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We chose this boundary condition because of the convenience for the parallelized code. This choice is not essential for our results. At least, similar diode effects were observed for periodic boundary conditions in the z direction, in which the two heat baths (T1 and T2) are located with the separation length Lz /2.
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We chose this boundary condition because of the convenience for the parallelized code. This choice is not essential for our results. At least, similar diode effects were observed for periodic boundary conditions in the z direction, in which the two heat baths (T1 and T2) are located with the separation length Lz /2.
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