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• W2085206125 abstract "Numerical calculations of the average dipole-coupling energy $bar E_mathrm{dip}$ in two-dimensional disordered magnetic nanostructures are performed as function of the particle coverage $C$. We observe that $bar E_mathrm{dip}$ scales as $bar E_mathrm{dip}propto C^{alpha^*}$ with an unusually small exponent $alpha^*simeq 0.8$--1.0 for coverages $Clesssim20%$. This behavior is shown to be primarly given by the contributions of particle pairs at short distances, which is intrinsically related to the presence of an appreciable degree of disorder. The value of $alpha^*$ is found to be sensitive to the magnetic arrangement within the nanostructure and to the degree of disorder. For large coverages $Cgtrsim20%$ we obtain $bar E_mathrm{dip}propto C^alpha$ with $alpha=3/2$, in agreement with the straighforward scaling of the dipole coupling as in a periodic particle setup. Taking into account the effect of single-particle anisotropies, we show that the scaling exponent can be used as a criterion to distinguish between weakly interacting ($alpha^* simeq 1.0$) and strongly interacting ($alpha^* simeq 0.8$) particle ensembles as function of coverage." @default.
• W2085206125 created "2016-06-24" @default.
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• W2085206125 date "2003-11-20" @default.
• W2085206125 modified "2023-10-01" @default.
• W2085206125 title "Scaling behavior of the dipole-coupling energy in two-dimensional disordered magnetic nanostructures" @default.
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• W2085206125 doi "https://doi.org/10.1103/physrevb.68.184420" @default.
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