Skip to main content
. 2020 Mar 24;9:e52224. doi: 10.7554/eLife.52224

Figure 1. Tests of exponent estimation for the DLFNN using N = 104 simulated fBm trajectories.

Figure 1.

(a) Plots showing the Hurst exponent estimates of fBm trajectories with n=102 data points by a triangular DLFNN with three hidden layers compared with conventional methods. Plots are vertically grouped by Hurst exponent estimation method: (left to right) rescaled range, MSD, sequential range and DLFNN. σH values are shown in the title. Top row: Scatter plots of estimated Hurst exponents Hest and the true value of Hurst exponents from simulation Hsim. The red line shows perfect estimation. Second row: Due to the density of points, a Gaussian kernel density estimation was made of the plots in the top row (see Materials and methods). Third row: Scatter plots of the difference between the true value of Hurst exponents from simulation and estimated Hurst exponent ΔH=Hsim-Hest. Last row: Gaussian kernel density estimation of the plots in the third row. (b) σH as a function of the number of consecutive fBm trajectory data points n for different methods of exponent estimation. Example structures for two hidden layers and n=5 time series input points of the anti-triangular, rectangular and triangular DLFNN are shown in (c, d and e), respectively. (f) σH as a function of the number of hidden layers in the DLFNN for triangular, rectangular and anti-triangular structures. (g) σH as a function of the number of randomly sampled fBm trajectory data points nrand with different number of hidden layers in the DLFNN shown in the legend. (h) σH as a function of the noise-to-signal ratio (NoiseSignal) (NSR) from Gaussian random numbers added to all n=102 data points in simulated fBm trajectories. (i) Plots of bias b(Hsim), variance Var(Hsim) and mean square error (MSE) as functions of Hsim. For each value of Hsim, fBm trajectories with n=100 points were simulated and estimated by a triangular DLFNN.