L’ubomir Baňas

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3 with |m| = 1 almost everywhere such that m t = − 1 1 + α 2 m × H eff − α 1 + α 2 m × (m × H eff), where effective field reads H eff = ∆m + π. The operator π denotes some general (nonlinear) field contribution. Challenges for numerical analysis: ▶ efficient treatment of nonlinearities ▶ side constraint |m| = 1 ▶ efficient computation of field contributions(More)
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