The process causes the time passage variations induced by the torsional vibration to average to zero, ultimately yielding the time stamps caused by the passage of each respective encoder segment.
Hence, this quantum simulation model will be robust to parameters deviations as long as these two sums are maintained at zero; i.e., local fluctuations of the microscopic parameters that (spatially) average to zero are inconsequential.
We therefore take our estimate of the current SV to be our prediction of the SV for 2015.0 to 2020.0, essentially assuming no average SA or equivalently that the SA will average to zero over the upcoming 5 years.
For a given set of target rates, the inverse image of (R(r_{a}, r_{b})) under Z, written (Z^{-1}(R(r_{a}, r_{b}))), is the set of all r distributions for which ȧ and ḃ average to zero.
Let R denote the map from a pair of firing rate targets ((r_{a},r_{b})) to ((f_{a}(r_{a}), f_{b}(r_{b}))), which are the average values of (f_{a}) and (f_{b}) necessary for ȧ and ḃ to average to zero.
When 4 τ 2 ω 0 2 − 1 > 0, we observe the presence of damped oscillations of the velocity in time with strong coupling leading to oscillating currents which average to zero in a sufficiently long interval along with the diffusion constant.
