1990
DOI: 10.1016/0375-9601(90)90123-6
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Steady configurations of a square dipole lattice in an external field

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Cited by 6 publications
(3 citation statements)
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“…The long-range order in regular lattices of magnetic dipoles has already been the subject of extensive theoretical inquiry. Most theoretical work on supermagnetism, more specifically on dipolar-coupled magnetic lattices, treat regular arrays with a well-defined lattice symmetry, [11][12][13][14] where the individual dipolar-coupled nanomagnets are assumed to be monodomain. 15 In the present study, we explore supermagnetism in arrays of 5 nm thick circular nanomagnets using the micromagnetic simulation software MuMax3.…”
mentioning
confidence: 99%
“…The long-range order in regular lattices of magnetic dipoles has already been the subject of extensive theoretical inquiry. Most theoretical work on supermagnetism, more specifically on dipolar-coupled magnetic lattices, treat regular arrays with a well-defined lattice symmetry, [11][12][13][14] where the individual dipolar-coupled nanomagnets are assumed to be monodomain. 15 In the present study, we explore supermagnetism in arrays of 5 nm thick circular nanomagnets using the micromagnetic simulation software MuMax3.…”
mentioning
confidence: 99%
“…This third domain will expand with increasing field strength towards both lower and larger values of θ. We can explain this behavior in the context of dipoles in square (non-deformed) Bravais lattices (with a global γ = 1), where the external field breaks the GS degeneracy and orients the dipoles along the field lines -in an AFE (FE) configuration for weak (strong) fields [45]. In other words: in a lattice with γ = 1 the dipoles do not have a preferred alignment direction (w.r.t.…”
Section: General Setup and Methodologymentioning
confidence: 97%
“…This third domain will expand with increasing field strength towards both lower and larger values of θ. We can explain this behavior in the context of dipoles in square (non-deformed) Bravais lattices (with a global γ = 1): In such square lattices, the external field breaks the GS degeneracy and orients the dipoles along the field lines-in an AFE (FE) configuration for weak (strong) fields [53]. In other words: in a lattice with γ = 1 the dipoles do not have a preferred alignment direction (w.r.t.…”
Section: Dws In Deformed Latticesmentioning
confidence: 99%