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Far away from the quantum wire (in the y direction), our system contains a narrow region with opposite field direction such that the overall flux vanishes as required in a cylinder, geometry., Such a field configuration has a negligible effect, however, on the confined, states
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Far away from the quantum wire (in the y direction), our system contains a narrow region with opposite field direction such that the overall flux vanishes as required in a cylinder geometry. Such a field configuration has a negligible effect, however, on the confined states.
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In contrast to the effective Rashba coupling and g factors for the wire, the effective pairing amplitudes do not oscillate with, U., The distinction arises because the y integration of the projected pairing terms is dominated by |y| ≈ W/2; hence, they are weakly sensitive to the oscillatory confined wave-function, tails
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In contrast to the effective Rashba coupling and g factors for the wire, the effective pairing amplitudes do not oscillate with U. The distinction arises because the y integration of the projected pairing terms is dominated by |y| ≈ W/2; hence, they are weakly sensitive to the oscillatory confined wave-function tails.
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H have similar magnitudes but opposite signs, a very small proximity-induced gap may arise because of cancellations. Such a situation is nongeneric, however, and is not expected to be relevant in practice
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H have similar magnitudes but opposite signs, a very small proximity-induced gap may arise because of cancellations. Such a situation is nongeneric, however, and is not expected to be relevant in practice.
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eff is chosen here simply so that, with InSb parameters, the topological phase does not appear too close to the critical point at a field of B = 0:2 T
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It is tempting to use measured values for mean-free paths for HgTe quantum wells and InSb wires to attempt a further comparison. We avoid this since the relevant quantities in the presence of a superconductor are not known.
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