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. 2021 Jun 1;12:3267. doi: 10.1038/s41467-021-23359-7

Fig. 4. Strongly coupled acoustic cavities constructed as a vertically-stacked heterostructure.

Fig. 4

a Spectrum for the MoS2/h-BN/MoS2 tri-layer; b Spectrum of the neighboring MoS2/MoS2 control area. The red tick in b highlights the location of the non-active second harmonic peak. Only odd modes are excited with the homogeneous pump excitation here. c FEM-predicted frequencies for the three lowest vibrational modes of the tri-layer system as function of the spacer h-BN layer thickness. Experimental data (open symbols) are included for the tri-layer (h-BN thickness = 5 L, normalized εZZ strain configurations are shown on the right) and for the control sample (h-BN thickness = 0 L). d, e The normalized εZZ strain profiles for vibrational modes in monolithic MoS2 (dotted lines) are shown in comparison with strain in the tri-layer system (solid lines) at the labeled frequencies.