Analytic theory for the switch from Bloch to Néel domain wall in nanowires with perpendicular anisotropy
M. D. DeJong and K. L. Livesey
Phys. Rev. B 92, 214420 (2015)
![](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_sjzn_6iAOEHSqrO9NhPsc1HJyXWkl-Cs5glUd63up30fhz-x2SenHZ606MA6PcqDBGZt48DsiGgO0hAsPpYLa-QUKcbOEJEhjvf-BKD-MwhBZ_mzZibxz_CFXYqpXK43lGHsQ98NfH8Hcn6eM1hbiCHQ=s0-d) |
(a) The geometry of a rectangular nanowire with perpendicular magnetic anisotropy, width w and thickness d. Arrows show the direction of magnetization. Depending on the size of w and d,
the lowest energy domain wall may be of (b) Bloch or (c) Néel type. In
the Bloch wall, the magnetization rotates perpendicular to the wire's
long z axis, in the x−y plane. In the Néel wall, the magnetization rotates along the wire's long z axis, in the y−z plane. |
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