2016
DOI: 10.1088/0022-3727/49/18/185006
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The role of the crystal orientation (c-axis) on switching field distribution and the magnetic domain configuration in electrodeposited hcp Co–Pt nanowires

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Cited by 2 publications
(1 citation statement)
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“…Consequently, even geometrically simple cylindrical magnetic nanowires (NWs) of magnetic materials with strong perpendicular magnetocrystalline anisotropy have been shown to exhibit a rich phase diagram of magnetic configurations ranging from uniform magnetization to longitudinal and transverse (multi-)domain states, depending on diameter, length, aspect ratio, externally applied field, and magnetic history of the NW. [19][20][21][22][23][24] Cylindrical magnetic CoNi NWs with a hexagonal close-packed (hcp) crystal structure oriented with their c-axis close to perpendicular to the NW axis are a prominent member of this class, which may be additionally tuned such to also display face-centered cubic (fcc) crystal structure with weaker crystalline anisotropy. [25][26][27][28][29] Previous experimental studies have revealed the existence of (A) a remanent longitudinal vortex state stabilized through the application of a longitudinal external field and/or moderate Ni-to-Co content ratio, and, more recently, (B) a multi-vortex/multi-transverse domain state stabilized by the application of a transverse field and/or low Ni-to-Co content ratio.…”
Section: Introductionmentioning
confidence: 99%
“…Consequently, even geometrically simple cylindrical magnetic nanowires (NWs) of magnetic materials with strong perpendicular magnetocrystalline anisotropy have been shown to exhibit a rich phase diagram of magnetic configurations ranging from uniform magnetization to longitudinal and transverse (multi-)domain states, depending on diameter, length, aspect ratio, externally applied field, and magnetic history of the NW. [19][20][21][22][23][24] Cylindrical magnetic CoNi NWs with a hexagonal close-packed (hcp) crystal structure oriented with their c-axis close to perpendicular to the NW axis are a prominent member of this class, which may be additionally tuned such to also display face-centered cubic (fcc) crystal structure with weaker crystalline anisotropy. [25][26][27][28][29] Previous experimental studies have revealed the existence of (A) a remanent longitudinal vortex state stabilized through the application of a longitudinal external field and/or moderate Ni-to-Co content ratio, and, more recently, (B) a multi-vortex/multi-transverse domain state stabilized by the application of a transverse field and/or low Ni-to-Co content ratio.…”
Section: Introductionmentioning
confidence: 99%