2008
DOI: 10.1103/physrevlett.100.179701
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Li and Rau Reply:

Abstract: Li and Rau Reply: Bode et al., in a Comment [1] on our Letter [2], claim that the vortex (V) core width d vc in magnetic nanodisks (NDs) is on the order of 10 nm and essentially independent of the ND diameter d. We are presenting published data (see also Fig. 1) that clearly show that this claim is incorrect. For instance, a recent transmission electron microscopy experiment on d 6 m Co elements gives d vc 80 nm [3]. Their claim rests in a formula [Eq. (1) in Ref. [1] ] published by Feldtkeller and Thomas [4] … Show more

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Cited by 64 publications
(124 citation statements)
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“…Thus, despite of the three times reduction in the effective strength (χ/3) of the transformed Hamiltonian H eff , the time for observing the optimal SS remains almost the same. Consequently, we expect degradation from atomic losses will be similar to the case of OAT [27].…”
mentioning
confidence: 94%
“…Thus, despite of the three times reduction in the effective strength (χ/3) of the transformed Hamiltonian H eff , the time for observing the optimal SS remains almost the same. Consequently, we expect degradation from atomic losses will be similar to the case of OAT [27].…”
mentioning
confidence: 94%
“…The electrons in the current sheet can also be pre-energized by reflections between the two bubbles, which is a Fermi-like process. Therefore, the current sheet is thermalized, corresponding to a high-beta magnetic reconnection which has a low efficiency at converting magnetic energy into the electron kinetic energy [54]. This is why the electron energization by magnetic reconnection is less significant than the enegization by the magnetic flux pileup and plasma bubble expansion.…”
mentioning
confidence: 99%
“…The double‐ζ and single‐ζ plus polarization basis sets are chosen for carbon and gold atoms, respectively. The electrode temperature is set to 300 K. Although the energy of the spin‐polarized state is about 20 meV per edge atom lower than that of spin‐unpolarized state, the energy is too small to stabilize the spin‐polarized state which would become unstable at finite temperature or in the presence of ballistic current through the device 15. To show the detectable transport properties in experiments, we just consider the spin‐unpolarized state.…”
Section: Computational Detailsmentioning
confidence: 99%