2014
DOI: 10.1103/physrevb.90.104417
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Spin-wave edge modes in finite arrays of dipolarly coupled magnetic nanopillars

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Cited by 52 publications
(43 citation statements)
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“…An accurate treatment of the finite magnetic systems require: (i) taking into account the boundary conditions at the system's edges, and (ii)taking into account the demagnetization field for all the periodic structure. This demagnetization field is shape-dependent (and not lattice-dependent), and, also, is non-uniform across the structure 31,33 . Several attempts were undertaken to treat finite magnetic periodic structures, either by using the PWE methods 48,49 or by developing dedicated methods for special cases 34 .…”
Section: Novel Magnonicmentioning
confidence: 99%
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“…An accurate treatment of the finite magnetic systems require: (i) taking into account the boundary conditions at the system's edges, and (ii)taking into account the demagnetization field for all the periodic structure. This demagnetization field is shape-dependent (and not lattice-dependent), and, also, is non-uniform across the structure 31,33 . Several attempts were undertaken to treat finite magnetic periodic structures, either by using the PWE methods 48,49 or by developing dedicated methods for special cases 34 .…”
Section: Novel Magnonicmentioning
confidence: 99%
“…Thus, the properties of the edge excitations in such systems should be wellunderstood. In one of our previous works 33 we calculated the spectrum of collective spin wave edge modes in a periodic dipolarly coupled nanodot array having one dot per a primitive cell. However, for an array of magnetic nanodots to have such interesting and unusual properties as non-reciprocity of a spin wave spectra 19 or non-trivial topological properties of a spin wave pass-bands 34,35 , it is necessary to have a complex primitive cell, e.g.…”
Section: Novel Magnonicmentioning
confidence: 99%
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“…This is consistent with the calculated SW energy spectrum. At this point, it should be emphasized that the dependence of the Berry phase on the crystal momentum is the consequence of the conservation of the time reversal symmetry, in contrast to the non-reciprocity of SW propagation 25,26 , which requires the violation of the time reversal symmetry.…”
Section: Spin Wave Eigenmodesmentioning
confidence: 99%