antropy.higuchi_fd¶
- antropy.higuchi_fd(x, kmax=10)[source]¶
Higuchi Fractal Dimension.
- Parameters:
- xlist or np.array
One dimensional time series.
- kmaxint
Maximum delay/offset (in number of samples).
- Returns:
- hfdfloat
Higuchi fractal dimension.
Notes
Original code from the mne-features package by Jean-Baptiste Schiratti and Alexandre Gramfort.
This function uses Numba to speed up the computation.
References
Higuchi, Tomoyuki. “Approach to an irregular time series on the basis of the fractal theory.” Physica D: Nonlinear Phenomena 31.2 (1988): 277-283.
Examples
>>> import numpy as np >>> import antropy as ant >>> import stochastic.processes.noise as sn >>> rng = np.random.default_rng(seed=42) >>> x = sn.FractionalGaussianNoise(hurst=0.5, rng=rng).sample(10000) >>> print(f"{ant.higuchi_fd(x):.4f}") 1.9983
Fractional Gaussian noise with H = 0.9
>>> rng = np.random.default_rng(seed=42) >>> x = sn.FractionalGaussianNoise(hurst=0.9, rng=rng).sample(10000) >>> print(f"{ant.higuchi_fd(x):.4f}") 1.8517
Fractional Gaussian noise with H = 0.1
>>> rng = np.random.default_rng(seed=42) >>> x = sn.FractionalGaussianNoise(hurst=0.1, rng=rng).sample(10000) >>> print(f"{ant.higuchi_fd(x):.4f}") 2.0581
Random
>>> rng = np.random.default_rng(seed=42) >>> print(f"{ant.higuchi_fd(rng.random(1000)):.4f}") 2.0013
Pure sine wave
>>> x = np.sin(2 * np.pi * 1 * np.arange(3000) / 100) >>> print(f"{ant.higuchi_fd(x):.4f}") 1.0091
Linearly-increasing time-series
>>> x = np.arange(1000) >>> print(f"{ant.higuchi_fd(x):.4f}") 1.0040