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Steering acoustic surface waves by nonlinear mixing
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6.Specifically for input beam angles and to the [11̄0] axis, the difference‐frequency wave vector can be steered from to by changing the input‐frequency ratio from to Due to crystal anisotropy, the actual propagation direction for the difference‐frequency beam would be steered from approximately to (The [21̄1̄] direction used in a reference in Fig. 1 is at 30° to the [11̄0] axis used here).
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