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. 2019 Jan 25;19(2):1282–1288. doi: 10.1021/acs.nanolett.8b04862

Figure 2.

Figure 2

Stochastic switching of the nonlinear resonator with a diameter of 5 μm. (a) Amplitude as a function of time for an effective temperature Teff = 25 × 103 K, showing a total of 8 fluctuation-induced transitions. The right-hand side of the figure shows a histogram of the amplitude. (b) Amplitude in the P-Q space for Teff = 25 × 103 K, each point is one sample of the measurement in part a. (c) Rate of up and down transitions as a function of effective temperature, fitted with Kramer’s law (eq 4), two sets of consecutive measurements are shown to check for consistency. (d) Amplitude as a function of time for an effective temperature Teff = 65 × 103 K, showing a total of 502 transitions. The right-hand side of the figure shows a histogram of the amplitude. (e) Amplitude in the P-Q space for Teff = 65 × 103 K. f) Residence time distributions for both states at Teff = 65 × 103, a Poisson distribution (eq 5) is fitted to the data and gives a transition time τk = 1.7 ms, corresponding to a transition rate rk = 0.58 kHz.