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In a Hall transport experiment there is no significant difference between the true Corbino geometry and the quasi-Corbino case of a finite strip with W□L. The current jy exists everywhere, except the extremities of the sample at y=±W/2, where the current lines exit and enter the left and the right contacts, respectively. In our case, the current lines must form closed loops, which most probably will pass through the source contact, or the adjacent to this contact ungated part of the channel.
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In a Hall transport experiment there is no significant difference between the true Corbino geometry and the quasi-Corbino case of a finite strip with W□L. The current jy exists everywhere, except the extremities of the sample at y=±W/2, where the current lines exit and enter the left and the right contacts, respectively. In our case, the current lines must form closed loops, which most probably will pass through the source contact, or the adjacent to this contact ungated part of the channel.
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14
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70350663571
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Similar results can be obtained within the Drude theory [neglecting the convective term (□□) v]. The oscillating part remains the same, while Eq. 21 acquires an additional factor of 1/2 in the second term, which does not modify the qualitative behavior of f (β).
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Similar results can be obtained within the Drude theory [neglecting the convective term (□□) v]. The oscillating part remains the same, while Eq. 21 acquires an additional factor of 1/2 in the second term, which does not modify the qualitative behavior of f (β).
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