Abstract:The continued increase in areal densities in magnetic recording makes it crucial to understand magnetization reversal in nanoparticles. We present finite-temperature micromagnetic simulations of hysteresis in Fe nanopillars with the long axis tilted at angles from 0 degrees to 90 degrees to the applied sinusoidal field. The field period is 15 ns, and the particle size is 9 × 9 × 150 nm. The system is discretized into a rectangular pillar of 7 × 7 × 101 spins each with uniform magnetization. At low angles, reve… Show more
“…as expected from the Stoner-Wohlfarth model). The effect of the morphology (cylinder compared to the prolate ellipsoid) is given by the lower values of both fields which was confirmed also in previous works [30]. This drop is, of coarse, more visible when the magnetic field is applied along the nanowires (ϕ H = 0 o ) than when they are close to the perpendicular direction (ϕ H = 90 o ).…”
A systematic micromagnetic study of the morphological characteristic effects over the magnetic static properties of Co-based complex shaped nanowires is presented. The relevance of each characteristic size (i.e. length L, diameter d, and size of the nanowires head T ) and their critical values are discussed in the coercive field optimization goal. Our results strongly confirms that once the aspect ratio ( L d ) of the nanowire is bigger than around 10, the length is no more the pertinent parameter and instead the internal diameter and the shape of the nanowires play a key role. We attribute this behavior to the non uniform distribution of the demagnetizing field which is localized in the nanowires head and acts as a nucleation point for the incoherent magnetization reversal. Finally, angular dependence of the magnetization are simulated and compared to the case of a prolate spheroid for all considered morphologies.
“…as expected from the Stoner-Wohlfarth model). The effect of the morphology (cylinder compared to the prolate ellipsoid) is given by the lower values of both fields which was confirmed also in previous works [30]. This drop is, of coarse, more visible when the magnetic field is applied along the nanowires (ϕ H = 0 o ) than when they are close to the perpendicular direction (ϕ H = 90 o ).…”
A systematic micromagnetic study of the morphological characteristic effects over the magnetic static properties of Co-based complex shaped nanowires is presented. The relevance of each characteristic size (i.e. length L, diameter d, and size of the nanowires head T ) and their critical values are discussed in the coercive field optimization goal. Our results strongly confirms that once the aspect ratio ( L d ) of the nanowire is bigger than around 10, the length is no more the pertinent parameter and instead the internal diameter and the shape of the nanowires play a key role. We attribute this behavior to the non uniform distribution of the demagnetizing field which is localized in the nanowires head and acts as a nucleation point for the incoherent magnetization reversal. Finally, angular dependence of the magnetization are simulated and compared to the case of a prolate spheroid for all considered morphologies.
“…Recent micromagnetic simulation of defect-free d=9 nm Fe nanopillars by Brown et al 26,27 showed that nucleation can start at both ends and propagate through the whole pillars in the time scale of nanoseconds. The calculated H sw is about 2 kOe for the fields applied parallel to the easy axis, which is close to our experimental value.…”
Magnetization reversal of individual, isolated high-aspect-ratio Fe nanoparticles with diameters comparable to the magnetic exchange length is studied by high-sensitivity submicron Hall magnetometry. For a Fe nanoparticle with diameter of 5 nm, the magnetization reversal is found to be an incoherent process with localized nucleation assisted by thermal activation, even though the particle has a single-domain static state. For a larger elongated Fe nanoparticle with a diameter greater than 10 nm, the inhomogeneous magnetic structure of the particle plays important role in the reversal process.
“…In this section we summarize recent simulation results for magnetization reversal in iron nanopillars 40 , and further evaluate these results in light of additional experimental data on such reversal. Figure 2a shows hysteresis loops at T = 100 K for the full micromagnetic model with the field misaligned at 0 • , 45 • , and 90 • to the long axis of the particle.…”
Section: Results Of Micromagnetic Simulationsmentioning
confidence: 92%
“…In this section we summarize recent simulation results for magnetization reversal in iron nanopillars 40 , and further evaluate these results in light of additional experimental data on such reversal.…”
Section: Results Of Micromagnetic Simulationsmentioning
We examine different models and methods for studying finite-tempera-ture magnetic hysteresis in nanoparticles and ultrathin films. This includes micromagnetic results for the hysteresis of a single magnetic nanoparticle which is misaligned with respect to the magnetic field. We present results from both a representation of the particle as a one-dimensional array of magnetic rotors, and from full micromagnetic simulations. The results are compared with the Stoner-Wohlfarth model. Results of kinetic Monte Carlo simulations of ultrathin films are also presented. In addition, we discuss other topics of current interest in the modeling of magnetic hysteresis in nanostructures, including kinetic Monte Carlo simulations of dynamic phase transitions and First-Order Reversal Curves.
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