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(a): Escape time as a function of α for different values of λ. (b): Escape time as a function of λ for different values of α.
Escape time, ℰ, against connection strength, β, for the 13 different three-node networks depicted in Figure 7, with λ = 0.9 and α = 0.05.
The escape time for these networks is constant in the network size N.
The fully connected network (network 13) has the highest escape time for all values of β.
This value is two orders of magnitude shorter than the thermal escape time for electrons (approximately 60 ps).
However, since not all nodes in the network begin oscillating at exactly the same time, we need to define the escape time for a trajectory of a network.
The exception is network 1 (group (a) which has the lowest escape time for β <~ 2.0, but a higher value for β >~ 2.0.
The particular value of the escape time for these networks appears well described by Equation 5. Figure 12 Illustration of directed paths and the FTC.
The thermal escape time for both electrons and holes are also calculated as a function of temperature, using Equation 5 and plotted in Figure 4.
High-field domain [22] is formed, and an increase in the applied bias leads to the reduction of the electron escape time for a single well at a time.
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