Dynamic micromagnetic simulation of the magnetic spectrum of permalloy nanodot array with vortex state

2017 ◽  
Vol 422 ◽  
pp. 57-60 ◽  
Author(s):  
Y. Peng ◽  
G.P. Zhao ◽  
F.J. Morvan ◽  
S.Q. Wu ◽  
M. Yue
2010 ◽  
Vol 405 (4) ◽  
pp. 1172-1175 ◽  
Author(s):  
X.H. Han ◽  
R.L. Liu ◽  
Q.F. Liu ◽  
J.B. Wang ◽  
T. Wang ◽  
...  

2017 ◽  
Vol 31 (22) ◽  
pp. 1750162 ◽  
Author(s):  
Amaresh Chandra Mishra ◽  
R. Giri

Using micromagnetic simulation, the magnetization reversal of soft permalloy rings of torus shape with major radius R varying within 20–100 nm has been investigated. The minor radius r of the torus rings was increased from 5 nm up to a maximum value r[Formula: see text] such that R- r[Formula: see text] = 10 nm. Micromagnetic simulation of in-plane hysteresis curve of these nanorings revealed that in the case of very thin rings (r [Formula: see text] 10 nm), the remanent state is found to be an onion state, whereas for all other rings, the remanent state is a vortex state. The area of the hysteresis loop was found to be decreasing gradually with the increment of r. The normalized area under the hysteresis loops (A[Formula: see text]) increases initially with increment of r. It attains a maximum for a certain value of r = r0 and again decreases thereafter. This value r0 increases as we decrease R and as a result, this peak feature is hardly visible in the case of smaller rings (rings having small R).


2008 ◽  
Vol 103 (1) ◽  
pp. 013910 ◽  
Author(s):  
Ronglin Liu ◽  
Jianbo Wang ◽  
Qingfang Liu ◽  
Haixin Wang ◽  
Changjun Jiang

2018 ◽  
Vol 32 (13) ◽  
pp. 1850156
Author(s):  
Amaresh Chandra Mishra ◽  
R. Giri

The remanent state of elliptical permalloy nanodisks depends on the orientation of the applied magnetic field with respect to the major and minor axes of the nanodisks [A. C. Mishra, Int. J. Mod. Phys. B 30, 1650192 (2016)]. The remanent state is usually an onion state if the external magnetic field is along the major axis, and is a vortex state if the external magnetic field is along the minor axis. In this work, we have analyzed the magnetization reversal of a crossed elliptic disk of permalloy using micromagnetic simulation. This is a new shape where two identical elliptic disks with semi-major axis of length a and semi-minor axis of length b intersect such that they are perpendicular to each other. If the value of b is very close to that of a, then the remanent state is a near saturation state. As the ratio a/b goes down, new complex remanent states are observed. The hysteresis loss is found to be decreased gradually with the increment of b for a given value of b.


2012 ◽  
Vol 538-541 ◽  
pp. 529-533
Author(s):  
Zhen Gang Guo ◽  
Li Qing Pan ◽  
Hong Mei Qiu ◽  
Xue Dan Zhao ◽  
Li Hong Yang

Domain wall motions and magnetization reversal processes in the nanoscale asymmetrical Co50Fe50rings have been studied using micromagnetic simulations. The results reveal that the switching fields and the plateau width of vortex state can be tuned through changing the asymmetrical parameter of magnetic nanorings. The chirality of vortex states can be easily controlled by the orientation of the applied magnetic field.


2019 ◽  
Author(s):  
Danijela Gregurec ◽  
Alexander W. Senko ◽  
Andrey Chuvilin ◽  
Pooja Reddy ◽  
Ashwin Sankararaman ◽  
...  

In this work, we demonstrate the application of anisotropic magnetite nanodiscs (MNDs) as transducers of torque to mechanosensory cells under weak, slowly varying magnetic fields (MFs). These MNDs possess a ground state vortex configuration of magnetic spins which affords greater colloidal stability due to eliminated dipole-dipole interactions characteristic of isotropic magnetic particles of similar size. We first predict vortex magnetization using micromagnetic stimulations in sub-micron anisotropic magnetite particles and then use electron holography to experimentally investigate the magnetization of MNDs 98–226 nm in diameter. When MNDs are coupled to MFs, they transition between vortex and in-plane magnetization allowing for the exertion of the torque on the pN scale, which is sufficient to activate mechanosensitive ion channels in cell membranes.<br>


2007 ◽  
Vol 20 (1) ◽  
pp. 43-49 ◽  
Author(s):  
N. Pompeo ◽  
S. Sarti ◽  
R. Marcon ◽  
H. Schneidewind ◽  
E. Silva

2005 ◽  
Vol 71 (5) ◽  
Author(s):  
S. V. Dordevic ◽  
Seiki Komiya ◽  
Yoichi Ando ◽  
Y. J. Wang ◽  
D. N. Basov

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