These are discussed and illustrated in the context of several prototype semiconductor spintronic devices, including spin-polarized light-emitting diodes and resonant tunneling structures such as the resonant interband tunneling diode.


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