Spin polarized carrier injection driven magneto-optical Kerr effect in Cr-doped ZnO nanorods

2019 ◽  
Vol 383 (24) ◽  
pp. 2988-2992 ◽  
Author(s):  
M. Malaidurai ◽  
B. Santosh Kumar ◽  
R. Thangavel
RSC Advances ◽  
2016 ◽  
Vol 6 (48) ◽  
pp. 42517-42521 ◽  
Author(s):  
R. Ciprian ◽  
C. Baratto ◽  
A. Giglia ◽  
K. Koshmak ◽  
G. Vinai ◽  
...  

A new system based on a Co film covered by ZnO nanorods has been fabricated with sputtering technique. It represents a promising candidate for future generation of magnetic gas sensing devices.


1995 ◽  
Vol 51 (8) ◽  
pp. 5586-5589 ◽  
Author(s):  
R. Mégy ◽  
A. Bounouh ◽  
Y. Suzuki ◽  
P. Beauvillain ◽  
P. Bruno ◽  
...  

2009 ◽  
Vol 1198 ◽  
Author(s):  
Yuet-Loy Chan ◽  
Ya-Jyuan Hung ◽  
Chia-Hao Wang ◽  
Ying-Chang Lin ◽  
Ching-Yuan Chiu ◽  
...  

AbstractThe interfacial regimes of cobalt/pentacene/cobalt (Co/Pc/Co) trilayers were emulated through the ultrathin pentacene/cobalt (Pc/Co) and cobalt/pentacene (Co/Pc) bilayers. Employing the magneto-optical Kerr effect (MOKE) measurement, we found the coercivity of Co bottom film in a thickness of 3.4 nm experienced a slight reduction upon the adsorption of Pc molecules. For the bilayers prepared with reversed order of deposition, the Co film deposited on a 6.4 nm Pc layer showed no observable ferromagnetic order at room temperature until its thickness reached 3 nm. After the onset of magnetic order, the x-ray images acquired on Pc/Co revealed a complicated magnetization patterns comparing to those observed on Co/Pc bilayers. Because the spin-polarized carriers will interact with the environment along their transport path, the presence of a non-magnetic layer and the occurrence of complicated domain structures suggested the spin-polarized carriers would experience a greater disturbance on their spin coherence when crossing the Pc/Co interface.


1993 ◽  
Vol 313 ◽  
Author(s):  
C. Chappert ◽  
D. Weiler ◽  
H. Tang ◽  
J.C. Scott ◽  
H. Hopster ◽  
...  

ABSTRACTWe have characterized magnetization loops of epitaxially grown Gd (0001) films on W (110) in the temperature range 145≤T≤300K. This was accomplished by measuring magneto-optical Kerr loops in UHV, in the transverse geometry, using a 2×10-4 deg sensitivity differential detector and He-Ne laser light.Films grown in the Stranski-Krastanov (SK) Mode (growth temperature 400°C) and films grown in a Frank-van-der-Merwe (FM) like Mode (growth temperature 20°C) behave significantly differently. While the room temperature grown films (FM) show square hysteresis behavior only after an annealing cycle to at least 300°C, the higher growth temperature (SK) leads to highly remanent films in the as grown state.The hysteresis behavior of these films is most important in conjunction with recently reported spin-polarized photoemission results, which showed that the growth temperature and therefore the film morphology has a strong influence on the surface magnetic reconstruction of Gd (0001) [1].


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