(13) If the chain is suﬃciently long we may neglect the edge ef- fects and assume that the deviation induced by the dipo- lar ﬁeld is nearly constant over the whole chain

in the expression of the second derivative, keeping only the linear terms in ξ, leads to E ∥ s ≃ E (0) s∥ + 1 2 k ( h2 k2 − 1 ) [ 1 + 8 h2 k2 ξI k 1 − h2 k2 ]    =− λt<0 (θ

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Magnetization Dynamics in 1D Chains of Ferromagnetic Nanoparticles Coupled with Dipolar Interactions: Blocking Temperature

cond-mat.mes-hall · 2019-07-11 · unverdicted · novelty 5.0

The paper evaluates the qualitative variation of the blocking temperature TB as a function of interparticle distance a and external field h in linear chains of ferromagnetic nanoparticles with long-range dipolar interactions for two geometries: longitudinal axial anisotropy in longitudinal or in a

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Magnetization Dynamics in 1D Chains of Ferromagnetic Nanoparticles Coupled with Dipolar Interactions: Blocking Temperature cond-mat.mes-hall · 2019-07-11 · unverdicted · none · ref 4
The paper evaluates the qualitative variation of the blocking temperature TB as a function of interparticle distance a and external field h in linear chains of ferromagnetic nanoparticles with long-range dipolar interactions for two geometries: longitudinal axial anisotropy in longitudinal or in a

(13) If the chain is suﬃciently long we may neglect the edge ef- fects and assume that the deviation induced by the dipo- lar ﬁeld is nearly constant over the whole chain

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