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We have not yet quantified the variability of these values across devices, but compare Fig. 1 to Fig. 3 for an example.
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A simple calculation of the frequency of small oscillations based on a single-rigid-vortex model (Ref.) overestimates the frequency (≈1 GHz at 1 mA) and predicts a linear dependence of frequency on current, different from our observations, but indicates that the Oersted field exerts a substantial restoring force on a vortex.
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A simple calculation of the frequency of small oscillations based on a single-rigid-vortex model (Ref.) overestimates the frequency (≈1 GHz at 1 mA) and predicts a linear dependence of frequency on current, different from our observations, but indicates that the Oersted field exerts a substantial restoring force on a vortex.
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Currents of opposite sign, i.e., negative currents, sometimes-but infrequently-drive small-angle dynamics for low fields. These are never observed for high fields, and should occur only if (1) Mfree and Mfixed are not parallel, and (2) the parallel configuration is somehow destabilized. This would occur if one, but not both, of the layers were in a vortexlike state.
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Currents of opposite sign, i.e., negative currents, sometimes-but infrequently-drive small-angle dynamics for low fields. These are never observed for high fields, and should occur only if (1) Mfree and Mfixed are not parallel, and (2) the parallel configuration is somehow destabilized. This would occur if one, but not both, of the layers were in a vortexlike state.
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