2022
DOI: 10.1103/physrevb.105.104435
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High spin-wave asymmetry and emergence of radial standing modes in thick ferromagnetic nanotubes

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Cited by 10 publications
(2 citation statements)
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“…In the next few decades, numerous research works are focused on the accelerating development of opto‐magnetization recording. To facilitate the potential applications in all‐optical magnetic recording, [ 7,8 ] magnetic resonance microscopy, [ 9,10 ] atom trapping, [ 11,12 ] holography [ 13 ] and manipulation of the spin wave, [ 14 ] the super‐resolved magnetization structures such as a single ellipsoidal or spherical magnetization spot, [ 15,16 ] magnetization needle, [ 17,18 ] magnetization spot arrays, [ 19,20 ] magnetization chain, [ 21,22 ] magnetic vortex core, [ 23 ] and twisted longitudinal magnetization texture [ 24 ] are garnered by tightly focusing the incident light fields tailored with amplitude, phase, and polarization modulations. The magnetization domain of these versatile magnetization structures is still inferior to the ultimate limit of 0.36λ/NA [ 18,25 ] (NA is the numerical aperture of the objective lens), which degrades the ultra‐high density storage.…”
Section: Introductionmentioning
confidence: 99%
“…In the next few decades, numerous research works are focused on the accelerating development of opto‐magnetization recording. To facilitate the potential applications in all‐optical magnetic recording, [ 7,8 ] magnetic resonance microscopy, [ 9,10 ] atom trapping, [ 11,12 ] holography [ 13 ] and manipulation of the spin wave, [ 14 ] the super‐resolved magnetization structures such as a single ellipsoidal or spherical magnetization spot, [ 15,16 ] magnetization needle, [ 17,18 ] magnetization spot arrays, [ 19,20 ] magnetization chain, [ 21,22 ] magnetic vortex core, [ 23 ] and twisted longitudinal magnetization texture [ 24 ] are garnered by tightly focusing the incident light fields tailored with amplitude, phase, and polarization modulations. The magnetization domain of these versatile magnetization structures is still inferior to the ultimate limit of 0.36λ/NA [ 18,25 ] (NA is the numerical aperture of the objective lens), which degrades the ultra‐high density storage.…”
Section: Introductionmentioning
confidence: 99%
“…They are extremely versatile as their properties change as a function of, both, their geometrical parameters, namely length, inner and outer radius, [10][11][12] and their axial, helical or vortex-like magnetic configuration [13,14]. A curvature-induced magnetochiral field originating from dipole-dipole interaction is expected [15] and can induce non-reciprocal spin-wave dispersion relations in case of cylindrical NTs with nanometric radii [8,14,[16][17][18][19]. Previous experimental studies based on microtubes prepared from rolled-up ferromagnetic layers [20,21] have not addressed magnetochiral effects as radii were in the micrometer regime.…”
mentioning
confidence: 99%