“…171,219,227,228,229,230,231 The amount of splitting (denoted as 2𝑔) increases with Λ , and can be controlled by modulating the strength of the pump signal (Figure 10.4d,e), 227,229,231 tuning the tension using a DC gate bias, 227,231 heating the resonator using a laser beam, 171,228 or even bending the substrate. 245 Transfer of energy between the modes can also occur 241 when ωp = | ω1 -ω2 | / n, for integer values of 𝑛 ≥ 2. 171,227,228,229,230,231 An example of this phenomenon in 2D NEMS resonators is shown in Figure 10.4f.…”