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H = 0.00166 in the time-domain calculation. We attribute most of the discrepancy to the inadequacy of the tight-binding approximation, the finite bandwidth of the beam, and the numerical inaccuracies of the simulations.
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24
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note
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One might wonder about the practicality of applying a large positive field in one arm and a large negative field in the other arm of such a tiny device. All that is required, however, is to establish a strong gradient of the field between the two arms.
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