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. 2021 Jun 1;2021:9850151. doi: 10.34133/2021/9850151

Figure 4.

Figure 4

3D surfaces (a) and 2D polar plots (b) of the acoustic velocity for MIL-53(Ga)lp projected normal to the (010) plane. (c) Acoustic switching enabled by the high anisotropy in acoustic waves of MIL-53(Ga)lp: when the same sound waves pass through the material, the output sound wave velocities will attenuate by very different magnitudes.