2001
DOI: 10.1109/20.951231
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Grain-boundary micromagnetism

Abstract: Abstract-Continuum and layer-resolved calculations are used to investigate the spin structure in the vicinity of grain boundaries. Reduced exchange in the grain-boundary region gives rise to a quasidiscontinuity of the magnetization and yields a perturbation which decays exponentially inside the grains. An effective intergranular exchange is obtained as a micromagnetically well-defined function of the grain-boundary exchange, and it is discussed how grain boundaries affect the hysteresis loops of nanostructure… Show more

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Cited by 33 publications
(37 citation statements)
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“…The magnetocrystalline anisotropy is ignored in these calculations, but their inclusion is straightforward. 22 For grains that touch each other with a contact area pR c 2 , as in Fig. 1(b), it is reasonable to assume that the magnetization change is localized in a volume of order 4pR 3 /3.…”
Section: Effective Exchange Stiffnessmentioning
confidence: 99%
“…The magnetocrystalline anisotropy is ignored in these calculations, but their inclusion is straightforward. 22 For grains that touch each other with a contact area pR c 2 , as in Fig. 1(b), it is reasonable to assume that the magnetization change is localized in a volume of order 4pR 3 /3.…”
Section: Effective Exchange Stiffnessmentioning
confidence: 99%
“…8,9 In the past, theoretical research has largely focused on quasione-dimensional structures, which have been tackled by phenomenological continuum and atomicresolution methods. [10][11][12][13][14] From a theoretical point of view, the spin structure at granular interfaces and in constrained domain walls was first investigated in the context of polycrystalline rare-earth transition-metal intermetallics, 10 although various earlier articles, such as Refs. [15][16][17][18][19], anticipate much of the involved physics.…”
Section: Introductionmentioning
confidence: 99%
“…13,14 Furthermore, the reduced exchange at interfaces gives rise to a quasidiscontinuity of the magnetization. In the absence of external fields it has a relative strength of 1/(1ϩ2AЈ␦ o /AD), where D is the thickness of the interface, and A and AЈ are the exchange stiffnesses in the bulk and in the interface region, respectively.…”
Section: Introductionmentioning
confidence: 99%
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“…To exploit the catalytic potential of nanoparticles, it is necessary to stabilize the magnetization at the reaction temperature. This may be achieved by using several magnetic impurities per cluster, by a moderate pressure to realize an effective exchange coupling 11,12 between particles, and/or by using catalytically inert particles such as Fe as exchange bridges.…”
Section: Introductionmentioning
confidence: 99%