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Thermally and field-driven mobility of emergent magnetic charges in square artificial spin ice.


ABSTRACT: Designing and constructing model systems that embody the statistical mechanics of frustration is now possible using nanotechnology. We have arranged nanomagnets on a two-dimensional square lattice to form an artificial spin ice, and studied its fractional excitations, emergent magnetic monopoles, and how they respond to a driving field using X-ray magnetic microscopy. We observe a regime in which the monopole drift velocity is linear in field above a critical field for the onset of motion. The temperature dependence of the critical field can be described by introducing an interaction term into the Bean-Livingston model of field-assisted barrier hopping. By analogy with electrical charge drift motion, we define and measure a monopole mobility that is larger both for higher temperatures and stronger interactions between nanomagnets. The mobility in this linear regime is described by a creep model of zero-dimensional charges moving within a network of quasi-one-dimensional objects.

SUBMITTER: Morley SA 

PROVIDER: S-EPMC6831649 | biostudies-literature | 2019 Nov

REPOSITORIES: biostudies-literature

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Thermally and field-driven mobility of emergent magnetic charges in square artificial spin ice.

Morley Sophie A SA   Porro Jose Maria JM   Hrabec Aleš A   Rosamond Mark C MC   Venero Diego Alba DA   Linfield Edmund H EH   Burnell Gavin G   Im Mi-Young MY   Fischer Peter P   Langridge Sean S   Marrows Christopher H CH  

Scientific reports 20191105 1


Designing and constructing model systems that embody the statistical mechanics of frustration is now possible using nanotechnology. We have arranged nanomagnets on a two-dimensional square lattice to form an artificial spin ice, and studied its fractional excitations, emergent magnetic monopoles, and how they respond to a driving field using X-ray magnetic microscopy. We observe a regime in which the monopole drift velocity is linear in field above a critical field for the onset of motion. The t  ...[more]

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