Direct observation of magnetic vortex behavior in an ordered La0.7Sr0.3MnO3 dot arrays

2016 ◽  
Vol 18 (40) ◽  
pp. 28254-28261 ◽  
Author(s):  
Zhenghua Li ◽  
Dapeng Dong ◽  
Dedi Liu ◽  
Jia Liu ◽  
Dongping Liu ◽  
...  

Directly observing the magnetic domain behavior in patterned nanostructures is crucial to the investigation into advanced spin-based devices.

2006 ◽  
Vol 3 (1) ◽  
pp. 21-25 ◽  
Author(s):  
Masamitsu Hayashi ◽  
Luc Thomas ◽  
Charles Rettner ◽  
Rai Moriya ◽  
Stuart S. P. Parkin

2008 ◽  
Vol 44 (11) ◽  
pp. 3241-3243 ◽  
Author(s):  
J.B. Kim ◽  
Y.P. Lee ◽  
K.-S. Ryu ◽  
S.-C. Shin ◽  
K.W. Kim ◽  
...  

AIP Advances ◽  
2018 ◽  
Vol 8 (5) ◽  
pp. 056801
Author(s):  
S. L. Zuo ◽  
B. Zhang ◽  
K. M. Qiao ◽  
L. C. Peng ◽  
R. Li ◽  
...  

1980 ◽  
Vol 45 (1) ◽  
pp. 74-74 ◽  
Author(s):  
Akira Tonomura ◽  
Tsuyoshi Matsuda ◽  
Junji Endo ◽  
Tatsuo Arii ◽  
Kazuhiro Mihama ◽  
...  

Author(s):  
T. Ono

This chapter defines a magnetic domain wall (DW) as the transition region where the direction of magnetic moments gradually change between two neighbouring domains. It has been pointed out that ferromagnetic materials are not necessarily magnetized to saturation in the absence of an external magnetic field. Instead, they have magnetic domains, within each of which magnetic moments align. The formation of the magnetic domains is energetically favourable because this structure can lower the magnetostatic energy originating from the dipole–dipole interaction. A magnetic vortex realized in a ferromagnetic disk is a typical example of nonuniform magnetic structure. In very small ferromagnetic systems, where a curling spin configuration has been proposed to occur in place of domains, the formation of DWs is not energetically favored.


2016 ◽  
Vol 43 (16) ◽  
pp. 8426-8434 ◽  
Author(s):  
Trevor P. Almeida ◽  
Adrian R. Muxworthy ◽  
András Kovács ◽  
Wyn Williams ◽  
Leslei Nagy ◽  
...  

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