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Figure 4.5 Transmission coe cient of (a) mode 0 and (b) mode 1 vs W C
for asymmetric y-branch three-terminal junction. The incident frequency
is 1.1 π v T / W I . Solid and dotted curves correspond to the transmission in
regions A and B, respectively [89].
phonons is independent of the temperature. However, the three-
terminal systems may offer a proper option for ballistic thermal
rectificationbyintroducingincoherencetothephonontransmission
from the third terminal, which is confirmed by Zhang et al. [91].
They found that ballistic thermal rectification exists in asymmetric
three-terminal atomic nanojunctions, even in symmetric three-
terminalstructureswithspin-phononinteraction.Morerecently,the
 
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