2013
DOI: 10.1088/1367-2630/15/3/035026
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Chiral nature of magnetic monopoles in artificial spin ice

Abstract: Micromagnetic properties of monopoles in artificial kagome spin ice systems are investigated using numerical simulations. We show that micromagnetics brings additional complexity into the physics of these monopoles that is, by essence, absent in spin models: in addition to a fractionalized classical magnetic charge, monopoles in the artificial kagome ice are chiral at remanence. Our simulations predict that the chirality of these monopoles can be controlled without altering their charge state. This chirality b… Show more

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Cited by 48 publications
(41 citation statements)
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“…Interestingly, the Dirac strings in this two dimensional system are one dimensional [29], which is a signature of 'dimensional reduction due to frustration' [70], and is a consequence of the fact that the strings do not branch which, along with the fact that they do not propagate around corners, can be understood by considering the local dipolar fields [71]. The direction of Dirac string propagation can be controlled, for example, by local chirality of the spins, given by the local curling of the spins at the ends of the islands interacting at a vertex [72] and the chirality of the moving domain wall [73] in a connected system. In the end, the prevailing propagation mechanisms will depend on the orientation of the applied field and the detailed geometry of the system.…”
Section: Emergent Magnetic Monopolesmentioning
confidence: 99%
“…Interestingly, the Dirac strings in this two dimensional system are one dimensional [29], which is a signature of 'dimensional reduction due to frustration' [70], and is a consequence of the fact that the strings do not branch which, along with the fact that they do not propagate around corners, can be understood by considering the local dipolar fields [71]. The direction of Dirac string propagation can be controlled, for example, by local chirality of the spins, given by the local curling of the spins at the ends of the islands interacting at a vertex [72] and the chirality of the moving domain wall [73] in a connected system. In the end, the prevailing propagation mechanisms will depend on the orientation of the applied field and the detailed geometry of the system.…”
Section: Emergent Magnetic Monopolesmentioning
confidence: 99%
“…[15][16][17] Furthermore, in isolated bar systems, monopole chirality may provide additional factors that influence the reversal paths in such systems. 18 Varying the angle of the applied field with respect to the geometrical structuring also offers a route to influence the magnetization reversal by biasing particular sub-lattice directions. Here the angular dependence of the nucleation of a DW from a vertex has been reveal an angular shift in the minimum DW nucleation field due to an asymmetric magnetization distribution at the vertex.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, due to magnetostatics, in elements above a certain thickness (ca. 5-10 nm in Permalloy, depending on lateral dimensions and thickness) the magnetization state changes from an 'onion' state (mostly uniform) to C or S states in which the magnetization bends at the extremities of the element 74 . These changes affect the magnetic symmetry of the vertices and the torques in the presence of an applied field, as shwon in Fig.…”
Section: A Square Icementioning
confidence: 99%