APS March Meeting 2013
Volume 58, Number 1
Monday–Friday, March 18–22, 2013;
Baltimore, Maryland
Session C10: Invited Session: Stabilization and Dynamics of Magnetic Skyrmions
2:30 PM–5:30 PM,
Monday, March 18, 2013
Room: 309
Sponsoring
Units:
DCMP GMAG
Chair: N.P. Onn, Princeton University
Abstract ID: BAPS.2013.MAR.C10.3
Abstract: C10.00003 : Realization and dynamics of 2D magnetic skyrmions*
3:42 PM–4:18 PM
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Abstract
Author:
Xiuzhen Yu
(The Institute of Physical and Chemical Research)
The skyrmion, a vortex-like topological spin texture, can be excited by the
external magnetic field (B) in helimagnets [1-6]. The skyrmion lattice was
recently confirmed by small-angle scattering neutron observations in a
helimagnet MnSi [1] where the skyrmion phase was observed in a narrow window
of (T, B)-plane. In contrast with unstable skyrmions in the bulk, by using
Lorentz transmission electron microscopy (TEM), we have realized
two-dimensional (2D) skyrmion crystal (SkX) over a wider region in (T,
B)-plane for thin helimagnets [2-6] which thicknesses are smaller than their
helical periods. Furthermore, we have realized the near RT ($\sim$280 K) formation of SkX in a helimagnet FeGe [3]. We have clarified the
stability condition for the SkX, i.e. the magnetic-dimension (from 2D to 3D)
variation of SkX phase diagram in (T, B)-plane.
The skyrmion acts as a magnetic flux owing to its curved spin texture. When
an electric current flowing through the skyrmion exceeds a critical current
density for depinning, the skyrmion can accept the spin transfer torque to
be driven along the current direction. Combining electrical and magnetic
control in a microdevice composed of a FeGe thin plate, we have realized
nanometric skyrmions under a weak magnetic field (150 mT) and manipulated
them with an ultra-low current density ($\sim$ 5 $\times$ 10$^{4}$A/m$^{2})$
[6], several orders lower than that required to drive domain walls in
conventional ferromagnets [7].
This work has been done in collaboration with Prof. Y. Tokura, Prof. N.
Nagaosa, Dr. Y. Matsui, Prof. Y. Onose, Mr. N. Kanazawa, Dr. K. Kimoto, Dr.
T. Hara, Dr. T. Nagai, and Ms. W-Z. Zhang.
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[1] S. M\"uhlbauer, \textit{et al}., \textbf{Science} \textbf{323}, 915 (2009)\\[0pt]
[2] X.Z. Yu, \textit{et al.}, \textit{Nature} \textbf{465}, 901 (2010)\\[0pt]
[3] X.Z. Yu, \textit{et al}., \textit{Nat. Mater. }\textbf{10}, 106 (2011)\\[0pt]
[4] S. Seki, \textit{et al}., \textit{Science} \textbf{336}, 198 (2012)\\[0pt]
[5] A. Tonomura, \textit{et al}. \textit{Nano Lett.} \textbf{102}, 186602 (2012)\\[0pt]
[6] X.Z. Yu, \textit{et al}., \textit{Nat. Commun.}, \textbf{3}:988(2012) \\[0pt]
[7] S. Parkin, \textit{et al}., \textit{Science}, \textbf{320}, 190 (2008)
*This work was supported by Funding Program for World-Leading Innovative R\&D on Science and Technology (FIRST program).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2013.MAR.C10.3